Digitized by tine Internet Arciiive in 2010 witii funding from Open Knowledge Commons http://www.archive.org/details/textbookofphysio1883fost A TEXT BOOK OF PHYsioLoay A TEXT BOOK C)F PHYSIOLOGY BY M. FOSTEK, M.A., M.D., F.RS. PRELECTOR IN PHYSIOLOGY AND FELLOW OF TRINITY COLLEGE, CAMBRIDGE. WITH IL L USTRA TIONS. FOURTH EDITION, REVISED. ?[onlron: MACMILLAN AND CO. 1883 \The Right of Translation is reserved.] PBINTED BY C. J. CLAY, M.A. & SON, AT THE UNIVERSITY PEESS, PREFACE TO THE FOURTH EDITION. In previous Editions of this work I endeavoured, by the use of smaU and large print, to distinguish between the more important and stable portions of Physiology, which ought to be made known to every one engaged in a serious study of the science, and the less settled, often controverted views which should be attacked by the more advanced students only. Experience however has taught me that the advantages of such a plan are more than counterbalanced by its disadvantages. I especially felt that the amount of space which I could fairly allow to the small print paragraphs was wholly insufficient to permit me to do justice to the conflicting views which I strove, in them, to expound. In this Edition accordingly I have made no attempt at any such distinction, and have used small print almost exclusively for the description of methods and apparatus. This step involving, as it necessarily did, the transference, into the body of the work, of some of the statements which previously had found their place in the small print vi PREFACE. portions, has given the volume, at first sight, the appear- ance of having heen largely altered. This however is not the case. For good or for bad, the book remains very much as it was ; and though I have done my best to remove some of the many defects present in previous editions, I have been encouraged, by the favour with which those editions have been successively received, to persevere in the views which I have always held as to which are the parts of physiology most to be insisted on, and which may be lightly touched or wholly omitted ; and though I would still most strenuously repudiate the idea, put forward by some, that there is such a thing as a physiology for medical men, different from that physiology which is a part of science, I have tried to make this volume especially useful to medical students. My decision to do away with the small print portions of former editions has been largely determined by the fact that my former pupils, now my colleagues at Cam- bridge, have undertaken to join with me in treating these higher or advanced parts of physiology in a more extended and satisfactory form. And the hope that the result of their labours will soon appear has led me, in this volume, to omit all references, and to use as little as possible the personal authority of the names of investi- gators. The fondness of students for the use of names of persons is as marked as the pertinacity with which they use them wrongly ; and if any observer may feel aggrieved at his name being absent from an ordinary text- book, he may at least have the satisfaction of reflecting that the omission of all names does something to prevent others receiving the credit of his labours. I'll E FACE. vii I cannot say liow niiicli 1 ;mi indebted to the con- tinued help of those friends \vho assisted me in former editions ; and I have also to acknowledt^e with gratitude the aid afforded me by Prof. C. IS. Hoy, to whose kindness I owe several of the new illustrations. The appendix on chemical matters, as in former editions, has been under the care of Mr Sheridan Lea; in this, which stands on a somewhat different footing from the rest of the work, references and names of authors have been retained. Trinity College, Cambridge, Fehruart/, 1883. CONTENTS. PAOE INTRODUCTORY 1 BOOK I. BLOOD. THE TISSUES OF MOVEMENT. THE VASCULAR MECHANISM. CHAPTER I. Blood, pp. 11 — 34. Seel. The Coagulation of Blood 13 Sec. 2. The Chemical Composition of Blood .2-1 Sec. 3. The History of the Corpuscles 2S Sec. 4. The Quantity of Blood, and its distribution in the body ... 33 CHAPTER II. The Contractile Tissues, pp. 35 — 103. Sec. 1. The Phenomena of Muscle and Nerve 37 Muscular and Nervous Lritability, p. 87. The Phenomena of a simple muscular contraction, p. 39. Tetanic contractions, p. 48. Sec. 2. The Changes in a Muscle during Muscular Contraction ... 54 The change in form, p. 54. Electrical changes, p. 58. Chemical changes, p. 64. Thermal changes, p. 70. The changes in a Nerve during the passage of a Nervous Impulse, p. 72. Sec. 3. The Nature of the Changes through which an Electric Current is able to generate a Xercous Impulse ....... 75 The action of the Constant Current, p. 75. Electrotonus, p. 77. Electrotonic Currents, p. 80. X CONTENTS. PAGE Sec. 4. The Muscle-Nerve Preparation as a Machine 83 The nature aud mode of application of the Stimulus as affecting the amount and character of the Contraction, p. 83. The influence of the Load, p. 87. The influence of the Size and Form of the Muscle, p. 88. The work done, p. 89. Sec. 5. The Circumstances which determine the Degree of Irritability of Muscles and Nerves ......... 90 The effects of severance from the Central Nervous System, p. 91. The Influence of Temperature, p. 93. The Influence of Blood Supply, p. 94. The Influence of Functional Activity, p. 95. Sec. 6. The energy of Muscle and Neire, and the nature of Muscular and Nervous Action .......... 98 Sec. 7. Other forms of Contractile Tissue ....... 101 Unstriated Muscular Tissue, p. 101. Cardiac Muscles, p. 102. Cilia, p. 102. Migrating Cells, p. 103. CHAPTER III. The Fundamental Properties of Nervous Tissues, pp. 104 — 114, Automatic actions, p. 107. Reflex actions, p. 109. Actions of sporadic ganglia, p. 112. Inhibition, p. 113. CHAPTER IV. The Vascular Mechanism, pp. 115 — 230. I. The Physical Phenomena of the Cieculation .... 116 Seel. Main general facts of the Circulation ...... 117 The Capillary Circulation, p. 117. The flow in the Arteries, p. 120. The flow iu the Veius, p. 127. Hydraulic principles of the Circu- lation, p. 128. Sec. 2. The Heart 135 The Phenomena of the Normal Beat, p. 135. The Mechanism of the Valves, p. 142. The Sounds of the Heart, p. 143. On the relative duration and special characters of the cardiac events, p. 146. The work done, p. 157. Variations in the Heart's Beat, p. 159. Sec. 3. The Pulse . ". 161 n. The Vital Phenomena of the Cieculation .... 176 Sec. 4. Changes in the Beat of the Heart 178 The Mechanism of the normal beat, p. 180. Inhibition of the beat, p. 184. The effects on the circulation of changes in the heart's beat, p. 194. CONTJjJNTS. xi PAGK Sec. 5. Changes in the calibre of the minute arteries. Vaso-viotor actions . 1^7 Vaso-molor Nerves, p. 1J9. Vaso-motor Centres, p. 212. The effects of local vascular constriction or dilution, p. 21G. Sec. G. Changes in the Capillary Districts 21'J Sec. 7. Changes in the Quantity of Blood 224 Sec. 8. The Mutual Jielations and the Co-ordination of the Vascular Factors 111 BOOK 11. THE TISSUES OF CHEMICAL ACTION WITH THEIR RESPECTIVE MECHANISMS. NUTRITION, CHAPTER I. The Tissoes and Mechanisms of Digestion, pp. 233 — 311. Seel. The Properties of the Digestive Juices 234 Saliva, p. 234. Gastric juice, p. 239. Bile, p. 247. Pancreatic juice, p. 250. Succus entericus, p. 255. Sec. 2. The act of secretion in the case of the Digestive Juices and the Nervous Mechanisms which regulate it 256 Sec. 3. The Muscular Mechanisms of Digestion 281 Mastication, p. 281. Deglutition, p. 282. Movements of the CEsopbagns, p. 284. Movements of the stomach, p. 285. Move- ments of the small intestine, p. 286. Movements of the large intestine, p. 288. Defsecation, p. 288. Vomiting, p. 290. Sec. 4. The Changes which the Food undergoes in the Alimentary Canal . 292 Sec. 5. Absorption of the Products of Digestion 301 The Lymphatics, p. 301. Entrance of the chyle into the lacteals, p. 303. Movements of the chyle, p. 304. Lymph-hearts, p. 306. The course taken by the several products of digestion, p. 306. CHAPTER II. The Tissues and Mechanisms of Respiration, pp. 312 — 383. Seel. The Mechanics of Pulmonary Respiration ...... 314 The Ebythm of Respiration, p. 316. The Eespiratory Move- ments, p. 319. Facial and LaryTigeal Eespiration, p. 324. Sec. 2. Changes of the Air in Eespiration 326 Sec. 3. The Respiratory Changes in the Blood . . . . . . 329 The relations of oxygen in the blood, p. 332. Hemoglobin ; its properties and derivatives, p. 333. Colour of venous and arterial blood, p. 338. The relations of the carbonic acid in the blood, p. 342. The relations of the nitrogen in the blood, p. 343. Sec. 4. Tlte Respiratory Changes in the Lungs 344 The entrance of oxygen, p. 344. The exit of carbonic acid, p. 346, xii CONTENTS. PAOE Sec. 5. The Respiratonj Changes in the Tissues 348 Sec. 6. The Nervous Mechanism of Respiration ...... 358 Sec. 7. The Effects of Respiration on the Circulation 364 Sec. 8. The Effects of Changes in the Air breathed ..... 375 The effects of deficient air. Asphyxia. Phenomena of asphyxia, p. 375. The circulation in asphyxia, p. 378. The effects of an increased supply of air. Apnoea, p. 380. The effects of changes in the composition of the air breathed, p. 380. The effects of changes in the pressure of the air breathed, p. 381. Sec. 9. Modified Respiratonj Movements 382 Sighing, Yawning, Hiccough, Sobbing, Coughing, Sneezing, Laughter and Crying, p. 382, CHAPTER III. Secretion by the Skin, pp. 384 — 391. The nature and amount of Perspiration, p. 385. Cutaneous Eespiration, p. 386. The Secretion of Perspiration, p. 387. The Nervous Mechanism of Perspiration, p. 388. Absorption by the Skin, p. 390. CHAPTER IV. Secretion by the Kidneys, pp. 392 — 414, Sec. 1. The Composition of Urine 893 Sec. 2. The Secretion of Urine 397 The relation of the secretion of urine to arterial pressure, p. 398. Secretion by the renal epithelium, p. 404. Sec. 3. Micturition • . . 410 CHAPTER V. The Metabolic Phenomena of the Body, pp. 415 — 478. Sec. 1, Metabolic Tissues 416 The History of Glycogen, p. 416. Diabetes, p. 424, The History of Fat, Adipose Tissue, p. 426. The Mammary Gland, p. 429, The Spleen, p. 432. Sec. 2. The History of Urea and its allies 436 Sec, 3, The Statistics of Nutrition 443 Compariso-n of Income and Output, p. 446, Nitrogenous Meta- bolism, p. 449. The effects of Fatty and of Carbohydrate Food, p. 453. Sec. 4, The Energy of the Body 457 The income of energy, p. 457. The expenditure, p. 458. The sources of Muscular Energy, p, 459, The sources and distribution of Heat, p. 461. Eegulation by variations in loss, p. 464. Regu- lation by variations in production, p. 465, Sec. 5, The Influence of the Nervous System on Nutrition .... 470 Sec. 6. Dietetics . . . 474 COS TEXTS. xiii BOOK III. THE CENTRAL NERVOUS SYSTEM AND Tl'S INSTRUMENTS. CHAPTER I. Sensory Nkkves, pp. 181 — 4iS9. CHAPTER II. SiGUT, pp. 490—555. PAGE Sec. 1. Dioptric Mechanisins 491 The Formation of the Image, p. 491. Accommodation, p. 493. Movements of the Pupil, p. 500. Imperfections in the Dioptric apparatus, p. 506. Sec. 2. Visual Sensations . . . , 511 The origin of Visual Impulses, p. 511. Simple Sensations, p. 519. Colour Sensations, p. 524. Sec. 3. Visual Perceptions .......... 535 Modified Perceptions, p. 536. Sec. 4. Binocular Vision 541 Corresponding or identical points, p. 511. Movements of the eye- balls, p. 542. The Horopter, p. 547. Sec. 5. Visual Judgments 549 Sec. 6. The Protective Mechanisms of the Eye 554 CHAPTER III. Hearing, Smell, and Taste, pp. 556 — 571. Sec. 1. Hearing 556 The acoustic apparatus, p. 557. Auditory Sensations, p. 559. Auditory Judgments, p. 565. Sec. 2. Smell 567 Sec. 3. Taste 570 xiv CONTENTS. CHAPTER IV. Feeling and Touch, pp. 572 — 584. PAGE bee. 1. General Sensibility and Tactile Perceptions 572 Sec. 2. Tactile Sensations 575 Sensations of Pressure, p. 575. Sensations of Temperature, p. 576. Sec. 3. Tactile Perceptions and Judgments 579 Sec. 4. The Muscular Sense 982 CHAPTER V. The Spinal Coed, pp. 585 — 607. Sec. 1. As a Centre or Group of Centres of Reflex Action .... 585 Inhibition of Reflex Action, p. 590. The Time required for Eeflex Actions, p. 513. Sec. 2. As a Centre or Group of Centres of Automatic Action . . . 595 Sec. 3. As a Conductor of Afferent or Efferent Impulses .... 598 CHAPTER VI. The Beain, pp. 608—650. Sec. 1. On the Phenomena exhibited by an animal deprived of its Cerebral Hemispheres ........... 608 Sec. 2. The Mechanisms of Co-ordinated Movements 614 Forced Movements, p. 620. Sec. 3. The Functions of the Cerebral Convolutions ; . . . . 623 Sec. 4. The Functions of other parts of the Brain 636 Corpora striata and optic thalami, p. 636. Corpora quadrigemina, p. 638. Cerebellum, p. 640. Crura cerebri and pons Varolii, p. 641. Medulla oblongata, p. 642. Sec. 5. The Rapidity of Cerebral Operations ...... 643 Sec. 6. The Circulation in the Brain 645 Sec. 7. The Cranial Nerves 648 CHAPTER VII. Special Musculae Mechanisms, pp. 651 — 664. Sec. 1. The Voice 651 Sec. 2. Speech . 657 Vowels, p. 657. Consonants, p. 658. Sec. 3. Locomotor Mechanisms ....■•••• 662 CONTENTS. BOOK IV. THE TISSUES AND MECHANISMS OF REPRODUCTION. CHAPTER I. Menstruation, pp. 669 — 671. CHAPTER II. Impregnation, pp. 672 — 673. CHAPTER III. The Nutrition of the Embryo, pp. 674 — 680. CHAPTER IV. Parturition, pp. 681 — 683. CHAPTER V. The Phases of Life, pp. %%i — 694-. CHAPTER VI. Death, pp. 695 — 696. APPENDIX. On the Chemical Basis op the Animal Body, pp. 697 — 770. INDEX, pp. 771—785. INTRODUCTORY. Among the simpler organisms kuowu to Biologists, perhaps the most simple as well as the most common is that which has received the name of Amoeba. There are many varieties of Amoeba, and probably many of the forms which have been described are, in reality, merely amoebiform phases in the lives of certain animals or plants ; but they all possess the same general characters. Closely resembling the white corpuscles of vertebrate blood, they are wholly or almost wholly composed of undifferentiated protophism, in the midst of which lies a nucleus, though this is sometimes absent. In many a distinction may be observed between a more solid external layer or ectosarc, and a more fluid granular interior or endosarc ; but in others even this primary differentiation is wanting. By means of a continually occurring flux of its protoplasmic substance, the amoeba is enabled from moment to moment not on!}' to change its form but also to shift its position. By flowing round the sub- stances which it meets, it, in a way, swallows them ; and having digested and absorbed such parts as are suitable for food, ejects or rather flows away from the useless remnants. It thus lives, moves, eats, grows, and after a time dies, having been during its whole life hardly an) thing more than a minute lump of protoplasm. Hence to the Pliysiologist it is of the greatest interest, since in its life the problems of physiology are reduced to their simplest forms. Now the study of an amoeba, with the help of knowledge gained by the examination of more complex bodies, enables us to state that the undifferentiated protoplasm of which its body is so largely composed exhibits certain fundamental phenomena which we may .speak of as ' vital.' F. 1 2 PHENOMENA OF PROTOPLASM. 1. It is contractile. There can be little doubt that the changes in the protoplasm of an amoeba which bring about its peculiar ' amoeboid ' movements, are identical in their fundamental nature with those which occurring in a muscle cause a contraction : a muscular contraction is essentially a regular, an amoeboid move- ment an irregular flow of protoplasm. The substance of the amoeba may therefore be said to be contractile. 2. It is irritable and automatic. When any disturbance, such as contact with a foreign body, is brought to bear on the amoeba at rest, movements result. These are not passive move- ni^ats, the effects of the push or pull of the disturbing body, proportionate to the force employed to cause them, but active manifestations of the contractility of the protoplasm ; that is to say, the disturbing cause, or ' stimulus,' sets free a certain amount of energy previously latent in the protoplasm, and the energy set free takes on the form of movement. Any living matter which, when acted on by a stimulus, thus suffers an explosion of energy, is said to be ' irritable.' The irritability may, as in the amoeba, lead to movement ; but in some cases no movement follows the application of the stimulus to irritable matter, the energy set free by the explosion taking on some other form than movement, ex. gr. heat. Thus a substance may be irritable and yet not contractile, though contractility is a very common manifestation of irritability. The amoeba (except in its prolonged quiescent stage) is rarely at rest. It is almost continually in motion. The movements cannot always be referred to changes in surrounding circumstances acting as stimuli; in many cases the energy is set free in conse- quence of internal changes, and the movements which result are called spontaneous or automatic movements. We may therefore speak of the protoplasm of the amoeba as being irritable and automatic. 3. It is receptive and assimilative. Certain substances serving as food are received into the body of the amoeba, and there in large measure dissolved. The dissolved portions are subse- quently converted from dead food into new living protoplasm, and become part and parcel of the substance of the amoeba. 4. It is metabolic and secretory. Pari passu with the re- ception of new material, there is going on an ejection of old material, for the increase of the amoeba by the addition of food is not indefinite. In other words, the protoplasm is continually undergoing chemical change (metabolism), room being made for the new protoplasm by the breaking up of the old protoplasm into products which are cast out of the body and got rid of. These products of metabolic action have, in many cases at all events, subsidiary uses. Some of them, for instance, we have reason to think, are of value for the purpose of dissolving and effecting other ISTHoDlCTonr. 3 preliminary clianges iu the raw food iiitrodnccd into the body of the amu3ba; and hence are retained within the body for some little time. Such products are generally spoken of as 'secretions.' Others which pass more rapidly away are generally called 'ex- cretions.' The distinction between the two is an uiiimp(jrtaut and freipiontly accidental one. The energy expended in tlic movements of the amceba is supplied by the chemical changes going on in the protoplasm, by the breaking up of bodies possessing much latent energy into bodies possessing less. Thus the metabolic changes which the food (as distinguished from tlie undigested stuff mechcinically lodged for a while in the body) undergoes in passing through the protoplasm of the amaba are of three classes : those preparatory to and culminating in tiie conversion of the food into protoplasm, those concerned iu the discharge of energy, and those tending to economise the immediate products of the second class of changes by rendering them more or less useful in carrying out the first. 5. It is respiratory. Taken as a whole, the metabolic changes are pre-eminently processes of oxidation. One article of food, i.e. one substance taken into the body, viz. oxygen, stands apart from all the rest, and one product of metabolism peculiarly associated with oxidation, viz. carbonic acid, stands also somewhat apart from all the rest. Hence the assumption of oxygen and the excretion of carbonic acid, together with such of the metabolic proces.ses as are more especially oxidative, are frequently spoken of together as constituting the respiratory processes. G. It is reproductive. The individual amceba represents a unit. This unit, after a longer or shorter life, havincr increased iu size by the addition of new protoplasm in excess of that which it is continually using up, may, by fission (or by other means) lesolve itself into two (or more) parts, each of which is capable of living as a fresh unit or individual. Such are the fundamental vital qualities of the protoplasm of an amoeba ; all the facts of the life of an amoeba are manifesta- tions of these protoplasmic qualities in varied sequence and sub- ordination. The higher animals, we learn from morphological studies, may be regarded as groups of amoebae peculiarly associated together. All the physiological phenomena of the higher animals are simi- larly the results of these fundamental qualities of protoplasm peculiarly associated together. The dominant principle of this association is the physiological division of labour corresponding to the morphological differentiation of structure. Were a larger or 'higher' animal to consist simply of a colony of undifferentiated amoebae, one animal differing from another merely in the number of units making up the mass of its body, without any differences between the individual units, progress of function would be an 1—2 4 THE FUNDAMENTAL TISSUES. impossibility. The accumulation of units would be a hindrance to welfare rather than a help. Hence, in the evolution of living beings through past times, it has come about that in the higher animals (and plants) certain groups of the constituent amoebiform units or cells have, in company with a change in structure^ been set apart for the manifestation of certain only of the fundamental properties of protoplasm, to the exclusion or at least to the complete subordination of the other properties. These groups of cells, thus distinguished from each other at once by the differentiation of structure and by the more or less marked exclusiveness of function, receive the name of 'tissues.' Thus the units of one class are characterized by the exaltation of the contractility of their protoplasm, their automatism, metabolism and reproduction being kept in marked abeyance. These units constitute the so-called muscular tissue. Of another tissue, viz. the nervous, the marked features are irritability and automatism, with an almost complete absence of contractility and a great restriction of the other qualities. In a third group of units, the activity of the protoplasm is largely confined to the chemical changes of secretion, contractility and automatism (as manifested by movement) being either absent or existing to a very slight degree. Such a secreting tissue, consisting of epithelium-cells, forms the basis of the mucous membrane of the alimentary canal. In the kidney, the substances secreted by the cells, being of no further use, are at once ejected from the body. Hence the renal tissue may be spoken of as excretory. In the epithelium-cells of the lungs, the protoplasm plays an altogether subordinate part in the assumption of oxygen and the excretion of carbonic acid. Still we may perhaps be permitted to speak of the pulmonary epithelium as a respiratory tissue. In addition to these distinctly secretory or excretory tissues, there exist groups of cells specially reserved for the carrying on of chemical changes, the products of which are neither cast out of the body, nor collected in cavities for digestive or other uses. The work of these cells seems to be of an intermediate character ; they are engaged either in elaborating the material of food that it may be the more easily assimilated, or in preparing used-up material for final excretion. They receive their materials from the blood and return their products back to the blood. They may be called the metabolic tissues par excellence. Such are the fat-cells of adipose tissue, the hepatic cells (as far as the work of the liver other than the secretion of bile is concerned), and probably many other cellular elements in various regions of the body. Each of the various units retains to a greater or less degree the power of reproducing itself, and the tissues generally are capable of regeneration in kind. But neither units nor tissues can reproduce other parts of the organism than themselves, much less the entire organism. For the reproduction of the complex iXTUonrcToi:)-. -, irKlivklual, certain units are .sot apart in tlio torin of ovarv ann thus inducetl bein<( in all other respects exactly like a natural clottiiij,'. Thus for instance hydrocele iluid, carefully removed without admixture of bK)od from a hydrocele, will in most cases remain fluid without any disposition to clot'. So also the serous fluid removed from the pericardial, pleural, or peritoneal cavities some liours after death in most cases shews no disposition to clot*. But these fluids, hychocelo or pericardial, though they do not clot spontaneously, will generally, upon the addition of serum or a little whipped blood, clot in a most unmis- takeable manner ^ Now libriuogen is certainly present in these fluids, and may be thrown down from them by the addition of sodium chloride or by other means ; and, since serum contains paraglobulin, it was at first thought that the absence of spontaneous coagulation in the untouched hydrocele or pericardial fluid was due to the absence of paraglobulin, which as we have seen is present with fibrinogen iu the spontaneously coagulable plasma of blood, and that the coagulating effect of the addition of the serum was due to the paraglobulin it contained, the jDaraglobulin and fibrinogen acting in some way or other upon each other to produce fibrin. And this view was supported by the fact that paraglobulin precipitated from serum was, like the entire serum, efficacious in giving rise to a coagulation in fibrinogenous pericardial, or hydrocele fluids. It was soon found however that certain specimens of pericardial and even hydrocele fluid did not need the addition of the para- globulin to make them coagulate ; that though they would not coagulate spontaneously they might be made to coagulate by adding to them a constituent of serum which was not paraglobulin but something else. Thus if serum, or indeed whipped blood, be mixed with a large quantity of alcohol and allowed to stand some days, the proteids present are in time so changed by the alcohol as to become insoluble in water. Hence if the copious precipitate, after long standing, be separated by filtration from the alcohol, dried at a low temperature not exceeding 40', and extracted with distilled water, the aqueous extract contains very little proteid matter, indeed very little organic matter at all. Nevertheless even a small quantity of this aqueous extract added alone to certain specimens of hydrocele fluid will bring about a speedy coagulation. The same aqueous extract has also a remarkable eSect in hastening the coagulation of fluids which though they Avill eventually clot, do so very slowly. Thus plasma may, by the careful addition of a ^ In some specimens, however, a spontaneous coagulation, generally slight, but in exceptional cases massive, may be observed. - If it be removed immediately after death it generally clots readily and firmly, giving a colourless clot consisting of librin and white corpuscles only. 3 In a few cases no coagulation can thus be induced. F. 2 18 FIBRIN-FERMEXT. [Book i. certain quantity of neutral salt and water, be reduced to such a condition that it coagulates very slowly indeed, taking perhaps days to complete the process. The addition of a small quantity of the aqueous extract we are describing will however bring about a coagulation which is at once rapid and complete. The active substance, whatever it be, in this aqueous extract exists in small quantity only, and its coagulating virtues are at once and for ever lost when the solution is boiled. Further, there is no reason to think that the active substance actually enters into the formation of the fibrin to which it gives rise ; it seems, without undergoing changes in itself, to act in some way or other on the actual fibrin factors (fibrinogen and paraglobulin or one of them) and to convert them or part of them into fibrin. It appears to belong to a class of bodies playing an important part in physiological processes and called ferments, of which we shall have more to say hereafter. We may therefore speak of it as ih.Q fibrin- ferment, the name given to it by its discoverer Alex. Schmidt. Fibrin-ferment appears to make its appearance in blood soon after it has been shed, and like other ferments is apt to be entangled in and carried down by any precipitates which occur in blood. It is carried down by the plasmine, and hence solutions of plasmine coagulate spontaneously. It exists in serum, and is carried down with paraglobulin when that substance is precipitated. And hence arises the serious question whether the coagiilating effects of serum or prepared paraglobulin on hydrocele or pericardial fluid are not, after all, due to the ferment present rather than to the paraglobulin. So that two views may be taken of the nature of coagulation. One^ teaches that fibrin arises from some mutual action of fibrinogen and para- globulin induced by the fibrin ferment ; the other^ that fibrin is formed through the conversion of fibrinogen alone by the agency of the ferment, paraglobulin either having nothing to do with the matter, or merely assisting by its presence in some indirect way. There can be no doubt that fibrinogen is an essential factor, that coagulation cannot take place without it and that it or some part of it actually becomes fibrin. There is equally no doubt that the presence of the fibrin-ferment is absolutely necessary. It is also more than probable that fibrin does not result from the union of fibrinogen and paraglobulin, since the quantity of fibrin formed is not greater than that of either of these two substances used to produce it. But we still need further light as to the exact nature of the change produced by the ferment, the true characters of the ferment itself, and the part played by paraglobulin. In favour of the view that paraglobulin is not concerned in the matter, it is asserted, that fibrinogen cautiously precipitated from plasma by small quantities of sodium chloride so as to obtain 1 That of Alexander Schmidt, and his pupils and others. ^ That of Hammarsten, Fredericq and others. c'liAi-. I.J J:lj)ul>. 10 it apart from piirai^lobuliM, and tlum iret'il fruiii A-riiK-nt hy repeated washing, will yieKl a solution not spuntanemisly coagulable, but clotting freely on the adtlition of ferment only. In f;iv(jur of the view that the presence of paraglobuliu is essential may be quoted the striking fact that certain specimens of hydrocele liuid may be met with which will not coagulate either spontaneously or nj)on the addition of ferment alone, but will coagulate upon the addition of paranlubulin and ferment. Such fluids may be supposed to contain fibrinogen only. And it has been argued that two substances have been confused under the name of tibrinogen : oiu; coagulating at the same temperature as paraglobuliu, and needing the cooperation of paraglobuliu to form fibrin ; and another body, which may be thrown down from solutions of plasmine or from blood at the temperature of 55" — GO" (the fluids thereby losing the power of coagulating), and which is fibrinogen already on its way to become fibrin, in fact a sort of nascent fibrin, capable of becoming actual fibrin in the total absence of paraglobuliu. Lastly the presence of a neutral salt, such as sodium chloride, appears to be essential to the process, coagulation not occurring even where all three factors are present, if no neutral salt accompanies them. Awaiting further investigation we may for the present conclude that fibrin is formed by the conversion, through the agency of a ferment, of a substance fibrinogen, which forms part of the plasmine spoken of above, but the exact nature of that conversion and whether paraglobuliu has any share in the matter, and if so what, must remain as yet undecided. This conception of coagulation as a chemical process between certain factors renders easy of comprehension the influence of various conditions on the coagulation of blood. The quickening influence of heat, the retarding efiect of cold, the favourable action of motion and of contact with surfaces, and hence the results of whipping and the influence exerted by the form and surface of vessels, become intelligible. The greater the number of points, that is the larger and rougher the surface presented by the vessel into which blood is shed, the more quickly coagulation comes on, for contact with surfaces favours chemical union. So also the presence of spongy platinum, or of an inert powder like charcoal, quickens the coagulation of tardily clotting fluids, such as many specimens of pericardial fluid. Having thus arrived at an approximative knowledge of the nature of coagulation, we are in a better position for discussing the question. Why does blood remain fluid in the vessels of the living body and yet clot when shed ? The older views may be at once summarily dismissed. The clotting is not due to loss of tempei-ature, for cold retards coagu- lation, and the blood of cold-blooded animals behaves just like that of warm-blooded animals in clotting when shed. It is not due to loss of motion, for motion favours coagidation. It is not due to 20 INFLUENCE OF THE LIVING BLOOD-VESSELS. [Book i. exposure to air, whereby either an increased access of oxygen or an escape of volatile matters is facilitated, for on the one hand the blood is fully exposed to the air in the lungs, and on the other shed blood clots when received, without any exposure to the atmosphere, in a closed tube over mercury. All the facts known to us point to the conclusion, that when blood is contained in healthy living blood-vessels, a certain relation or equilibrium exists between the blood and the containing vessels of such a nature that as long as this eqviilibrium is maintained the blood remains fluid, but that when this equilibrium is disturbed by events in the blood or in the blood-vessels or by the removal of the blood, the blood undergoes changes which result in coagulation. The most salient facts in support of this conclusion are as follows. 1. After death, when all motion of the blood has ceased, the blood renaains for a long time fluid. It is not till some time afterwards, at an epoch when post-mortem changes in the blood and in the blood-vessels have had time to develope themselves, that coagulation begins. Thus some hours after death the blood in the great veins may be found perfectly fluid. Yet such blood has not lost its power of coagulating ; it still clots when removed from the body, and clots too when received over mercury without exposure to air, shewing that the fluidity of the highly venous blood is not due to any excess of carbonic acid or absence of oxygen. Eventually it does clot even within the vessels, but perhaps never so firmly and completely as when shed. It clots first in the larger vessels, but remains fluid in the smaller veins, for a very long time, for many hours in fact, since in these the same bulk of blood is exposed to the influence of, and reciprocally exerts an influence on, a larger surface of the vascular walls than in the larger veins. 2. If the vessels of the heart of a turtle (or any other cold- blooded animal) be ligatured, and the heart be cut out and placed in favourable circumstances so that it may continue to beat for as long a period as possible, the blood will remain fluid within the heart as long as the pulsations go on, i. e. for one or two days (and indeed for some time afterwards), though a portion taken away at any period of the experiment will clot very speedily. 3. If the jugular vein of a large animal, such as an ox oi" horse, be ligatured when full of blood, and the ligatured portion excised, the blood in many cases remains perfectly fluid, along the greater part of the length of the piece, for twenty-four or even forty-eight hours. The piece so ligatured may be suspended in a framework and opened at the top so as to imitate a living test-tube, and yet the blood will often remain long fluid, though a portion removed at any time into another vessel will clot in a few minutes. If two such living test-tubes be prepared, the blood may be poured from one to the other without coagulation taking place. The above facts illustrate the absence of coagulation in intact Chap, i.] JlLOUl). 21 or slightly altered living blooj-vessols ; tliu following shew that coagulation may take plaee even in the living vessels. 4. ]f a needle or piece of wire or thread he introduced into the living blood-vessel of an animal, cither during life or imme- diately after death, the piece will be found encrusted with fibrin. 5. If in a living animal a blood-vessel be ligatured, the ligature being of such a kind as to injure the inner coat, coagu- lation takes place at the ligature and extends for some distaiic(; from it. Thus if the jugular vein of a rabbit be ligatured roughly in two places, clots will in a few hours be found in the ligatured portion, reaching upwards and downwards from the ligatures, the middle portion being the least coagulated. Clots Avill also l)e found on the far side of each ligature. The clots will still appear if the ligature be removed immediately after being applied, provided that in the process the inner coat has been wounded. If the ligatures bo applied in such a way as not to injure the inner coat, coagulation will not take place, though the blood may remain for many hours perfectly at rest between the ligatures. So also when an artery is ligatured a conspicuous clot is formed on the cardiac side of the ligature. The clot is largest and firmest in the immediate neighbourhood of the ligature, gradually thinning away from thence and reaching usually as far as where a branch is given off. Between this branch and the ligature there is stasis ; the walls of the artery suffer from the want of renewal of blood, and thus favour the propagation of the coagulation. On the distal side of the ligature where the artery is much shrunken, the clot which is formed, though naturally small and inconspicuous, is similar*. 6. Any injury of the inner coat of a blood-vessel causes a coagulation at the spot of injury. Any treatment of a blood-vessel tending to injure its normal condition causes local coagulation. 7. Disease involving the inner coat of a blood-vessel causes a coagulation at the part diseased. Thus inflammation of the lining membrane of the valves of the heart in endocarditis is frequently accompanied by the deposit of fibrin. In aneurism the inner coat is diseased, and layers of fibrin are commonly deposited. So also in fatty and calcareous degeneration without any aneurismal dilation there is a tendency to the formation of clots. Similar phenomena are seen in the case of serous fluids which coagulate spontaneously. If, as soon after death as the body is cold and the fat is solidified, the pericardium be carefully removed from a sheep b}'- an incision round the base of the heart, the pericardial fluid may be kept in the pericardial bag as in a living cup for many hours without clotting, and yet a small portion removed with a pipette clots at once, and a thread left hanging into the fluid soon becomes covered with fibrin. The only interpretation which embraces these facts is that so long as a certain normal relation between the linintr surfaces of 22 SOURCES OF THE FIBRIN FACTORS. [Book i. the blood-vessels and the blood is maintained, coagulation does not take place ; but when this relation is disturbed by the more or less gradual death of blood-vessels, or by their more sudden disease or injury, or by the presence of a foreign body, coagulation sets in. Two additional points may here be noticed. 1, Stagnation of blood favours coagulation within the blood-vessels, apparently because the blood-vessels, like other tissues, demand a renewal of the blood on which they depend for the maintenance of their vital powers. 2. The influence of surface is seen even in the coaofulation within the vessels. In cases of coas^ulation from gradual death of the blood-vessels, as in the case of an excised jugular vein, the fibrin, when its deposition is sufficiently slow, is .seen to appear first at the sides, and from thence gradually, frequently in layers, to make its way to the centre. So in aneurism, the deposit of fibrin is frequently laminated. In cases where coagulation results from disease of the lining membrane, the rougher the interior, the more speedy and complete the clotting. So also a rough foreign body, presenting a large number of surfaces and points of attachment, more readily produces a clot when intro- duced into the living blood-vessels than a perfectly smooth one. We may perhaps go a step further, for there are certain weighty reasons for believing that in normal circulating blood all the fibrin- iactors are not present in the plasma, and that a disturbance of the equilibrium between the blood and the blood-vessels gives rise to coagulation by inducing changes in certain corpuscles, either the ordinary white corpuscles or corpuscles of a special kind, whereby one or more of the fibrin-factors are discharged into the plasma. 1. When blood is received direct from the blood-vessels into alcohol, the aqueous extract of the precipitate contains little or no fibrin-ferment. If the blood be allowed to stand a little while before being thrown into alcohol some ferment makes its appearance ; and the longer, up to clotting, that the blood stands before being treated with alcohol, the more efficacious is the aqueous extract of the precipitate. Fibrin-ferment therefore seems to make its appearance in blood after being shed. 2. When blood, kept from clotting by exposure to cold or through being retained by ligatures in a living blood-vessel, is allowed to stand till the corpuscles have sunk, the upper layers of the plasma, free from both red and white corpuscles, exhibit when removed very little power of coagulation and, upon examination, are found to contain a very small quantity only of fibrin-ferment. 3. We have reasons for thinking that when blood is shed, a certain number of corpuscles, which we may speak of as white corpuscles, leaving it for the present uncertain whether they are to be regarded as a special kind of corpuscles or not, are broken up and disappear. Putting these facts together we are led to think that normal blood plasma circulating in the normal blood-vessels contains CiiAi'. i] JllJJOl). 23 no fihriu-fiTinont, but that wlion tlio equilibrium of blood is (listurbL'iJ, either by the shedding of the 1)1()()(1 or by injury to the blood-vessels or by the introduction of foreign Ixjdies, fibrin-ferniction wave. In an ordinary contraction occurring in the living body the stimulus is never applied to one end of the fibre ; the nervous impulse which in such cases acts as the stimulus to the muscle, falls into the fibre at about its middle, where the nerv^e ends in an end-plate, and the contraction wave starting from the end-plate travels along the muscular fibre in both directions. In such a case therefore, still more even than in the urarised muscle stimulated artificially at one end, must the whole fibre be occupied at the same time by the wave of contraction. Changes in microscopic stmctnre. When portions of living irritable muscle are examined under the microscope, contraction waves similar to those just described, but feebler and of shorter Fig. 10. MCSCULAB fibre rNTDEEGOIXO COXTRACTION. The muscle is that of Telephoms melanurus treated -with osmic acid. The fibre at c is at rest, at a the contraction begins, at b it has reached its maximum. The right-liand side of the figure shews the same fibre as seen in polarized light. (After Engeknann.) 56 THE CHANGE OF FORM. [Book i. length, may be observed passing along tbe fibres. By appropriate treatment with osmie acid or other reagents, these short contraction waves may be fixed, and the structure of the contracted portion compared at leisure with that of the portions of the fibre at rest. In Fig. 10, representing a fibre of the muscle of an insect (in which these changes can be more satisfactorily studied than in vertebrate muscle), the contraction wave begins near a, and has reached about its maximum at h, while at c the fibre is at rest, the contraction wave not having reached it (or having passed over it, for the beginning and end of the wave are exactly alike). It wiU be seen that at h, each disc of the fibre is shorter and broader than at c. Further, while at c the dim band x is conspicuous, and the light band y, with its accessory markings y , is together lighter than the dim band x, at h in the fully contracted part of the fibre the dim band appears light as compared with the black line y occupying the middle of the previously light band. In the contracted muscle then there is a reversal of the state of things in the resting muscle, the light band (or part of the light band) of the latter in contracting becomes dark, and the dim band of the latter becomes by comparison light. Between rest and full contraction there is an intermediate stage, as at d, in which the distinction between dim and bright bands seems to be largely lost. The subject however is one offering peculiar difficulties in the way of investigation, and while most, though not all, observers agree in the broad facts which have just been stated, there is great diversity of opinion concerning further details and especially as to the interpretation of the various appearances observed. The accessory markings in the middle of the light band have, in particular, been the subject of controversies into which we cannot enter here. When the fibre is examined in polarised light it is seen that the dim band is anisotropic, and the light band isotropic. This is the case during all the phases of the contraction. At no period is there any confusion between the anisotropic and isotropic material ; these maintain their relative positions, both become shorter and broader; but it will be observed that the isotropic substance diminishes in height to a much greater extent than does the anisotropic substance. The latter in fact appears to increase in bulk at the expense of the former. Kelaxatiou. The shortening as we have seen is followed by a relaxation, the muscle returning to its original length. When an appropriate weight is attached to the muscle this return is generally complete, the curve speedily rejoining, as shewn in Fig. 3, the base line from which it started; but when no load is used and the muscle therefore is acted upon by its own weight and that of a very light lever only, the return is incomplete ; the curve, though descending near to, fails to touch the base line and runs nearly parallel to it for some considerable distance. The relaxation is therefore obviously assisted by the extendiag force of the load ; CnAP. II.] THE CONTRACTILE TISSUES. 57 but, nevertheless, is iii the main the result of intrinsic processes going on in the muscle, the reverse of those leading to the shorten- ing. The return of the muscle to its elongated condition, is not a mere passive stretching, after the causes leading to the shortening have passed away ; it like the shortening itself is a manifestation of activity. And hence we find that the complete- ness of the relaxation is dependent on the complex changes which we speak of as the nutrition of the muscle. Thus in their natural position in the living body, muscles, owing to their vigorous nu- trition, assisted by tlie fact that their anatomical disposition keeps them always on the stretch, return completely to their original length, after even powerful and prolonged contractions. In a muscle out of the body, on the other hand, even when loaded, re- peated successive contractions frequently result in the failure to achieve complete relaxation becoming very conspicuous ; and the tetanus cur\'es. Figs. 6 and 7, shew very strikingly this shortcoming, which is often spoken of as the 'contraction remainder.' We may speak of the relaxation as the result of an elastic reaction, but only in the sense that the elastic qualities of the muscle, at any moment, are the expression of deep-seated and con- tinually varying molecular changes going on in the muscular sub- stance. And in this connection attention may be called to a peculiar physical character of contracting muscle. Living muscle at rest is very extensible, but when stretched returns after the extending cause has been removed, rapidly and completely to its former length. In physical language muscle is spoken of as possessing slight but perfect elasticity. It might be imagined that during a contraction this extensibility would be diminished in order that none of the resistance which the muscle had to overcome, no part of the weight for instance which had to be Kfted, should be employed in stretching the muscle itself and thus lead to an apparent waste of energy. On the contrary we find that during a contraction there is an increase of extensibility ; thus if a muscle at rest be loaded \\-ith a given weight, say 50 gi-ammes, and its extension observed, and be then while unloaded thrown into tetanus, and the load applied during the tetanus, the extension in the second case will be distinctly greater than in the first. During the contraction there is so to speak a greater mobility of the muscular molecules, and though this greater mobility may have its advantages, the loaded muscle has in contracting to overcome its own increased tendency to lengthen on extension before it can produce any effect on the weight which it has to lift. The elasticity and extensibility of the muscular substance is how- ever a complicated and difficult subject, and it will be sufficient to reassert that it is essentially a vital property, being dependent, like the irritability of the muscular substance, on certain nutritive factors. As the muscular substance becomes weary with too much work or impoverished by scanty nutrition, its elasticity suffers pan passu 58 MUSCLE CURRENTS. [Book i. with its irritability. The exhausted muscle when extended does not return so readily to its proper length as the fresh active muscle, and, as we shall see, the dead muscle does not return at all. Electrical Changes. Muscle-currents. If a muscle be removed in an ordinary manner from the body, and two non-polarisable electrodes \ con- ^Mjjuu^^ Fig. 11. NoN-PoLAEisABLE Electbodes. a, the glass tube; z, the amalgamated zinc slips connected with their respective wires; z. s., the zinc sulphate solution; cli. c, the plug of china clay; c', the portion of the china-clay plug projecting from the end of the tube ; this can be moulded into any required form. nected with a delicate galvanometer of many convolutions, be placed on two points of the surface of the muscle, a deflection of the galvanometer will take place indicating the existence of a current passing through the galvanometer from the one point of the muscle to the other, the direction and amount of the deflection varying according to the position of the points. The 'muscle- currents' thus revealed are seen to the best advantage when the muscle chosen is a cylindrical or prismatic one with parallel fibres, and when the two tendinous ends are cut off by clean incisions at right angles to the long axis of the muscle. The muscle then presents a (artificial) transverse section at each end and a longi- tudinal surface. We may speak of the latter as being divided into two equal parts by an imaginary transverse line on its surface 1 These (Fig. 11) consist essentially of a slip of thoroughly amalgamated zinc dipping into a saturated solution of zinc sulphate, which in turn is brought into connection with the nerve or muscle by means of a plug or bridge of china-clay moistened with normal sodium chloride solution ; it is important that the zinc should be thoroughly amalgamated. This form of electrodes gives rise to less polarisation than do simple platinum or copper electrodes. The clay affords a connection be- tween the zinc and the tissue which neither acts on the tissue nor is acted on by the tissue. Contact of any tissue with copj^er or platinum is in itself sufficient to de- velope a current. Oh A I'. II ] THE CONTRACTILE TT.'^^UES. 59 called the 'equator ' containincy all the points of the surface midway between the two e ids. Fi<:j. 12 is a diap^ainmatic representation of such a muscle, the line ah being the equator. In such a mu.scle the development of the muscle-currents is found to be as follows. The greatest deflection is observed when one electrode is placed Fig. 12. Diagram illustrating the electric currents of nerve and muscle. Being purely diagrammatic, it may serve for a piece either of nerve or of muscle, except that the currents at the transverse section cannot be shewn in a nerve. The arrows shew the direction of the current through the galvanometer. ah the equator. The strongest currents are those shewn by the dark lines, as from a, at equator, to x ov to ij at the cut ends. The current from a to c is weaker than from a to y, though both, as shewn by the arrows, have the same direction. A current is shewn from e, which is near the equator, to /, which is farther from the equator. The current (in muscle) from a point in the circumference to a point nearer the centre of the transverse section is shewn at gh. From « to b or from X to y there is no current, as indicated by the dotted Unes. at the mid-point or equator of the muscle, and the other at either cut end ; and the deflection is of such a kind as to shew that posi- tive currents are continually passing from the equator through the galvanometer to the cut end, that is to say, the cut end is negative relatively to the equator. The currents outside the muscle may be considered as completed by currents in the muscle from the cut end to the equator. In the diagram Fig. 12, the aiTows indicate the direction of the currents. If the one electrode be placed at the equator ah, the effect is the same at whichever of the two cut ends cc or y the other is placed. If, one electrode remaining at the equator, the other be shifted from the cut end to a spot c nearer to the equator, the current continues to have the same direction, but is of less intensity in proportion to the nearness of the electrodes to each other. If the two electrodes be placed at unequal distances e and/, one on either side of the equator, tliere will be a feeble current from the one nearer the equator to the one farther off, and the current will be the feebler, the more nearly they are equidistant from the equator. 60 MUSCLE CURRENTS. [Book i. If they are quite equidistant, as for instance when one is placed on one cut end x, and the other on the other cut end y, there will be no current at all. If one electrode be placed at the circumference of the transverse section and the other at the centre of the transverse section, there will be a current through the galvanometer from the former to the latter; there will be a current of similar direction but of less intensity when one electrode is at the circumference g of the transverse section and the other at some point li nearer the centre of the transverse section. In fact, the points which are relatively most positive and most negative to each other are points on the equator and the two centres of the transverse sections ; and the intensity of the current between any two points will depend on the respective distances of those points from the equator and from the centre of the transverse section. Similar currents may be observed when the longitudinal surface is not the natural but an artificial one ; indeed they may be witnessed in even a piece of muscle provided it be of cylindrical shape and composed of parallel fibres. These 'muscle-currents' are not mere transitory currents dis- appearing as soon as the circuit is closed ; on the contrary they last a very considerable time. They must therefore be maintained by some changes going on in the muscle, by continued chemical action in fact. They disappear as the irritability of the muscle vanishes, and are connected with those nutritive, so-called vital changes which maintain the irritabihty of the muscle. Muscle-currents such as have just been described, may, we repeat, be observed in any cylindrical muscle suitably prepared, and similar currents, with variations which need not be discussed here, may be seen in muscles of irregular shape with obliquely or otherwise ar- ranged fibres. And du Bois-Keymond, to whom chiefly we are indebted for our knowledge of these currents, has been led to re- gard them as essential and important properties of living muscle. He has moreover advanced the theory that muscle may be con- sidered as composed of electro-motive particles or molecules, each of which like the muscle at large has a positive equator and negative ends, the whole muscle being made up of these molecules in somewhat the same way, (to use an illustration which must not however be strained or considered as an exact one) as a magnet may be supposed to be made up of magnetic particles each with its north and south pole. There are reasons however for thinking that these muscle-currents have no such fundamental origin, that they are in fact of surface and indeed of artificial origin. Without entering largely into the controversy on this question, the following important facts may be mentioned. 1. When a muscle is examined while it still retains untouched its natural tendinous terminations, the currents are much less than Cmap. ii] the contractile TISSUES. Gl when artiticial transverse sections have been made ; the natural tendinous end is less negative than the cut surface. But the tendinous end becomes at once negative when it is di])ped in water or acid, indeed when it is in any way injured. The less roughly in fact a muscle is treated the less evident are the muscle- ciu-rents, and it has been maintained that if adequate care be taken to maintain a muscle in an absolutely natural condition no such currents as those we have been describing exist at all. 2. Englemann has shewn that the surface of the uninjured in- active* ventricle of the frog's heart is isoelectric, i. e. that no current is obtained when the electrodes are placed on any two points of the surface. If however any part of the surface be injured, or if the ventricle be cut across so as to expose a cut surface, the injured spot or the cut surface becomes at once most powerfully negative towards the uninjured surface, a strong current being developed which passes through the galvanometer from the uninjured surface to the cut surface or to the injured spot. The negativity thus developed in a cut surface passes off in the course of some hours, but may be restored by making a fresh cut and exposing a fresh surface. Now, when a muscle is cut or injured the substance of the fibres dies at the cut or injured surface. And many physiologists, among whom the most prominent is Hermann, have been led by the above and other facts to the conclusion that muscle-currents do not exist naturally in untouched muscles, that the muscular substance is naturally, when living, isoelectric, but that whenever a portion of the muscular substance dies, it becomes while dying negative to the living substance, and thus gives rise to currents. They explain the typical currents (as they might be called) manifested by a muscle with a natural longitudinal surface and artificial transverse sections, by the fact that the dying cut ends are negative relatively to the rest of the muscle. Du Bois-Reymond and those vn.\\\ him offer special explanations of the above facts and of other objections which have been urged against the theory of naturally existing electro-motive molecules. Into these we cannot enter here. We must rest content with the statement that in an ordinary muscle currents such as have been described may be mtnessed, but that strong arguments may be adduced in favour of the view that these currents are not ' natural ' phenomena but essentially of artificial origin. It will therefore be best to speak of them as ' currents of rest.' Negative variation of the Muscle-current. The controversy whether the " currents of rest " observable in a muscle be of natural origin or not, does not affect the truth or the importance of the fact that an electrical change takes place in a muscle whenever it enters into a contraction. When currents of rest are observable in a muscle these are found to undergo a diminution at the onset of a ^ The necessity of its being inactive will be seen subsequently. 62 NEGATIVE VARIATION. [Book i. contraction, and this diminution is spoken of as ' the negative variation ' of the currents of rest. The negative variation may be seen when a muscle is thrown into a single contraction, but is most readily shewn when the muscle is tetanized. Thus if a pair of electrodes be placed on a muscle, one at the equator, and the other at or near the transverse section, so that a considerable deflection of the galvanometer needle, indicating a considerable current of rest, be gained, the needle of- the galvanometer will, when the muscle is tetanized by an interrupted current sent through its nerve (at a point too far from the muscle to allow any escape of the current into the electrodes connected with the galvanometer), swing back towards zero ; it returns to its original deflection when the tetanizing current is shut off. Not only may this negative variation be shewn by the galvano- meter, but it, as well as the current of rest, may be used as a galvanic shock and so employed to stimulate a muscle, as in the experiment known as ' the rheoscopic frog.' For this purpose the muscles and nerves need to be very irritable and in thoroughly good condition. Two muscle-nerve preparations A and B having been made and each placed on a glass plate for the sake of insulation, the nerve of the one B is allowed to fall on the muscle of the other A in such a way that one point of the nerve comes in contact with the equator of the muscle, and another point with one end of the muscle or with a point at some distance from the equator. At the moment the nerve is let fall and contact made, a current, viz. the 'current of rest' of the muscle A, passes through the nerve ; this acts as a stimulus to the nerve, and so causes a contraction in the muscle connected with the nerve. Thus the muscle A acts as a battery, the completion of the circuit of which by means of the nerve of B serves as a stimulus, causing the muscle B to contract. If while the nerve of B is still in contact with the muscle of A, the nerve of the latter is tetanized with an interrupted current, not only is the muscle of A thrown into tetanus but also that of B; the reason being as follows. At each spasm of which the tetanus of A is made up, there is a negative variation of the muscle-current of A. Each negative variation in the muscle- current of A serves as a stimulus to the nerve of B, and is hence the cause of a spasm in the muscle of B ; and the stimuli following each other rapidly, as being produced by the tetanus of A they must do, the spasms in B to which they give rise are also fused into a tetanus in B. B in fact contracts in harmony with A. This experiment shews that the negative variation accompanjdng the tetanus of a muscle, though it causes only a single swing of the galvanometer, is really made up of a series of negative variations, each single negative variation corresponding to the single spasms of which the tetanus is made up. But an electrical change may be manifested even in cases when Chap, ii] THE COyTRACTlLK TISSUES. 63 110 currents of rest exist. We have stated (p. Gl) that the surface of the iininjurt-'d inactive ventricle of the frog's heart is isijeh-ctric, 110 currents being observed when the electrodes of a galvanometer are placed on two points of the surface. Nevertheless a most distinct current is developed whenever the ventricle contracts. This may be shewn either by tlie galvanometer or by the rheos- copic frog. If the nerve of an irritable muscle-nerve preparation be laid over a pulsating ventricle, each beat is responded to by a spasm of the muscle of the preparation. In the case of ordinary muscles too instances occur in w hich it seems impossible to regard the electrical change manifested during the contraction as the mere diminution of a preexisting current. Accordingly Hermann and those who with him deny the existence of ' natural ' muscle-currents speak of a muscle as de- veloping during a contraction a ' current of action,' occasioned as they believe by the muscular substance as it is entering into the state of contraction becoming negative towards the muscular substance which is still at rest, or has returned to a state of rest. In fact, they regard the negativity of muscular substance as characteristic alike of beginning death and of a beginning contraction. So that in a muscular contraction a wave of negativity, starting from the end-plate when indirect, or from the point stimulated when direct stimulation is used, passes along the muscular substance to the ends or end of the fibre. We cannot however enter more fully here into a discussion of this difficult subject. Whichever view be taken of the nature of these muscle-currents, and of the electric change dunng contraction, whether we regard that change as a ' negative variation ' or as a ' current of action,' it is important to remember that it takes place entirely during the latent period. It is not in any way the result of the change of form, it is the forerunner of that change of form. Just as a nervous impulse passes down the nerve to the muscle without any visible changes, so a molecular change of some kind, unattended by any visible events, known to us, at present, only by an electrical change, runs along the muscular fibre from the end-plates to the terminations of the fibre, preparing the way for the visible change of form which is to follow. This molecular invisible change is the work of the latent period, and careful obsersations have shewn that it, like the visible contraction which follows at its heels, travels along the fibre from a spot stimulated towards the ends of the fibres, in the form of a w ave having about the same velocity as the contrac- tion, viz. about 3 metres a second^ 1 In the muscles of the fiog; but as we have seen ha\-ing probably a higher velocdty in the intact mammalian muscles, within the hving body, and var}"ing according to circumstances. 64 CHEMICAL CHANGES. [Book i. Chemical Changes. Before we attack the important problem, What are the chemical changes concerned in a muscular contraction ? we must study in some detail the chemical features of muscle at rest. And here we are brought face to face with the chemical differences between living and dead muscles. All muscles, within a certain time after removal from the body, or while still within the body, after 'general' death of the body, lose their irritability. The loss of irritability, even when rapid, is gradual, but is succeeded by au event which is somewhat more sudden, viz. the entrance into the condition known as rigor mortis, the occurrence of which is marked by the following features. The muscle, previously possessing a certain translucency, becomes much more opaque. Previously very extensible and elastic, it becomes much less extensible and at the same time loses its elasticity; the muscle now requires considerable force to stretch it, and when the force is removed, does not, as before, return to its natural length. To the touch it has lost much of its former softness, and becomes firmer and more resistent. The entrance into rigor mortis is characterised by a shortening or con- traction, which may, under certain circumstances, be considerable. The energy of this contraction is not great, so that when opposed, no actual shortening takes place. When rigor mortis has been fully developed, no muscle-currents whatever are observed. The onset of this rigidity may be considered as the token of the death of the muscle itself. As we shall see, the chemical features of the dead rigid muscle are strikingly different from those of the living muscle. If a dead muscle, from which all fat, tendon, feiscia, and con- nective tissue have been as much as possible removed, and which has been freed from blood by the injection of saline solution, be minced and repeatedly washed with water, the washings will contain certain forms of albumin and certain extractive bodies, of which we shall speak directly. When the washing has been continued until the wash-water gives no proteid reaction, a large portion of muscle will still remain undissolved. If this be treated with a 10 p. c. solution of a neutral salt, ammonium chloride being the best, a large portion of it will become imperfectly dissolved into a viscid fluid which filters with difficulty. If the viscid filtrate be allowed to fall drop by drop into a large quantity of distilled water, a white flocculent matter will be precipitated. This flocculent precipitate is myosin. It is a proteid, giving the ordinary proteid reactions, and having the same general elementary composition as other proteids. It is soluble in dilute saline solutions, especially those of ammonium chloride, and may be classed in the globulin family, though it is not so soluble as paraglobulin. Dissolved in saline solutions it readily coagulates when heated, i. e. Chap, ii.] THE CONTRACTILE TISSUES. 05 is converted into coagulated proteid", and it is worthy of notice that it coac,nilates at a lower temperature, viz. 5o' — GO'C, than does soruni-albuniin, paraglobulin and many other proteids; it is precipitated and after long action coagulated by alcohol, and is precipitated by an excess of sodium chloride. By the action of dilute acids it is very readily converted into what is called syntonin or acid-albumin'^ by the action of dilute alkalis into alkali-albumin. Speaking generally it may be said to be inter- mediate in its character between fibrin and globulin. On keeping, and especially on drying, its solubility is much diminished. Of the substances which arc left in washed muscle, from which the myosin has thus been extracted by ammonium chloride solution, little is known. If washed muscle be treated directly with dilute hydrochloric acid, the greater part of the material of the muscle passes at once into syntonin. The quantity of syntonin thus obtained may be taken as representing the quantity of myosin previously existing in the muscle. The portion insoluble in dilute hydrochloric acid consists in part of the substance of the sarco- Icmma, of the nuclei, and of the tissue betAveen the bundles, and in part probably of certain structural elements of the fibres themselves. If living contractile frog's muscle, freed as much as possible from blood, be frozen^, and while frozen, minced, and rubbed up in a mortar with four times its weight of snow containing 1 p. c. of sodium chloride, a mixture is obtained which at a temperature just below 0" C. is sufiiciently fluid to be filtered, though with difficulty. The slightly opalescent filtrate, or muscle- plasma as it is called, is at first quite fluid, but Avill when exposed to the ordinary temperature become a solid jelly, and afterwards separate into a clot and sei'um. It will in fact coagidate like blood-plasma, with this difference, that the clot is not firm and fibrillar, but loose, granular and flocculent. During the coagidation the fluid, which before was neutral or slightly alkaline, becomes distinctly acid. The clot is myosin. It gives all the reactions of myosin obtained from dead muscle. The serum contains ordinary serum-albumin, one or more pe- culiar proteids* coagidating at a lower temperature than does serum- albumin, and extractives. Such muscles as are red also contain a small quantity of haemoglobin, to which indeed theu' redness is due. Thus while dead muscle contains myosin, serum-albumin, and other proteids and extractives with certain insoluble matters and certain gelatinous elements not referable to the muscle-substance ' See Appendix. • Ibid. 3 Since, as we shall presently see, a muscle may be frozen and thawed again without losing any of its ^-ital powers, we are at liberty to regard the frozen muscle as a still Hving muscle. * See Appendix. F. 5 66 RIGOR MORTIS. [Book i. itself, living muscle contains no myosin, but some substance or substances which bear somewhat the same relation to myosin that the fibrin factors do to fibrin, and which give rise to myosin upon the death of the muscle. We may in fact speak of rigor mortis as characterised by a coagulation of the muscle-plasma, comiparable to the coagulation of blood-plasma, but differing from it inasmuch as the product is not fibrin but myosin. The rigidity, the loss of suppleness, and the diminished translucency appear to be at all events largely, though probably not wholly, due to the change from the fluid plasma to the solid myosin. We might compare a living muscle to a number of fine transparent membranous tubes containing blood-plasma. When this blood-plasma entered into the 'jelly' stage of coagulation, the system of tubes would present many of the phenomena of rigor mortis. They would lose much of their suppleness and translucency, and acquire a certain amount of rigidity. There is however one very marked and important difference between rigor mortis of muscle and the coagulation of blood : blood during its coagulation undergoes only a slight change in its reaction ; but muscle during the onset of rigor mortis becomes distinctly acid. A living muscle at rest is in reaction neutral, or, possibly from some remains of lymph adhering to it, faintly alkaline. If on the other hand the reaction of a thoroughly rigid muscle be tested, it will be found to be most distinctly acid. This development of an acid reaction is witnessed not only in the solid untouched fibre but also in expressed muscle-plasma ; it seems to be associated in some way with the appearance of the myosin. The exact causation of this acid reaction has not at present been clearly worked out. Since the coloration of the litmus pro- duced is permanent, carbonic acid, which as Ave shall immediately state, is set free at the same time, cannot be regarded as the active acid, for the reddening of litmus produced by carbonic acid speedily disappears on exposure. On the other hand it is possible to ex- tract from rigid muscle a certain quantity of lactic acid, or rather of a variety of lactic acid known as sarcolactic acid^; and it has been thought that the appearance of the acid reaction of rigid muscle is due to a new formation or to an increased formation of this sarcolactic acid. But there is considerable doubt whether any such increase of sarcolactic acid does actually take place in rigor mortis. Hence though there can be no doubt that an acid reaction is established, we are not yet in a position to affirm positively the exact manner in which that reaction is produced, the complex nature of the muscular substance suggesting to the chemist several ways in which it might come about. Coincident with the appearance of this acid reaction, though as we have said, not the direct cause of it, a large development of carbonic acid takes place when muscle becomes rigid. Irritable ^ See Appendix. r'liAr. 11.] THE COXTHACTILE TISSUES. 0? living muscular substance like all living jirotoplasni is continually respirinuf, continually consuiniuL,' ()xyL,n-n an^ed long ago that the effect of long continued contraction is to diminish the substances in muscle which are soluble in water, but to increase those which are soluble in alcohol. In other words, during contraction some substance or substances soluble in water are converted into another or other substances insoluble in water but soluble in alcohol. During or after rigor mortis, glycogen is converted into sugar, and it has been contended that a similar change takes place during contraction; but we are not, at present at all events, in a position to affirm that such a conversion is a necessary and integral part of the chemical transformations which lie at the bottom of a muscular contraction. We shall have occasion to treat more fully and from a different point of view, of the relations between muscular exercise and the quantity of urea discharged by the kidneys. Meanwhile we may state that not only does this all-important nitrogenous crystalline body appear to be absent from normal muscle, both during rest and after contraction, but we have as yet no adequate evidence that the contraction of a muscle is followed by the appearance in the substance of the muscle or in the blood passing through it of any new nitrogenous product, or by any increase in any of the nitrogenous extractives which we have mentioned as normally present in muscle. In fact all we know at present is that a contraction is followed by an increase in the discharge of carbonic acid, and by certain changes v/hich lead to an acid reaction. Beyond this we are in the dark. Thermal Changes. The view hoAvever that chemical changes lie at the bottom of a muscular contraction, that the energy which takes on the form of muscular work arises from a metabolism of the muscular substance, is supported by a variety of considerations and especially perhaps by the fact, that the develoj)ment of energy as muscular work, is accompanied by a development of energy as heat. Though we shall have hereafter to treat this subject more fully, the leading facts may be given here. Whenever a muscle contracts, its temperature rises, indicating that heat is given out. When a mercury thermometer is plunged into a mass of muscles, such as those of the thigh of the dog, a rise of the mercury is observed upon the muscles being throAvn into a prolonged contraction. More exact results however are obtained by means of a thermopile, by the help of which the rise of temperature caused by a few repeated single contractions, or indeed by a single contraction, may be observed and the amount of heat given out approximatively measured. Chap, ii.] THE COXTUACTJ LK TISSUES. 71 Tlio tlu'nnoj)il/ the events luhich talce place in the 110 REFLEX ACTIONS. [Book i. protoplasm of the reflex centre. It is not that the afferent impulse is simply reflected in the nerve-cell, and so becomes with but little change an efferent impulse. On the contrary, an afferent impulse passing along a single sensory fibre may give rise to efferent im- pulses passing along many motor nerves, and call forth the most complex movements. An instance of this disproportion of the afferent and efferent impulses is seen in the case where the contact with the glottis of a foreign body so insignificant as a hair causes a violent fit of coughing. Under such circumstances a slight contact with the mucous membrane, such as could not possibly give rise to anything more than few and feeble impulses, may cause the discharge of so many efferent impulses along so many motor nerves, that not only all the respiratory muscles, but almost all the muscles of the body, are brought into action. Similar though less striking instances of how incommensurate are afferent and efferent impulses may be seen in most reflex actions. In fact, the afferent impulse when it reaches the protoplasm of the nerve produces there a series of changes, of explosive disturbances, which, except that the nerve-cell does not in any way change its form, may be likened to the explosive changes in a muscle on the arrival of an impulse along its motor nerve \ The changes in a nerve-cell during reflex action, we might say during any form of activity, far more closely resemble the changes during a muscular contraction than those wdiich accompany the passage along a nerve of either an afferent or efferent impulse. The simple passage along a nerve is accompanied by little expenditure of energy ; it neither gains nor loses force to any great extent as it progresses. The transmutation in a nerve- cell is most probably (though the direct proofs are perhaps wanting) accompanied by a large expenditure of energy, and a simple nervous impulse in suffering the transmutation in a central nervous organ may accumulate in intensity to a very remarkable extent, as in the case of strychnia poisoning. The nature of the efferent impulses is, however, determined also by the nature of the afferent impulses. The nerve-centre remaining in the same condition, the stronger or more numerous impulses will give rise to the more forcible or more comprehensive movements. Thus if the flank of a brainless frog be very lightly touched, the only reflex movement which is visible is a slight twitching of the muscles lying immediately underneath the spot of skin stimulated. If the stimulus be increased, the movements will spread to the hind-leg of the same side, which frequently will execute a movement calculated to push or wipe av/ay the stimulus. By forcibly pinching the same spot of skin, or otherwise increasing the stimulus, the resulting movements may be led to embrace the fore-leg of the same side, then the opposite side, and finally, almost all the muscles of the body. In other words, the disturbance ^ The question as to how far these processes in the central cells are connected with the development of consciousness is here purposely passed over. CiiAi«. Ill ] REFLEX ACTIONS. . Ill set going in the cfiitral luTve-cells, confined ulion tlic stimulus is slight to a few nei"ve-cells and to a few nerve-fibres, overjiaws, so to speak, when the stimulus is increased, on to a number of adjoining and (we must conclude) connected cells, and thus throws impulses into a larger and larger number of efferent nerves. Certain relations may he observed between the sentient spot stimulated and the resulting movement. In the simplest cases of retlcx action this relation is merely of such a kind that the muscles thrown into action are those governed by a motor nerve which is the fellow of the sensory nerve, the stimulation of which calls forth the movement. In the more complex reflex actions of the brainless frog, and in other cases, the relation is of such a kind that the resulting movement bears an adaptation to the stimulus: the foot is with- drawn from the stimulus, or the movement is calculated to push or wipe away the stimulus. In other words, a certain purpose is evident in the reflex action. Thus in all cases, except, perhaps the very simplest, the move- ments called forth by a reflex action are exceedingly complex, com- pared with those which result from the dii-ect stimulation of a motor trunk. When the peripheral stump of a divided sciatic nerve is stimulated with the interrupted current, the muscles of the leg are at once thrown into tetanus, continue in the same rigid condition during the passage of the current, and relax immediately on the current being shut off. When the same current is applied for a second only, to the skin of the flank of a brainless frog, the leg is drawn up and the foot rapidly swept over the spot irritated, as if to wij)e aw^ay the irritation ; but this movement is a complex one, requiring the contraction of particular muscles in a definite sequence, with a carefully adjusted jDroportion between the amounts of contraction of the individual muscles. And this complex move- ment, this balanced and aiTanged series of contractions, may be repeated more than once as the result of a single stimulation of the skin. When a deep breath is caused b}- a dash of cold water, the same co-ordinated and carefully arranged series of contractions is also seen to result, as part of a reflex action, from a simple stimulus. And many more examples might be given. In such cases as these, part of the complexity may be due to the fact that the stimulus is applied to terminal sensor}^ organs and not directly to a nerve-trunk. As we shall see in speaking of the senses, the impulses which are generated by the application of a stimulus to a sensory organ are more complex than those which result from the direct stimulation of a sensory nen'e-trunk. Never- theless, reflex actions of gi-eat if not of equal complexity may be induced by stimuli apjDlied directly to a nerve-trunk. We are therefore obliged to conclude that in a reflex action, the processes which are originated in the central nerv^e-cells by the arrival of even simple impulses along afferent nen^es may be highly complex; and that it is the constitution and condition of the nerve-cells which 112 GAXGL/A. [Book I. determine the complexity and character of the movements which are affected. In other words, the central nerve-cells concerned in reflex actions are to be regarded as constituting a sort of molecular machinery, the character of the resulting movements being deter- mined by the nature of the machinery set going and its condition at the tim.e being, the character and amount of the afferent impulses determining exactly what parts of and how far the central machinery is thrown into action. Actions of Sporadic Ganglia. Seeing that in the spinal cord the nerve-cells undoubtedly are the central structures concerned in the production of reflex action, it is only natural to infer that the nerve-cells of the sporadic ganglia possess similar functions. Yet the evidence of this is at present of very limited extent. With regard to the ganglia on the posterior roots of the spinal nerves, all the evidence goes to shew that these possess no power Vvdiatever of reflex action. Of the larger ganglia visible to the naked eye, such as the ciliary, otic, &c., we have indications of reflex action in one only, viz. the submaxillary, and these indications are, as we shall see in treating of the salivary glands, disputed. We have no exact proof that the ganglia of the sympathetic chain, or of the larger sympathetic plexuses, are capable of executing reflex actions. In fact, in searching for reflex actions in ganglia, we are reduced to the small microscopic groups of cells buried in the midst of the tissues to which they belong, such as the ganglia of the heart, of the intestine, the bladder, &c. When a quiescent frog's heart is stimulated by touching its surface, a beat takes place. This beat is, as v/e shall see, a complex, co-ordinated move- ment, very similar to a reflex action brought about by means of the spinal cord; and in its production it is probable that the cardiac ganglia are in some way concerned. When a quiescent intestine is touched or otherwise stimulated, peristaltic action is set up. Here again the ganglia present in the intestinal walls may be supposed to play a part ; but this movement is much more simple than the beat of the heart, and as regards it, and more especially as regards the similar peristaltic action of the ureter, it becomes difficult to distinguish between a movement governed by ganglia, and one produced by direct stimulation of the muscular fibres. We have seen that the gi-eat distinction between a reflex action and a movement caused by direct stimulation of a nerve or of a muscle lies in the greater complexity of the former ; and we may readily imagine, that by continued simplification of the central nervous machinery, the two might in the end become so much alike as to be almost indistinguishable. In the vertebrate animal then the chief seat of reflex action is the spinal cord and brain. We say 'and brain' because, as we shall see later on, the brain, in addition to its automatism, is as busy a field of reflex action as the spinal cord. Chap, mi.] 1*R0J'ERTIES OF NERVOUS TISSUES. 113 Inhibition. I u speaking of reflex action, wo took it for granted that the spinal cord was, at the moment of the arrival of the afferent impulses at the central nerve-cells, in a quiescent state ; that the nerve-cells themselves were not engaged in any auto- matic action. We were justified in doing so, because as far as the muscles generally of the body are concerned, the spinal cord is in a brainless frog perfectly quiescent ; an afferent impulse reaching an ordinary nerve-cell of the spinal cord does not find it preoccupied in discharging efferent impulses to the muscles with which by means of nerve-fibres it is connected. But what happens when afferent impulses reach a nerve-cell or a group of nen^e-cells already engaged in automatic action ? We have already referred to an automatic respiratory' centre in the medulla oblongata. We may here premise, what we shall shew more in detail hereafter, that the pneumogastric nerve is peculiarly associated as an afferent nerve with this respiratory centre. Now if the central end of the divided pneumogastric be stimulated at the time when the respiratory centre is engaged m its accustomed rhythmic action, sending out complex co- ordinated impulses of inspiration (and of expiration) at regular intervals, one of two things may happen, the choice of events being determined by circumstances which need not be considered here. The most striking event, and the one which interests us now, is that the respiratory rhythm is slowed or stopped altogether. That is to say, afferent impulses which, under ordinaiy con- ditions, would, on reaching a quiescent nervous centre, give rise to movement, may, under certain conditions, when brought to bear on an already active automatic nervous centre, check or stop movement by interfering with the production of efferent impulses in that centre. This stopping or checking an already present action is spoken of as an ' inhibition ; ' and the effect of the pneumogastric in this way on the respiratory centre is spoken of as ' the inhibitory action of the pneumogastric on the respiratory centre.' The other event is that the respiratory rhythm is accelerated. We shall hereafter discuss the explanation of the two events. We may however state that according to one view the pneumo- gastric contains among its afferent fibres two sets, which are either of a different nature from each other, or are so differently connected with the respiratory centre, that impulses arriving along one stop, while those arriving along the other quicken, the action of that centre. Hence, the one set are called ' inhibitory,' the other ' ac- celerating' or 'augmenting' fibres. But we are concerned at present only with the fact that the stimulation of a nerve may produce either inhibitory or augmentative effects. Similarly the vaso-motor centre in the medulla may, by im- pulses arriving along various afferent tracts, be inhibited, during V. 8 114 INHIBITION. [Book i. Chap. hi. which the muscular walls of various arteries are relaxed ; or augmented, whereby the tonic contraction of various arteries is increased. The most striking instance of inhibition is offered by the heart. If when the heart is beating well and regularly, the pneumogastric be divided, and the peripheral portion be stimulated even for a very short time with an interrupted current, the heart is immediately brought to a standstill. Its beats are aiTested, it lies perfectly flaccid and motionless, and it is not till after some little time that it recommences its beat. Here again it is usually said that the pneumogastric contains efferent cardio-inhibitory fibres, impulses passing along which from the medulla stop the automatic actions of the cardiac ganglia; the respiratory inhibitory fibres of the same nerve are afferent, i.e. impulses pass along them up to the medulla. Though inhibition is most clearly seen in the case of automatic actions, other actions may be similarly inhibited. Thus, as we shall see later on, the reflex actions of the spinal cord may, by appropriate means, be inhibited. To sum up, then, the most fundamental properties of nervous tissues. Nerve-fibres are concerned in the propagation only, not in the origination or transformation, of nervous impulses. As far as is at present known, impulses are propagated in the same manner along both sensory and motor nerves. Sensory impulses differ from motor impulses inasmuch as the former are generated in sensory organs and pass up to the central nervous cells, while the latter pass from the central nervous cells to the muscles or to some other peripheral organs. The operations of the nerve-cells are either automatic or reflex. In both an automatic and a reflex action, the diversity and the co-ordination of the impulses are determined by the condition of the nerve-cells. During the passage of an impulse along a nerve- fibre, there is no augmentation of energy ; in passing through a nerve-cell, the augmentation may be, and generally is, most con- siderable. When afferent impulses reach a centre already in action, the activity of that centre may, according to circumstances, be either depressed or exalted, may be ' inhibited ' or ' augmented.' CHAPTER IV. THE VASCULAE MECHANISM. In order that the blood may be a satisfactory medium of com- munication between all the tissues of the body, two things are necessary. In the first place, there must be through all parts of the body a flow of blood, of a certain rapidity and general con- stancy. In the second place, this flow must be susceptible of both general and local modifications. In order that any tissue or organ may readily adapt itself to changes of circumstances (action, repose, &c.), it is of advantage that the quantity of blood passing to it should be not absolutely constant, but capable of variation. In order that the material equilibrium of the body may be main- tained as exactly as possible, it is desirable that the loading of the blood with substances proceeding fi'om the unwonted activity of any one tissue, should be accompanied by a gi-eater flow of blood through some excretory or metabolic tissue by which these substances may be removed. Similarly it is of advantage to the body that the general flow of blood should in some circum- stances be more energetic, and in others less so, than normal. The first of these conditions is dependent on the mechanical and physical properties of the vascular mechanism ; and the problems connected with it are almost exclusively mechanical or physical problems. The second of these conditions depends on the intervention of the nervous system ; and the problems con- nected with it are essentially physiological problems. 8—2 116 PHYSICAL PHENOMENA OF CIRCULATION. [Book i, I. The Physical Phenomena of the Circulation. The apparatus concerned in the Maintenance of the Normal Flow is composed of the following factors : 1. The heart, beating rhythmically by virtue of its contractility and intrinsic mechanisms, and at each beat discharging a certain quantity of blood into the aorta. [For simplicity's sake we omit for the present the pulmonary circulation.] 2. The arteries, highly elastic throughout, with a circular mus- cular element increasing in relative importance as the arteries diminish in size. It must not be forgotten that the muscular element is also elastic. When an artery divides, the united sectional area of the branches is, as a rule, larger than the sectional area of the stem. Thus the collective capacity of the arteries is continually (and rapidly) increasing from the heart towards the capillaries. If all the arterial branches were fused together, they would form a funnel, with its apex at the aorta. The united sectional area of the capillaries has been calculated by Vierordt to amount to several (eight ?) hundred times that of the aorta. 3. The capillaries, channels of exceedingly small but variable size. Their walls are elastic (as shewn by their behaviour during the passage of blood-corpuscles through them), exceedingly thin and permeable. They are permeable both in the sense of allowing fluids to pass through them by osmosis, and also in the sense of allowing white and red corpuscles to traverse them. The small arteries and veins, which gradually pass into and from the capil- laries properly so called, are similarly permeable, the more so, the smaller they are. 4. The veins, less elastic than the arteries (the difference being especially marked when both sets of vessels become distended) and with a very variable muscular element. The united sectional area of the veins diminishes from the capillaries to the heart, thus resem- bling the arteries ; but the united sectional area of the venae cavse at their junction with the right auricle is greater than that of the aorta at its origin. (The proportion is nearly two to one.) The total capacity of the veins is similarly much greater than that of the arteries. The veins alone can hold the total mass of blood which in life is distributed over both arteries and veins. Indeed nearly the whole blood is capable of being received by what is merely a part of the venous system, viz. the vena portsa and its branches. Such veins as are for various reasons liable to a reflux of blood from the heart towards the capillaries are provided with valves. SEC. 1. MAIN GENERAL FACTS OF THE CIRCULATION. The Capillary Circulation. If the web of a frog's foot be examined with a microscope, the blood, as judged of by the movements of the corpuscles, is seen to be passing in a continuous stream from the small arteries through the capillaries to the veins. The velocity is greater in the arteries than in the veins, and greater in both than in the capillaries. In the arteries faint pulsations, sjmchronous with the heart's beat, are occasionally visible ; and not unfrequently varia- tions in velocity and in the distribution of the blood, due to causes which will be hereafter discussed, are Nvitnessed from time to time. The flow through the smaller capillaries is very variable. Sometimes the corpuscles are seen passing through the channel in single file with great regularity; at other times, they may be few and far between. Sometimes the corjiuscle may remain stationary at the entrance into a capillary, the channel itself being for some little distance entirely free from corpuscles. Any one of these conditions readily passes into another; and, especially with a somewhat feeble circulation, instances of all of them may be seen in the same field of the microscope. It is only when the vessels of the web are unusually full of blood that all the capillaries can be seen equally filled with corpuscles. The long oval red corpuscle moves with its long axis parallel to the stream, frequently rotating on its long axis and sometimes on its short axis. The flexibility and elasticity of a corpuscle are well seen when it is being driven into a 118 THE CAPILLARY CIRCULATION. [Book i. capillary narrower than itself, or when it becomes temporarily lodged at the angle between two diverging channels. The small mam- malian corpuscles rotate largely as they are driven along. In the web of the frog's foot the average velocity with which the corpuscles move may be put down as about half a millimetre in a second. In the human retina, the velocity of the capillary flow has, by indirect methods, been estimated at '75 mm. per sec. The movement of the blood in the capillaries is very slow, compared with that in the arteries or even in the veins. In the larger capillaries, and especially in the small arteries and veins which permit the passage of several corpuscles abreast, it is observed that the red corpuscles run in the middle of the channel, forming a coloured core, between which and the sides of the vessel all round is a layer, which has been called the ' inert layer,' or better the 'plasmatic layer,' containing no red corpuscles. This division into a plasmatic layer and an axial stream is due to the fact that in any stream passing through a closed channel the friction is greatest at the immediate sides, and diminishes towards the axis. The corjDuscles pass where the friction is least, in the axis, A quite similar axial core is seen when any fine particles are driven with a sufficient velocity in a stream of fluid through a narrow tube. As the velocity is diminished the axial core becomes less marked and disappears. In the plasmatic layer, especially in that of the veins, are frequently seen white corpuscles, sometimes clinging to the sides of the vessel, sometimes rolling slowly along, and in general moving irregularly, and often in jerks. The greater the velocity of the flow of blood, the fewer the white corpuscles in the plasmatic layer, and with a very rapid flow they, as well as the red corpuscles, may be all confined to the axial stream. The presence of the white corpuscles in the plasmatic layer has been attributed to their being specifically lighter than the red corpuscles, it being affirmed that when fine particles of two kinds, one lighter than the other, are driven through a narrow tube, the heavier particles flow in the axis and the lighter in the more peripheral portions of the stream. This however has been disputed, and the phenomenon explained by the white corpuscles being dis- tinctly more adhesive than the red, as is seen by the manner in which they become fixed to the glass slide and cover-slip when a drop of blood is mounted for microscopical examination. By reason of this adhesiveness which possibly may vary with the varying nutritive conditions of the corpuscles and of the blood- vessels, the white corpuscles, it is urged, become temporarily attached to the walls of the vessel, and consequently appear in the plasmatic layer. The resistance to the flow of blood thus caused by the Mction generated in so many minute passages, is one of the most important physical facts in the circulation. In the large arteries the friction is small ; it increases as they divide, and receives a very great Chap, iv.] THE VASCULAR MIX If AX ISM. 119 120 THE FLOW IN THE ARTERIES. [Book i. Fig, 17. Apparatus for investigating Blood-pbessuee. At the tipper right-hand comer, is seen, on an enlarged scale, the carotid artery, clamped by the forceps hd, with the vagus nerve v lying by its side. The artery has been ligatured at V and the glass cannula c has been introduced into the artery between the ligature V and the forceps hd, and secured in position by the ligature I. The shrunken artery on the distal side of the cannula is seen at ca'. p.h. is a box containing a bottle holding a saturated solution of sodium car- bonate or a solution of sodium bicarbonate of sp. gr. 1083, and capable of being raised or lowered at pleasure. The solution flows by the tube p. t regulated by the clamp c" into the tube t. A syringe, with a stop-cock, may be substituted for the bottle, and attached at c". This indeed is in many respects a more convenient plan. The tube t is connected with the leaden tube t, and the stopcock c with the mano- meter, of which m is the descending and m' the ascending limb, and s the support. The mercury in the ascending limb bears on its surface the float fl, a long rod attached to which is fitted with the pen p, writing on the recording surface ?•. The clamp cl. at the end of the tube t has an arrangement shewn on a larger scale at the right hand upper corner. The descending tube m of the manometer, and the tube t being completely filled along its whole length with fluid to the exclusion of all air, the cannula c is filled with fluid, slipped into the open end of the thick- walled india-rubber tube i, until it meets the tube t (whose position within the india-rubber tube is shewn by the dotted lines), and is then securely fixed in this position by the clamp cl. The stopcocks c and c" are now opened, and the pressure-bottle raised or fluid driven in by the syringe until the mercury in the manometer is raised to the required height. The clamp c" is then closed and the forceps bd removed from the artery. The pressure of the blood in the carotid ca. is -in consequence brought to bear through t upon the mercury in the manometer. addition in the minute arteries and capillaries. We may speak of it therefore as the 'peripheral friction' and the resistance which it offers as the 'peripheral resistance.' It need perhaps hardly be said that this peripheral friction not only opposes the flow of blood through the capillaries themselves, but, working backwards along the whole arterial system, has to be met by the heart at each systole of the ventricle. It is well known that when any portion of the skin is pressed upon, it becomes pale and bloodless; this is due to the pressure driving the blood out of the capillaries and minute vessels and preventing any fresh blood entering into them. By carefully investigating the amount of pressure necessary to prevent the blood entering the capillaries and minute arteries of the web of the frog's foot, or of the skin beneath the nail in man or elsewhere, the internal pressure which the blood is exercising on the walls of the capillaries and minute arteries and veins may be approximately determined. In the frog's web this has been found to be equal to about 7 or 11 mm, mercury. 2. The Flow in the Arteries. When an artery is severed, the flow from the proximal section is not equable, but comes in jets, which correspond to the heart- fJn.M'. IV. 1 THE I'ASCL'LAA' MFJ'HAMSM. 121 beats, though the flow does not cease between the jets. The blood is ejected with considerable force; thus, in l)r Stephen Hales' experiments, when the crural artery of a mare was severed, the jet, even alter much loss of blood, rose to the height of two feet. The larger the artery and the nearer to the heart, the greater the force with whieh the blood issues, and the more marked tne intcrmittencc of the tlow. The How from the distal section may be very slight, or may take place with consiilerablc force and marked intermittence, according to the amoimt of collateral communication. Arterial pressure. If a mercury (or other) manometer. Fig. V7 m, in', be connected with a large artery, e.g. the carotid, in such a way that while the blood is allowed to flow uninterruptedly along the artery, there is free communication between the interior of the artery and the proximal (descending) limb of the manometer, the following facts are observed. Immediately that communication is established between the interior of the artery and the manometer, blood rushes from the former into the latter, driving some of the mercury from the de- scending limb into the ascending limb, and thus causing the level of the mercury in the ascending limb to rise rapidly. This rise is marked by jerks corresponding with the heart-beats. Having reached a certain level, the mercury ceases to rise any more. It does not, however, remain absolutely at rest, but undergoes oscilla- tions ; it keeps rising and falling. Each rise, which is very slight compared with the total height to which the mercury has risen, has the same rhythm as the systole of the ventricle. Similarly, each fall corresponds with the diastole. If a float, swimming on the top of the mercury in the ascending limb of the manometer, and bearing a brush or other marker, be brought to bear on a travelling surface, some such tracing as that represented in Fig. 18 will be described. Each of the smaller r r Fig. 18. Tracing of Arterial Pressure with a Mercury Manometer. The smaller curves p p are the pulse-curves. The space from r to r embraces a respiratory undulation. The tracing is taken from a clog, and the irregularities visible in it are those frequently met with in this animal. curves ( p, p) corresponds to a heart-beat, the rise corresponding to the systole and the fall to the diastole of the ventricle. The larger undulations (r, r) in the tracing, which are respiratory in origin, 122 ARTERIAL PRESSURE. [Book i. will be discussed hereafter. This observation teaches us that the blood, as it is passing along the carotid artery, is capable of support- ing a column of mercury of a certain height (measured by the difference of level between the mercury in the descending limb, and that in the ascending limb, of the manometer), when the mercury is placed in direct communication with the side of the stream of blood. In other words, the blood, as it passes through the artery, exerts a lateral pressure on the sides of the artery, equal to so many millimeters of mercury. In this lateral pressure we have further to distinguish between the slighter oscillations corre- sponding with the heart-beats, and a mean pressure above and below which the oscillations range. A similar mean pressure with similar oscillations is found, when any artery of the body is examined in the same way. In all arteries the blood exerts a certain pressure on the walls of the vessels which contain it. This is generally spoken of as arterial pressure or arterial tension, and the pressure in the aorta of any animal is usually spoken of as its blood- pressure. Description of Experiment, The carotid, or other vessel, is laid bare, clamped in two places and divided between the clamps. Into the cut ends is inserted a hollow |— piece of the same bore as the artery, the cross portion forming the continuation of the artery. The other portion is connected by means of a non-elastic flexible tube with the descending limb of the manometer. In order to avoid loss of blood, fluid is in- jected into the flexible tube until the mercury in the manometer stands a very little below what may be beforehand guessed at as the probable mean pressure. The fluid chosen is a saturated solution of sodium car- bonate or a solution of sodium bicarbonate of sp. gr. 1083, with a view to hinder the coagulation of the blood in the tube. When the clamps are removed from the artery the blood rushes through the cross of the |— piece. Some passes into the side limb of the H piece and continues to do so until the mean pressure is quite reached. Thenceforward there is no more escape ; but the pressure continues in the interior of the |— piece, is transmitted along the connecting tube to the manometer, and the mercury continues to stand at a height indicative of the mean pressure with oscillations corresponding to the heart's beats. Practically the use of the I— piece is found inconvenient. Accordingly the general custom is to ligature the artery, to place a clamp on the vessel on the proximal side of the ligature, and to introduce a straight cannula. Fig. 17 c, connected with the manometer, into the artery between the ligature and the clamp, and to secure it in that position. In this case, on loosing the clamp, the whole column of blood in the artery is brought to bear on the manometer, and the tracings taken illustrate the lateral pressure not of the artery in which the cannula has been placed, but of the vessel (aorta &c. as the case may be) of which it is itself a branch. Tracings of the movements of the column of mercury in the mano- meter may be taken either on a smoked surface of a revolving cylinder (Fig. 1), or by means of a brush and ink on a continuous roll of paper, as in the more complex kymograph (Fig. 1 9). CHAI'. IV.] THE VASCULAR MECHANISM. 123 In such a inorcury luunometer, the in«rtia of tlio mercury obscuros many of tho features of the minor curves caused by the heart^beats. When therefore tlu-se, rath(^r than variations in the mean pressure, arc bcin<^ studied, other methods have to be adopted. The average pressure of the blood in the same body is greatest in the hxrgest arteries, and diminishes as the arteries get less; but the fall is a very gradual cue until the smallest arteries are reached, in which it becomes very rapid. In the carotid of the horse, the mean arterial pressure varies from 150 to 200 mm. of mercury ; of the dog from 100 to 175 ; of the rabbit from 50 to 90. In the carotid of man it probably amounts to 150 or 200. Fig. 19. Labge Kymograph with continuous roll of papek. The clock-work machinery, some of the details of which are seen, unrolls the paper from the roU C, carries it smoothly over the cylinder B, and then winds it up into the roll A. Two electromagnetic markers are seen in the position ia which they record their movements on the paper as it travels over B. The manometer, or any other recording instrument used, can be fixed either in the notch immediately in front of B or in any other position that may be desired. Since in all arteries the blood is pressing on the arterial walls with some considerable force, all the arteries must be in a state of permanent distension, so long as blood is flowing through them from the heart. When the blood-current is cut off, as by a ligature, this expansion or distension disappears. Not only is there a permanent expansion corresjaonding to the mean pressure, but just as the mercury in the manometer rises above the level of mean pressure at each systole of the heart, and 124 THE VELOCITY OF THE FLOW. [Book i. falls below it at each diastole, so at any spot in the artery there is for each heart-beat a temporary expansion succeeded by temporary contraction, the diameter of the artery in its temporary expansions and contractions oscillating, in correspondence with the oscillations of the manometer, beyond and within the diameter of permanent expansion. These temporary expansions constitute what is called the pulse, and will be discussed more fully hereafter. The velocity of the flow. When even a small artery is severed a considerable quantity of blood escapes from the proximal cut end in a very short space of time. That is to say, the blood moves in the arteries from the heart to the capillaries, with a very con- siderable velocity. By various methods, this velocity of the blood- current has been measured at different parts of the arterial system; the results, owing to imperfections in the methods employed, cannot be regarded as satisfactorily exact, but may be accepted as approxi- mately true. The velocity of the arterial stream is greatest in the largest arteries, and diminishes from the heart to the capillaries, •pari passu with the increase of the width of the bed, i.e. with the increase of the united sectional area. Methods. The Hsemadromometer of Yolkmann. An artery, e.g. a carotid, is clamped in two places, and divided between the clamps. Two cannulse, of a bore as nearly equal as possible to that of the artery, or of a known bore, are inserted in the two ends. The two cannulse are con- nected by means of two stop-cocks, which work together, with the two ends of a long glass tube, bent in the shape of a U, and filled with normal saliae solution, or with a coloured innocuous fluid. The clamps on the artery being released, a turn of the stop-cocks permits the blood to enter the proximal end of the long U tube, along which it courses, driving the fluid out into the artery through the distal end. Attached to the tube is a graduated scale, by means of which the velocity with which the blood flows along the tube may be read off. Even supposing the cannulse to be of the same bore as the artery, it is evident that the conditions of the flow through the tube are such as will only admit of the result thus gained being considered as an approximative estimation of the real velocity in the artery itself. The Hheometer (Stromuhr) of Ludwig. This consists of two glass bulbs A and B, Fig. 20, communicating above with each other and with the common tube C by which they can be filled. Their lower ends are fixed in the metal disc Z>, which can be made to rotate, through two right angles, round the lower disc E. In the upper disc are two holes a and b continuous with A and B respectively, and in the lower disc are two similar holes a and b', similarly continuous with the tubes H and 0. Hence, in the position of the discs shewn in the figure, the tube G is continuous through the two discs with the bulb A and the tube H with the bulb B. On turning the disc D through two right angles the tube G becomes continuous with B instead of A, and the tube H with A instead of B. There is a further arrangement, omitted from the figure for the sake of simplicity, by which when the disc D is turned through one Chap. iv.J THE VASCULAR MKCIIAXISM. 125 instead of two right angles from either of the above positions, G becomes directly continuous with //, both being completely shut off from the bulbs. Fig. 20. Dugbammatic Representation of Lutwio's Stkomuhr. The ends of the tubes H and G are made to fit exactly into two cajinulse inserted into the two cut ends of the artery about to be experi- mented upon, and having a bore as nearly equal as possible to that of the artery. The method of experimenting is us follow^s. The disc D, being placed in the intermediate position, so that a and h are both cut ofi" from a and h' , the bulb A is filled with pure olive oil up to the mark o:, and the bulb B, the rest of A, and the junction C, with defibrinated' blood; and C is then clamped. The tubes H and G are also filled ^ith de- fibrinated blood, and G is inserted into the cannula of the central, U into that of the peripheral, end of the artery. On removing the clamps from the artery the blood flows through G to H, and so back into the artery. The observation now begins by turning the disc D into the position shewn in the figure ; the blood then flows into A , driving the oil there contained out before it into the bulb B, in the direction of the arrow, the defibrinated blood pre^dously present in B passing by H into the artery, and so into the system. At the moment that the blood is seen to rise to the mark x, the disc D is with all possible rapidity turned through two right angles: and thus the bulb B, now largely filled with oil, placed in communication with G. The blood-stream now drives the oil back into A, and the new blood in ^-1 through If into the artery. As soon as the oil has wholly returned to its original position, the disc is again turned round, and A once more placed in communication with G, and the oil once more driven from A to B. And this is repeated several times, indeed generally until the clotting of the blood or the admixture of the oil Avith the blood puts an end to the experiment. Thus the flow of blood is used to fill alternately with blood or oU the space of the bulb ^, whose ca\ity as far as the mark x has been exactly measured; hence if the number of times in any given time the disc J) has to be turned round be kno-«Ti, the number of times A has been filled is also known, and thus the quantity of blood which has passed in that time through the 126 MEASUREMENTS OF VELOCITY OF FLOW. [Book i. cannula coimected with the tube G is directly measured. For instance, supposing that the quantity held by the bulb A when filled up to the mark £c is 5 c.c, and supposing that from the moment of allowing the first 5 c.c. of blood to begin to enter the tube to the moment when the escape of the last 5 c.c. from the artery into the tube was complete, 100 seconds had elapsed, dui'ing which time 5 c.c. had been received 10 times into the tube from the artery (all but the last 5 c.c. being returned into the distal portion of the artery), obviously "5 c.c. of blood had flowed from the proximal section of the artery in one second. Hence supposing that the diameter of the cannula (and of the artery, they being the sam.e) were 2 mm., with a sectional area therefore of 3-14: square mm., an outflow through the section of -5 c.c. or 500 c.mm. in a second would give (l-yl-), a velocity of about 159 mm. in a second. The Heematachometer of Vierordt is constructed on the principle of measuring the velocity of the current by observing the amount of devia- tion undergone by a pendulum, the free end of which hangs loosely in the stream. A square or rectangular chamber, one side of which is of glass and marked with a graduated scale in the foi'm of an arc of a circle, is connected by means of two short tubes with the two cut ends of an artery; the blood consequently flows from the proximal (central) portion of the artery through the chamber into the distal portion of the artery. Within the chamber and suspended from its roof is a short pendulum, which when the blood-stream is cut ofi" from the chamber hangs motionless in a vertical position, but when the blood is allowed to flow through the chamber, is driven by the force of the current out of its position of rest. The pendulum is so placed that a marker attached to its free end travels close to the inner surface of the glass side along the arc of the gTaduated side. Hence the amount of de^dation from a vertical position may easily be read off on the scale from the outside. The graduation of the scale haAong been carried out by experimenting with streams of known velocity, the velocity can at once be calculated from the amount of deviation. An instrument based on the same principle has been invented by Chauveau and improved by Lortet. In this the part which corresponds to the pendulum in Yierordt's instrument is prolonged outside the chamber, and thus the portion within the chamber is made to form the short arm of a lever, the fulcrum of which is at the point where the waU of the chamber is traversed and the long arm of which projects outside. A somewhat wide tube, the wall of which is at one point composed of an india-rubber membrane, is introduced between the two cut ends of an artery. A long light lever pierces the india-rubber membrane. The short expanded arm of this lever projecting within the tube is moved on its fulcrum in the india-rubber ring by the current of blood passing through the tube, the greater the velocity of the current, the larger being the excursion of the lever. The movements of the short arm give rise to corresponding movements in the opposite direction of the long arm outside the tube, and these, by means of a marker attached to the end of the long ai-m, may be directly inscribed on a recording surface. This instrument is very well adapted for observing changes in the velocity of the flow. In determining actual velocities, for which purpose it has to be experimentally graduated, it is not so useful. Chap. iv.J THE VASCULAR MECHANISM. 127 in the horse, Volkinanu found the velocity of the stream to bo ill tlic caiotitl artery about 300 iiiiii., in the maxillary artery 165 mm., and in the metatarsal artery 50 mm. in the .second. Chauveau determined the velocity in the carotid of the horse to vary from 520 to 150 mm. per sec. at each beat of the heart, flow- ing at the former rate during the height of each pulse-expansion, and at the latter in the interval between each two beats. Ludwig and Dogiel found the velocity in the dog and in the rabbit to vary within very wide limits, not only in different arteries, l)ut in the same artery under different circumstances. Thus while in the carotid of the rabbit it may be said to vary from 100 to 200 mm. per sec, and in the carotid of the dog from 200 to 500 mm. per sec, both these limits were frequently passed. 3. The Flow in the Veins. When a vein is severed, the flow from the distal cut end {i.e. the end nearest the capillaries) is continuous, the blood is ejected with comparatively little force, and with no great velocity. When a vein is connected with a manometer, the lateral pressure is found to be very small ; it is greater in the veins farther from the heart than in those nearer the heart. In the former it is much less than that of the small arteries, and in the latter amounts only to a few millimetres of mercury. Indeed in the immediate neigh- bourhood of the heart the pressure may (during the inspii-atory movement) become negative, i.e. when the manometer is brought into connection with the interior of the vein, the mercury in the distal limb falls, instead of, as in the case of an artery, rising. In the case of most veins, under ordinary circumstances the mercury of a manometer connected with a vein does not shew any of those pulse-oscillations which are so striking in the arteries. As a general rule the pulse is seen on the arterial side only of the capillaries, though in special cases, under conditions which we shall study presently, it may make its way through the capillaries from the arteries to the small veins ; and it is probable that in general a slight impulse does make its way right through the capil- laries, but so feeble that it cannot be recognised by ordinary in- struments save in special cases. Moreover, in the great veins near the heart, under certain circumstances at all events, the movements of that organ may make themselves felt as a so-called 'venous pulse' transmitted in a backward direction along the veins from the heart. But these exceptional instances and these recuiTent oscillations do not invalidate the truth of the general statement that the pulse is absent from the veins. The exact determination of venous pressure is attended ^vith great ex]")crimental difficulties, and our knowledge in 128 THE FLOW IN THE VEINS. [Book i. this direction is very incomplete ; but in all probability the pressure in a vein varies within much wider limits than does the pressure in the corresponding artery. In the small veins the velocity of the current, measured in the same way as in the case of the arteries, is very slight. It increases in the larger veins, corresponding to the diminution of the area of ' the bed ' ; it is about 200 mm. per sec. in the jugular vein of the dog. Thus the flow in the veins presents strong contrasts with that in the arteries. In the arteries, even in the smallest branches, there is a considerable mean pressure. In the veins, even in the small veins where it is largest, the mean pressure is very slight. In other words, there is always a difference of pressure tending to make the blood flow continuously from the arteries into the veins, A pulse is present in the arteries, but, with certain exceptions, absent in the veins. The velocity of the stream of blood in the arteries is considerable ; in the small veins it is much less, but it increases in the larger trunks ; for in both arteries and veins it corresponds with the area of the bed, diminishing in the former from the heart to the capillaries, and increasing in the latter from the capillaries to the heart. Hydraulic Principles of the Circulation. All the above phenomena are the simple results of an intermit- tent force (like that of the systole of the ventricle) working in a closed circuit of branching elastic tubes, so arranged that while the individual tubes first diminish (from the heart to the capillaries) and then increase (from the capillaries to the heart), the area of the bed first increases and then diminishes, the tubes together thus forming two cones placed base to base at the capillaries, with their apices converging to the heart. To this it must be added that the friction in the small arteries and capillaries, at the junction of the bases of the cones, offers a very great resistance to the flow of the blood through them. It is this peripheral resistance (in the minute arteries and capillaries, for the resistance offered by the friction in the larger vessels may, when compared with this, be practically neglected), reacting through the elastic walls of the arteries upon the intermittent force of the heart, which gives the circulation of the blood its peculiar features. Circmnstances determining the character of the flow. When fluid is driven by an intermittent force, as by a pump, through a perfectly rigid tube (or system of tubes), there escapes at each stroke of the pump from the distal end of the system just as much fluid as enters it at the proximal end. The escape moreover takes place at the same time as the entrance, since the time taken up by CiiAi'. IV.] 77/ A" VASCi'LMt MKCIIAMSM. Il>9 the transmission of the shock is so small, tli;it it may bo neglectod. This result remains the same when any resistance to the tiow is introduced into the system. The force of the pump remaining the same, the introduction of the resistance undoubtedly lessens the quantity issuing at the distal end at each stroke, but it does so simply by lessening the (juantity entering at the proximal end ; the income and outgo remain equal to each other, and occur at almost the same time. And what is true of the two ends, is also true of any part of the course of the system, so iar, at all events, as the following proposition is concerned, that in a system of rigid tubes, either with or without an intercalated resistance, the tiow caused by an intermittent force is, in every part of the tubes, intermittent synchronously with that force. In a system of elastic tubes in which there is little resistance to the progress of the fluid, the flow caused by an intermittent force is also intermittent. The outgo being nearly as easy as the income, the elasticity of the walls of the tubes is scarcely at all called into play. These behave practically like rigid tubes. When, however, sufficient resistance is introduced into any part of the course, the fluid, being unable to pass by the resistance as rapidly as it enters the system from the pump, tends to accumulate on the proximal side of the resistance. This it is able to do by expanding the elastic walls of the tubes. At each stroke of the pump a certain quantity of fluid enters the system at the proximal end. Of this only a fraction can pass through the resistance during the stroke. At the moment when the stroke ceases, the rest still remains on the proximal side of the resistance, the elastic tubes having expanded to receive it. During the interval between this and the next stroke, the distended elastic tubes, striving to return to their natural undistended condition, press on this extra quantity of fluid which they contain and tend to drive it past the resistance. Thus in the rigid system (and in the elastic system without resistance) there issues, from the distal end of the system, at each stroke, just as much fluid as enters it at the proximal end, while between the strokes there is perfect quiet. In the elastic system with resistance, on the contrary, the quantity which passes the resistance is only a fraction of that which enters the system from the pump, the remainder or a portion of the remainder continuing to pass during the inter\al between the strokes. In the former case, the system is no fuller at the end of the stroke than at the besrinninof ; in the latter case there is an accumulation of fluid between the pump and the resistance, and a corresponding dis- tension of that part of the system, at the close of each stroke — an accumulation and distension, however, which go on diminishing until the next stroke comes. The amount of fluid thus remaining after the stroke will depend on the amount of resistance in relation to the force of the stroke, and on the distensibility of the tubes ; and the amount which passes the resistance before the next stroke 130 INTERMITTENT FLOW. [Book i. will depend on the degree of elastic reaction of which the tubes are capable. Thus, if the resistance be very considerable in relation to the force of the stroke, and the tubes very distensible, only a small portion of the fluid will pass the resistance, the greater part remaining lodged between the pump and the re- sistance. If the elastic reaction be great, a large portion of this will be passed on through the resistance before the next stroke comes. In other words, the greater the resistance (in relation to the force of the stroke), and the more the elastic force is brought into play, the less intermittent, the more nearly continuous, will be the flow on the far side of the resistance. If the first stroke be succeeded by a second stroke before its quantity of fluid has all passed by the resistance, there will be an additional accumulation of fluid on the near side of the resistance, an additional distension of the tubes, an additional strain on their elastic powers, and, in consequence, the flow between this second stroke and the third will be even more marked than that between the first and the second, though all three strokes were of the same force, the addition beino- due to the extra amount of elastic force called into play. In fact, it is evident that, if there be a sufficient store of elastic power to fall back upon, by continually repeating the strokes a state of things will be at last arrived at, in which the elastic force, called into play by the continually increasing dis- tension of the tubes on the near side of the resistance, will be sufiicient to drive through the resistance, between each two strokes, just as much fluid as enters the near end of the system at each stroke. In other words, the elastic reaction of the walls of the tubes will have converted the intermittent into a continuous flow. The flow on the far side of the resistance is in this case not the direct result of the strokes of the pump. All the force of the pump is spent, first in getting up, and afterwards in keeping up, the over-distension of the tubes on the near side of the resistance ; the cause of the continuous flow lies in the over-distension of the tubes which leads them to empty of themselves into the far side of the resistance, at such a rate, that they discharge through the resistance during a stroke and in the succeeding interval just as much as they receive from the pump by the stroke itself. This is exactly what takes place in the vascular system. The friction in the minute arteries and capillaries presents a considerable resistance to the flow of blood through them into the small veins. In consequence of this resistance, the force of the heart's beat is spent in maintaining the whole of the arterial system in a state of over-distension, as indicated by the arterial pressure. The over- distended arterial system is, by the agen3y of its elastic walls, con- tinually emptying itself by overflowing through the capillaries into the venous system, overflowing at such a rate, that just as much blood passes from the arteries to the veins during each systole and its succeeding diastole as enters the aorta at each systole. CiiAiv IV.] TIIK I'ASrr/.A/i M/'X'I/AX/SM. 131 It cannot be too much insisted upon that the whole arterial system is over-distended. This is what is meant by the high arterial pressure. On the other hand, the veins are much les.s distended. This is shewn by the low venous pressure. The dis- tended arteries are continually striving to pass their suq>lus in a continuous stream through the capillaries into the vein.s, so as to bring both venous and arterial pressure to the same level. As continually the heart by its beat is keeping the arteries distended, and thus maintaining the ditference between the arterial and venous pressure, and thus preserving the steady capillary stream. When the heart ceases to beat, the arteries do succeed in emptying their suqilus into the veins, and when the pressure on both sides of the capillaries is thus equalized, the flow through the capillaries ceases. In the facts just discussed, it makes no essential difference whether the outflow on the far side of the resistance be an open one, or whether, as is the case in the vascular system, the fluid be returned to the pump, provided only that the resistance offered to that return be sufficiently small. We shall see, in speaking of the heart, that, so far from there being any resistance to the flow of blood from the great veins into the auricle, the flow is favoured by a variety of circumstances. We have seen moreover that, besides the very sudden decrease in the immediate neighbourhood of the capillaries, there is in passing along the whole vascular system from the aorta to the venae cav£e a gradual fall of pressure. A little consideration shews that this must be the case. After what has been said it is obvious that the movement of the blood may be compared to that of a body of fluid, driven by pressure from the ventricle through the vessels to its outflow in the auricle. Were the pressure a continuous one, and were there no peripheral resistance, there would be a gradual fall of pressure, from the part farthest from the outfall, viz. the aorta, to the part nearest the outfall, viz. the veme cavte. The introduction of the peripheral resistance and its attendant phenomena gives rise to the feature of a very sudden and marked fall in the capillar}' region, but leaves untouched the gradual character of the fall in the rest of the course, from the aorta to the minute arteries, and from the minute veins to the vena3 cava?. To recapitulate : there are three chief factors in the mechanics of the circulation, (I) the force and frequency of the heart-beat, (2) the peripheral resistance, (3) the elasticity of the arterial walls. These three factors, in order to produce a normal circulation, must be in a certain relation to each other. A disturbance of these relations brings about abnormal conditions. Thus, if the peripheral resistance be reduced beyond certain limits, while the force and frequency of the heart remain the same, so much blood passes through the capillaries at each stroke of the heart that there is not sufficient left behind to distend the arteries, and bring their 9—2 132 VARIATIONS IN VELOCITY. [Book i. elasticity into play. In this case the intermittence of the arterial flow is continued on into the veins. An instance of this is seen in the experiments on the sub-maxillary gland, where sometimes the resistance oflered by the minute arteries of the gland is so much lowered, that the pulse is carried right through the capillaries, and the blood in the veins of the gland pulsates^ A like result occurs when, the peripheral resistance remaining the same, the frequency of the heart's beat is lowered. Thus the beats may be so infrequent that the whole quantity sent on by a stroke has time to escape before the next stroke comes. Lastly, if, while the heart's beat and the peripheral resistance remain the same, the arterial walls become more rigid, the arteries will be unable to expand sufficiently to retain the surplus of each stroke or to exert sufficient elastic reaction to carry forward the stream between the strokes ; and in consequence more or less intermittence will become manifest. Circumstances determining the velocity of the flow. We have seen that the velocity of the blood-stream diminishes from the aorta to the capillaries, and increases from the capillaries to the great veins. Thus in the dog the velocity in the great arteries may be stated at from 300 to 500 mm., in the capillaries at less than 1 mm. ('5 to "75 mm.), and in the large veins at about 200 mm. in a sec. In fact, the greater part of the time of the circuit is taken up in the capillary region. An iron salt, injected into the jugular vein of one side of the neck of a horse, makes its appear- ance in the blood of the jugular vein of the other side in about 30 seconds. Hering's mean result in the horse was 27*6 sees. In the dog Vierordt found it to be 15*2 sees.; in the rabbit 7 sees. Without laying too much stress on this experiment, it may be taken as a fair indication of the time in which the whole circuit may be completed. It takes about the same time to pass through about 20 mm. of capillaries. Hence, if any corpuscle had in its circuit to pass through 10 mm. of capillaries, half the whole time of its journey would be spent in the narrow channels of the capillaries. Since, however, the average length of a capillary is about "5 mm., about one second is spent in the capillaries. In- asmuch as the purposes served by the blood are chiefly carried out in the capillaries, it is obviously of advantage that its stay in them should be prolonged. The local differences in the velocity of the stream are directly dependent on the area of the 'bed.' When a fluid is driven by a uniform pressure through a narrow tube with an enlarge- ment in the middle, the velocity of the stream diminishes in the enlargement, but increases again when the tube once more narrows. So a river slackens speed in a ' broad' but rushes on ^ See Book i. cap. i. sec. 2, on the Secretion of the Digestive Juices. Chap iv] TlIK V ASCI' LA R MhV//A.V/S.]/. |:33 rapidly again when the banks close in. Exactly in the same way the velocity of the blood-stream slackens from the aorta to the capillaries corresponding with the increased total ])ed, but hurries on again as the numerous veins are gathered into the smaller bed of the vena? cavie. The loss of velocity in the caj)illaries, as com- pared with the arteries, is not due to there being so much more friction in the narrow channels of the former than in the wide canals of the latter. For the peripheral resistance caused by the friction in the capillaries and small arteries is an obstacle not only to the tiow of blood through these small vessels where the resist- ance is actually generated, but also to the escape of the blood from the large into the small arteries, and indeed from the heart into the large arteries. It exerts its influence along the whole arterial tract. And it is obvious that if it were this peripheral resistance which checked the flow in the capillaries, there could be no re- covery of velocity along the venous tract. The rapidity of the flow in arteries, capillaries, and veins, is in each case determined by the total sectional area of the channels. There is, however, a loss of velocity on the whole course. At each stroke as much blood enters the right auricle as issues from the left ventricle ; but the sectional area of the vense cavge is greater than that of the aorta, so that even if the auricle were tilled in exactly the same time as the ventricle is emptied, the blood must pass more rapidly through the nan"ow aorta than through the broad venae cavse, in order that the same quantity of blood should pass each in the same time. The diastole of the auricle, however, is distinctly longer than the systole of the ventricle; the time during which the auricle is being filled is greater than that during which the ventricle is being emptied, and hence the velocity of the venous flow into the auricle must be still less than that of the arterial blood in the commencinof aorta. The temporary variations of the velocity of the stream in any given channel, and these we have already (p. 127) seen to be very considerable in the case of the arteries at least, are dependent on a variety of circumstances. In a tube of constant calibre, the velo- city with which fluid flows from one point to another, for instance from the point a to the point h, will be in main dejiendent on the difierence between the pressures existing at a and h. The loAver the pressure at h as compared with a the gi-eater the rapidity with which the fluid flows from a to h. And temporary variations of pressures form undoubtedly the main cause of the temporarj^ varia- tions observable in the velocity of the arterial flow. Thus with each systole of the ventricle there is an increase of velocity in the whole arterial flow folloAved by a diminution during the diastole. So also if the peripheral resistance in the minute arteries into which a larger artery divides be suddenly lowered (by the action of vaso-motor nerves, in a manner which we shall presently discuss), without tlie calibre of the larger artery itself being changed, the pressure on the distal (peripheral) side of the artery may be much 134 VARIATIONS IN VELOCITY. [Book i. diminished, while the pressure on the proximal (cardiac) side re- mains at first unaltered ; and this would necessarily cause an increase in the rapidity of the stream through that artery. But, as we shall see later on, from the complications of the vascular machinery such problems as these become very intricate; and the results of observations on variations in arterial velocity are not altogether intelligible. It has been suggested that varying conditions of the blood, by affecting the amount of adhesion between the blood and the walls of the vessels, may be an important factor in determining the variations in the velocity of the stream. SEC. 2. THE HEART. The heart is a pump, the motive power of which is supplied by the contraction of its muscular fibres. Its action consequently presents problems which are partly mechanical, and partly vital. Regarded as a pump, its effects are determined by the frequency of the beats, by the force of each beat, by the character of each beat — whether, for instance, slow and lingering, or sudden and sharp — and by the quantity of fluid ejected at each beat. Hence, with a given frequency, force, and character of beat, and a given quantity ejected at each beat, the problems which have to be dealt with are for the most part mechanical. The vital problems are chiefly con- nected with the causes which determine the frequency, force, and character of the beat. The quantity ejected at each beat is governed more by the state of the rest of the body, than by that of the heart itself Tlie Phenomena of the Normal Beat. The visible movements. When the chest of a mammal is opened and artificial respiration kept up, a complete beat of the whole heart, or cardiac cycle, may be observed to take place tus follows. The great veins, inferior and superior vense cavse and pulmonary veins, are seen, while full of blood, to contract in the neighbourhood of the heart: the contraction runs in a peristaltic wave towards the auricles, increasing in intensity as it goes. Anived at the auricles, which are then full of blood, the wave suddenly spreads, at a rate too rapid to be fairly judged by the eye, over the whole of those organs, which accordingly contract with a sudden sharp systole. In the systole, the walls of tlie auricles press towards the auriculo- 136 MOVEMENTS OF THE HEART. [Book i. ventricular orifices, and the auricular appendages are drawn inwards, becoming smaller and paler. During the auricular systole, the ven- tricles may be seen to become more and more turgid. Then follows, as it were immediately, the ventricular systole, during which the ventricles become more conical. Held between the fingers they are felt to become tense and hard. As the systole progresses, the aorta and pulmonary arteries expand and elongate, and the heart twists slightly on its long axis, moving from the left and behind towards the front and right so that more of the left ventricle becomes dis- played. As the systole gives way to the succeeding pause or diastole, the ventricles resume their previous form, the aorta and pulmonary artery contract and shorten, the heart turns back to- wards the left, and thus the cycle is completed. A more exact determination of the changes in the form and position of the heart during a beat is attended with considerable difficulties. The following experiment has been made with the view of studying these changes without opening the chest and thus without depriving the heart of its natural supports. If, in the un- opened chest of a rabbit or dog, three needles be inserted through the chest-wall so that their points are plunged into the substance of the ventricle, one (B) at the base, close to the auricles, another (A) through the apex, and a third (M) at about the middle of the ventricle, all three needles will be observed to move at each beat of the heart. The head of B wdll move suddenly upwards, shewing that the point of the needle plunged in the ventricle moves down- wards, whereas A will only quiver, and move neither distinctly up- wards nor downwards. M wall move upwards (and therefore its point dowTiwards), but not to the same extent as B. The nearer to B, M is, the more it moves : the nearer to A, the less. After the death of the animal, the needles, if properly inserted at first, perpendicular to the chest, will be found with all their heads directed downwards, indicating that the Avhole ventricle has been drawn up by the contraction of the empty aorta and pulmonary artery. The behaviour of the needles during the beat has been in- terpreted as follows. At the systole the whole heart is thrust downward by the elongation of the aorta and pulmonary artery. The needle A at the apex however does not move its place, because this downward movement is compensated by an upward movement due to a shortening, during systole, of the longitudinal diameter of the ventricle. The base in which the needle B is plunged, moves downwards and draws closer to A, i. e. to the apex, partly by the downward thrust from the elongation of the great arteries and partly fi^om the shortening of the ventricle itself. Naturally the behaviour of the needle M is intermediate in character, its downward movement being the more conspicuous the nearer it is to B, The experiment then is taken to prove that during the systole the ventricle shortens in its riiAP. IV.] THE VAsrrLAi: mhciiamsm. 1:57 longitudiiiiil diameter, but that tlie apex ri'inains statifjuary on account of the compensating downward thrust of the whtjle ventricle. It has been urged however that this method is untrust- worthy, and that simihxr movements of needles thus placed might be produced by the twisting of the heait on its l«jng axis, com- bined with an a])j)r<)ximation of the heart to the chest-wall. And tlitierent cunclusions have been arrived at by taking ]ila.ster of Paris models on the one hand of a dog's heart, which, while having ceased beating but not yet become rigid, has been filled with blood at a moderate pressure, and on the other hand of a heart of the same size in which a condition simulating systolic contraction has been brought about by immersing the empty heart in a saturated solution of ]i()tassium bichromate at 50" C The former is taken to represent the diastolic and the latter the systolic form of the heart; and the results are checked by measurements taken between marks placed on various points of the surface of the heart as well as by sections of a heart filled wdth blood and hardened in a cold solu- tion of potassium bichromate and of one emptied and hardened in the same solution warmed to 50^ A comparison of the two hearts in these ditierent conditions tends to shew that while both the right-to-left and autero-posterior diameters are diminished during systole, especially in the plane of the ostia venosa (whereby the auriculo-ventricular orifices become narrowed) the longitudinal diameter, at all events of the left ventricle, is not lessened, the distance between the apex and the auriculo-ventricular groove remaining unchanged. The right ventricle, the change of form of which is complicated, does shorten to a certain extent, and there is during systole a downward movement of the conus arteriosus upon the plane of the ventricular base (which possibly may explain the movement of the needle B in the above mentioned experiment) so that the distance between the apex and the u])per border of the conus is less duiing systole than during diastole. This method also confirms the view" that the left ventricle in systole turns on its long axis, towards the right, the movement increasing from the base downwards so that the groove between the two ventricles forms a closer spiral than during diastole. Objections may be brought against this method also, and it seems impossible to explain the movements of a lever placed upon the heart unless wo admit that during systole, the antero-posterior diameter, of the middle portion of the ventricle at least is increased instead of lessened. We may however probably go so far as to conclude that as far as the ventricles are concerned tTie chief change during systole is one from a roughly hemispherical to a more conical form, effected without any marked diminution of the distance between the apex and the ventricular base. Cardiac Impulse. If the hand be placed on the chest, a shock or impulse will be felt at each beat, and on examination 138 CARDIAC IMPULSE. [Book t. this impulse, 'cardiac impulse,' will be found to be synchronous with the systole of the ventricle. In man, the cardiac impulse may be most distinctly felt in the fifth costal interspace, about an inch below and a little to the median side of the left nipple. The same impulse may be felt in an animal by making an incision through the diaphragm from the abdomen, and placing the finger between the chest-wall and the apex. It then can be distinctly recognized as the result of the hardening of the ventricle during the systole. And the impulse which is felt on the outside of the chest is the same hardening of the stationary portion of the ventricle in contact with the chest- wall, transmitted through the chest- wall to the finger. In its flaccid state, during diastole, the apex is (in a standing position at least) at this point in contact with the chest- wall, Ijang between it and the tolerably resistant diaphragm. During the systole, while being brought even closer to the chest- wall, by the movement to the front and to the right of which we have already spoken, it suddenly grows tense and hard. The ventricles, in executing their systole, have to contract against resistance. They have to produce within their cavities, tensions greater than those in the aorta and pulmonary arteries, respectivel}^ This is, in fact, the object of the systole. Hence, during the swift systole, the ventricular portion of the heart becomes suddenly tense, just as a bladder full of fluid would become tense and hard when forcibly squeezed. The sudden onset of this hardness gives an impulse or shock both to the chest- wall and to the diaphragm, which may be felt readily both on the chest-wall, and also through the diaphragm when the abdomen is opened, and the finger inserted. If the modification of the sphygmograph (see section on Pulse), called the cardiograph, be placed on the spot where the impulse is felt most strongly, the lever is seen to be raised during the systole of the ventricles, and to fall again as the systole passes away, very much as if it were placed on the heart directly. A tracing may thus be obtained, of which we shall have to speak more fully immediately. If the button of the lever be placed, not on the exact spot of the impulse, but at a little distance from it, the lever will be depressed during the systole. While at the spot of impulse itself the contact of the ventricle is increased during systole, away from the spot the ventricle retires from the chest-wall (by the diminution of its right-to-left diameter), and hence, by the mediastinal attachments of the peri- cardium, draws the chest-wall after it. Endo-cardiac events. In order to study more fully the changes going on in the heart during the cardiac cycle, it becomes necessary to know something of what is taking place in the interior of the cavities of the heart. Chauveau and Marey, by introducing into the right auricle and ventricle respectively of the horse, through the jugular vein, small elastic bags, each communicating with a Chat iv. 77//; IM.SVTA.I/; M /:('// A. \/S.]/ 139 recording tambour, were enabled to take simultaneous tracings of changes occurring in the two cavities. These results are embodied in Fig. 21, of which the upper curve is a tracing taken Fig. 21. Simultaneous tracings from the interior of the right Auricle, from THE interior OF THE RIGHT VENTRICLE, AND OF THE CaRDIAC ImPULSE, IN THE HoBSE. (After Chadveau AND Maret.) To be read from left to rights. The upper curve represents changes taking place -within the auricle, the middle curve changes within the ventricle. The lower curve represents the variations of pressure transmitted to a lever outside the chest and constituting the cardiac impulse. A complete cardiac cycle, beginning at the close of the ventricular systole, is comprised between the thick vertical lines I and II. The thin vertical lines represent tenths of a second. The explanation of the letters is given in the text. from the auricle, the middle curve a similar tracing taken from the ventricle, while the lower curve is a cardiographic tracing of the cardiac impulse. All these curves were taken simultaneously on the same recording surface. Method. A tube of appropriate curvature is furnished with two small elastic bags, one at the extreme end and the other at such a distance that when the former is within the cavity of the ventricle the latter is in the cavity of the auricle ; sucli an instrument is spoken of as a ' cardiac sound.' Each bag (Fig. 22 A) or 'ampulla' communicates by a separate air-tight tube with an air-tight tambour (Fig. 22 B) on which a lever rests so that any pressure on either bag is communicated to the cavity of its respective tambour, the lever of which is raised in ' It must be remembered that the curves in the diagram are intended merely to illustrate the changes occurring at different times in the same chamber, or to shew what changes in the one chamber are coincident in point of time with changes in the other. They in no way indicate the amount of pressure exerted in the auricle as compared with that in the ventricla 140 KN DO-GARB I AC EVENTS. [Book i. proportion. The writing points of all three levers are brought to bear on the same recording surface exactly underneath each other. The tube is carefully introduced through the right jugular vein into the right side of the heart until the lower (ventricular) bag is fairly in the Fig. 22. SIabey's Tambouk, with Cardiac Sound. A. A simple cardiac sound such as may be used for exploration of the left ventricle. The portion a of the ampulla at the end is of thin india-rubber, stretched over an open framework with metallic supports above and below. The long tube h serves to introduce it into the cavity which it is desired to explore. B. The Tambour. The metal chamber m is covered in an air-tight manner with the india-rubber c, bearing a tliin metal plate vi to which is attached the lever I moving on the hinge /;. The whole tambour can bo placed by means of the clamp cl at any height on the upright s . The india-rubber tube t serves to connect the interior of the tambour either with the cavity of the ampulla of A or with any other cavity. Supposing that the tube t were connected with b, any pressui'e exerted on a would cause the roof of the tamboar to rise and the point of the lever would be pro- portionately raised. cavity of the right ventricle, and consequently the upper (auricular) bag in the cavity of the right auricle. Changes of pressure on either ampulla then cause movements of the corresponding lever. When the pressure, for instance, on the ampulla in the auricle is increased, the auricular lever is raised and describes on the recording surface an ascending curve ; when the pressure is taken off the curve descends ; and so also with the ventricle. The ' sound ' may in a similar manner be readily introduced through the carotid artery into the left ventricle and the changes taking place in that chamber also explored; these are found to be very similar to those of the right ventricle. We may employ these curves as giving a general and usefiil view of the sequence of events in the interior of the heart; but we must bear in mind exactly what they mean. The tracings given CiiAr. iv.j Till': VASCrLAl; MF.CIIAMSM. \\\ by till' auricuhu" iiud vciitriciihir levi-rs really rcprcsoiit variiilions in the pressure exerted ou the respective uni})ullie, and so far are instructive; but they must not be taken as representing variations in the pressure exerted on the blood in the several cavities. For we can easily conceive that, in the systole of the ventricle for instance, the contraction of the muscular walls might continue after all the blood contained in the ventricle had been driven out. In such a case the ventricle would continue to press upon the ampulla, and this continued pressure would be transmitted to the lever, and indicated on the curve; but we should be in error in interpreting this part of the curve as meaning that the ventricle was still continuing to exert pressure on the blood as yet remain- ing in its cavity. With this caution, and with the remark that the tracing of the cardiac impulse is very unlike the usual cardio- graphic tracings taken from man, we may use the curves to deduce the following conclusions. A complete cardiac cycle is comprised between the vertical lines I and II. The recording surface was travelling at such a rate that the intervals between any two of the thin vertical lines coiTesponds to one-tenth of a second. Hence in this case (the heart being that of a horse) the whole cardiac cycle occupied about f§ths of a second. Any point in the cycle might of course be taken as its commencement. In the figure, the cycle is supposed to begin shortly after the end of the ventricular systole, and the beginning of the diastole. On examining the three curves we see, at a, a steady rise of the auricular, accompanied by similar gradual ascents of the ventricular and also of the cardiograph lever. These may be interpreted as indicating that the blood is pouring from the great veins into the auricle, increasing the pressure there, and at the same time passing on into the ventricle, increasing the internal pressure there as well, a, and also by distending the ventricle, causing it to press somewhat on the chest-wall and thus to raise the cardiograph lever, a". This continues for about j*gths of a second, and is then followed by the sudden rise of auricular pressure h due to the auricular systole, followed by a sudden fall as the blood escapes into the ventricle and the systole ceases. The sudden entrance of blood into the ventricle causes a sudden increase of the pressure in the ventricle as indicated by the ventricular lever h', and a sudden increase in the pressure on the chest-wall h". The auricular systole is followed immediately by the sudden strong ventricular systole c', the lever rising very abruptly. Owing to the presence of the tricuspid valves, the pressure exerted by the ventricular systole is kept off the auricle almost altogether; but the chest-wall, as shewn by the tracing at c", feels the sudden increase of the pressure of the ventricle against it. The most important points concerning this rise of ventricular pressure are that it is sudden in its onset and also rapid in its decline, and 14-2 THE If EC II A y ISM OF THE VALVES. f Boo re i. that it lasts for a comparatively long time; in the figure this part of the curve embraces more than four-tenths of a second. These features, the sudden rise, the long duration, and the rapid fall of the pressure exerted by the ventricle are seen in all tracings of the ventricles engaged in a cardiac beat whatever be the method employed. They mean of course that the muscular contractions which constitute the ventricular systole come on suddenly, that they last altogether a considerable time, and that relaxation is also rapid. With the end of the ventricular systole the cycle represented in figure ends, and a new cycle begins, repeating the same changes. The meaning of the features on the curves marked e and d, &c., as well as a more complete discussion of the changes thus briefly described, we must defer till we have spoken of The Mechanism of the Valves. The auriculo-ventricular valves present no difficulty. As the blood is being driven by the auricular systole into the ventricle, a reflux current is probably set up, by which the blood, passing along the sides of the ventricle, gets between them and the flaps of the valve (whether tricuspid or mitral). As the pressure of the auricular systole diminishes, the same reflux current floats the flaps up, until at or immediately after the close of the systole they meet, and thus the oriflce is at once and firmly closed, at the very beginning of the ventricular beat. The increasing intraventricular pressure serves only to render the valve more and more tense, and in consequence more secure, the chordae tendinese (the slackening of which through the change of form of the ventricle is probably obviated by a regulative contraction of the papillary muscles) at the same time preventing the valve from being inverted or even bulging into the auricle, and indeed, according to some observers, keeping the valvular sheet actually convex to the ventricular cavity, by which means the complete emptying of the ventricle is more fully effected. Since the same papillary muscle is in many cases connected by chordye with the adjacent edges of two flaps, its contraction also serves to keep these flaps in more complete apposition. Moreover the extreme borders of the valves, outside the attachments of the chordse, are excessively thin, so that when the valve is closed, these thin portions are pressed flat together back to back ; hence while the tougher central parts of the valves bear the force of the ventricular systole, the opposed thin membranous edges, pressed together by the blood, more completely secure the closure of the orifice. CiiAi'. iv.j Tin: VAsccLMi Mi':('iiAxis.]r. 113 The semilunar valves are, durint^'tlic ventricular systole, pressed outwards towards but not close to the arterial walls, reflex currents probably keepinrj them in an intermediate position, their orifice formiufif an eijuilateral triangle with cun-ed sides ; they thus offer little obstacle to the escape of blood from the cavities of the ventricles. The ventricle propels the blood with great force and rapidity into the aorta and the whole contents arc s})eedily ejected. ISow, when in a closed channel a rapid cun-ent suddenly ceases, a negative pressure makes its appearance in the rear of the fluid, and sets up a reflux cuiTent. So when the last portions of blood leave the ventricle a negative pressure makes its appearance behind them in the ventricle, and leads to a reflux current from the aorta towards the ventricle. This alone would tend to bring the valves together; but in all probability it is not till a short (variable) time afterwards, that upon the commencing diastolic relaxation of the ventricle, the elastic rebound of the arterial walls completely fills and renders tense the pockets, causing their fi-ee margins to come into close and firm contact, and thus entirely blocking the way. The corpora Arantii meet in the centre, and the thin membranous festoons or lunulse are brought into exact apposi- tion. As in the tricuspid valves, so here, while the pressure of the blood is borne by the tougher bodies of the several valves, each two thin adjacent lunulse, pressed together by the blood acting on both sides of them, are kept in complete contact, without any strain being put upon them ; in this way the orifice is closed in a most efficient manner. The ingenious view put forward by Briicke that during the ven- tricular systole, the flaps are pressed back flat against the arterial walls, and in the case of the aorta completely cover up the orifices of the coronary arteries, so that the flow of blood from the aorta into the coronary arteries can take place only during the ventricular diastole or at the very beginning of the systole, and not at all during the systole itself, has been disproved. Tlie Sounds of the Heart. When the ear is applied to the chest, either directly or by means of a stethoscope, two sounds are heard, the first a com- paratively long dull booming sound, the second a short sharp sudden one. Between the first and second sounds, the internal of time is very short, too short to be measurable, but between the second and the succeeding first sound there is a distinct pause. The sounds have been likened to the pronunciation of the syllables, lubb, dup, so that the cardiac cycle, as far as the sounds arc concerned, might be represented by : — lubb, du]\ pause. 144 THE SOUNDS OF THE HEART. [Book r. The second short sharp sound presents no difficulties. It is coincident in point of time with the closure of the semilunar valves, and is heard to the best advantage over the second right costal cartilage close to its junction with the sternum, i. e. at the point where the aortic arch comes nearest to the surface. Its characters are such as would belong to a sound generated by the sudden tension of valves like the semilunar valves. It is obscured and altered, replaced by ' murmurs ' when the semilunar valves are affected by disease, the alteration being most manifest to the ear at the above-mentioned spot when the aortic valves are affected. When the aortic valves are hooked up by means of a wire intro- duced down the arteries, the second sound is obliterated and replaced by a murmur. These facts prove that the second sound is due to the sudden tension of the aortic (and pulmonary) semi- lunar valves. The first sound, longer, duller, and of a more ' booming ' character than the second, heard with greatest distinctness at the spot where the cardiac impulse is felt, presents many difficulties in the way of a complete explanation. It is heard distinctly when the chest-walls are removed. The cardiac impulse therefore can have little or nothing to do with it. In point of time, and in the position in which it may be heard to the gi'eatest advantage (at the spot of the cardiac impulse where the ventricles come nearest to the surface), it corresponds to the closure of the auriculo-ven- tricular valves. In point of character it is not such a sound as one would expect from the vibration of membranous structures, but has, on the contrary, many of the characters of a muscular sound. In favour of its being a valvular sound, may be urged the fact that it is obscured, altered, replaced by murmurs, when the tricuspid or mitral valves are diseased ; and according to some authors clamp- ing the great veins so as to shut off the blood supply stops the sound though the beat continues. The first argument may be met by the consideration that a murmur though itself undoubtedly of valvular origin, might largely or completely hide a sound occurring at the same time as the closure of the valves but due to other causes ; and the second is directly contradicted by an experiment of Ludwig and Dogiel. These observers tied in succession, in the order of the flow of blood, the great veins and arteries of the heart of a dog so as to completely deprive the heart of blood, and listened to the heart both within the body and after removal. For the short time that the heart continued to beat, the first sound was heard, feeble but with its main characters recognisable. From this they inferred that the sound was of muscular origin. But there is a great difficulty in regarding the sound as a muscular one, for a muscular sound is the result of a tetanic contraction, the height of the note produced varying with the rate of re- petition of the simple contractions which go to make up the Chat. IV.] TlIK VAScri.Ml Ml-CIf.WfS.V. 145 tetanus, A simple contraction or spasm cannot possibly produce a sound liaviiif^ tlic cluiractcrs of the iirst cardiac sound. And tho evidence, tliougli perlia|)s not conclusive, fjoes to shew that the beat of the heart is a slow long-continued single sjjasm, interracdiato between the contraction of an ordinary striated and that of an unstriated muscle, and not a tetanic contraction. We cannot, it is true, now rely in support of this view on the fact that when the nerve of a rheoscopic muscle-nerve pi-ejiaration is placed on the beating ventricle, each beat is followed by a single spasm of the muscle, and not by a tetanus ; for we now know that many forms of tetanus {o.rj. those caused by the constant current, by strychnia, and probably all natural voluntary contractions) give rise, in a rheoscopic muscle-nerve preparation, to a single initial spasm and not to a tetanus. But the general features of the beat, its long latent period and the gradation of the ventricular systole through the auricular systole into the rhythmic contractions of the un- striated fibres of the Avails of the great veins, render it difficult to suppose that the beat is really a tetanus. Moreover the long duration of the ventricular systole is readily explained by the wave of contraction passing in a complicated peristaltic manner over the different fibres in succession. But if the beat be a simple contraction, it cannot give rise to a muscular sound, unless we suppose that this sequence of simple contractions over various parts of the ventricle in succession is adequate to produce such a sound. This, however, does not seem very satisfactory. On the other hand, if we reject the distinctly muscular origin of the sound, we are almost driven to suppose that the abnipt systole is able even in the absence of blood to produce such a sudden tension of the valves, and of the ventricular v.-alls, as to give rise to a note. On such a view, the sound ought to vary in character according as the ventricle is more or less filled, beinsr low and booming when it is full, and high and sharp v.dien the contents are scanty. And such is said to be the case. But the matter does not at present seem ripe for any dogmatic statement. In the normal state of things, the beats of the two ventricles are so far synchronous with each other that practically onh^ one first sound and one second sound is heard. It sometimes happens hov/ever that the synchronism fails to such an extent and the closure of the pulmonary and aortic valves respectively are sej^a- rated by such an interval as to give the second sound a double character. 10 146 SPECIAL CARDIAC PHASES. [Book i. On the relative duration and special characters of the Cardiac events. We may now return to a more detailed study of what is taking place in the heart during a beat. We have already spoken of the conclusions which may be drawn from Chauveau and Marey's curves, and have incidentally (p. 138) referred to the cardiograph. Various forms of cardiograph have been used to record the cardiac impulse. In some the pressure of the impulse as in the sphygmograph is transmitted directly to a lever which writes upon Fia. 23. Caediogeaphic tbacing of Caeduc Impulse in Man (from Landois). An entire beat occurs between a and /. Tbe auricular systole is marked by 6, the end of tbe Tentricular relaxation by/. At c, the highest point of the curve, the blood begins to be propelled from the ventricle, d and e are considered by some to indicate the closure of the aortic and semilunar valves respectively, see text. Five cardiac beats are represented ; the convex curve which their base line forms is due to the respiratory movements. a travelling surface. In others the impulse is, by means of an ivory button, brought to bear on an air-chamber, connected by a tube with a tambour as in Fig. 22 ; the pressure of the cardiac impulse compresses the air in the air-chamber, and through this the air in the chamber of the tambour by which the lever is raised. In such delicate and complicated movements as those of the heart however, the use of long tubes filled with air is liable to introduce various errors. A cardiographic tracing of ordinary characters is given in Fig. 23. Curves of the variations in internal pressure may be obtained by passing a tube connected with a mercurial manometer (as in the investigation of arterial pressure, p. 122) into the right ventricle through the jugular vein or into the left ventricle through the carotid artery. But this method, though useful for the purpose of investigating generally the pressure exerted by the cardiac walls, is, by reason of the inertia of the mercury, unsuitable for detecting rapid and small changes. Chap, iv.] 77/ /; I 'A SC UL A R M ECU . I \ IS .1/. HT Tracings of the movements of the ventricles themselves, coitc- sponding to the cardiac impulse and so to a certain extent to the variations of internal pressure, may also be taken directly by bringing a light lever to bear on the outside of the ventricles, the chest having been previously opened and artificial respiration kept up. A cune* taken bv this method is shewn in Fig. 24. id &, jh la Fig. 24. Normal heart curve shewing changes in the antero-posterior diameter of the ventricle obtained from the cat by a light recording lever moved by a button which pressed gently on the anterior surface of the ventricle. The time curve gives 50 double vibrations per sec. and lines have been drawn to shew the duration of the different phases of the ventricular movement, a to 6 corresi;onds to the distension of the ventricle including the auricular systole, the wave-like rise during this period being due to the increase in the diameter of the ventricle resulting from the entrance into it of the contents of the auricle. The period from 6 to c corresponds to the time from the commencement of the ventricular contraction to the moment when the or^'an has completed its change in shape from a flattened to a more rounded form. The highest part of the cur^'e corresponds also in time with the opening of the semilunar valves as well as the firm closure of the auriculo-ventr!cular valves. The duration of this ^ The majority of cardiographic, sphygmographic and other tracings shew certain points which can be understood at a glance, but many characteristics can only be learned by "measuring out the curve" as it is termed. This is done as foUows. Every tracing ought to bear on it an abscissa line, marked by a point which remains motionless while the recording surface is travelling. Moreover, either before or after taking a curve, while the paper or recording surface is at rest, the point of the lever should be always moved up and down so as to describe a segment of a circle of which the axis of the lever is the centre. The tracing thus prepared, when it has to be measured, is pinned out on aboard, and, by means of a pair of compasses, the distance between whose points has previously been made equal to the distance between the axis and the point of the lever used in making the experiment, the centre of the circle of which the curved lines previously made as directed are segments is found and marked on the paper. Through this centre, which of course corresponds to the position of the axis of the lever, a horizontal line is drawn parallel to the abscissa line. Keeping one of the compass points on this line, segments of circles are drawn in succession through various points of the cnr^-e, the distance between the points of the compass being fixed, but the centre of the circle described being shifted backwards and forwards along the horizontal line. The points where these segments cut the horizontal line are marked upon it, and the distances between them measured as, for example, in Fig. 29, p. 166. If the curve of a tuning-fork, the point of whose recording style was carefully placed on the same vertical line as the point of the lever, be also present, the segments of circles may be continued until they cut this, and the time corresponding to distances between them (as, for instance, in Fig. 24 the intervals between a. h. c, rf,) thus directly mep.=nred off. 10—3 148 SPECIAL CARDIAC PHASES. [Book i. period in this case is only about 3-50tlis of a sec. The period from c to tf is that during which the ventricle having grasped its contents is emptying its cavity and remaining contracted. It can be seen that only during the first half of this period is there any marked descent of the lever point ; in other words the antero-posterior diameter does not continue to diminish during the whole period of the systole, indicating that little or no blood was thrown out during the second half of this period, the ventricle remaining simply contracted after having emptied its cavity. The period from ci to a is that during which the ventricular muscle is relaxing. Here, as is frequently the case, there is no period of pause between the close of the relaxation of the ventricle and the commencement of the succeeding distension. The tracing gives no evidence as to the time of closure of the semilunar valves. The chief mterest and the chief difficulties are attached to the systole of the ventricles. In order to understand this, the most important of the cardiac events, it must be borne in mind that, as we have already seen, the pressure of the blood in the aorta is always considerable. This pressure closes and keeps closed the semilunar valves ; and it is not till the pressure in the ventricle becomes greater than the pressure in the aorta that these valves open to allow of the escape of the ventricular contents. The blood therefore does not begin to pass from the left ventricle into the aorta until some time, and that a variable time, after the commence- ment of the systole of the ventricle ; and the same may be said of the right ventricle and pulmonary artery, it being understood that the arterial pressure on the right side is less than on the left. In Fig. 24 the ventricular lever reaches its maximum c at once^ gradually declining afterwards till the more sudden fall begins, and we may suppose that the escape of blood from the ventricle begins at the moment when the maximum is attained; and this view is confirmed by carefully comparing a tracing of the expansion of an artery with the cardiac tracing. It is quite possible however to conceive that owing to circumstances, such as an increasing con- traction of the ventricular fibres or deficient expansion of the arteries, the pressure might continue to increase even after blood was escaping from the cavity of the ventricle. And indeed in some curves, the ventricular lever after the first sudden leap continues to rise gradually and does not reach the maximum point until afterwards. In such cases the summit of the first rise must be taken as marking the beginning of the flow from the ventricle. By the sudden systole the blood is ejected with considerable force and rapidity from the ventricle, and as the ventricle becomes empty a negative pressure, as we have seen, makes its appearance behind the column of blood which leaves the cavity and leads to the closure of the semilunar valves. Much dispute has taken place as to the exact condition of the ventricle at the moment of closure of the semilunar valves. The slight rise e in Chauveau and Marey's curves (Fig. 21) in the ventricular curve, seen also in the auricle at e and in the cardiac impulse at e", and which has been taken to indicate the shutting of the semilunar valves, appears quite at the close of the descent of the ventricular lever. This would mean that at the moment of the closure of the valves the ventricle Chap, iv] THE VASCULAR MI-ClIAXISSf. 149 hatl not only completed its contraction but was far advanced in relaxation. Such a view is not only d pi^iori improbable but i.s directly contradicted by the fact that when we compare a tracing obtained by ])laeing a lever directly on the heart or indeed a tracing of the cardiac impulse with a pulse tracing, that is a tracing of the expansion of an artery, we find that the ventricle continues con- tracted after its contents have entirely k-ft the cavity. That is to say, the actual How of blood takes place only during the middle portion of the time during which the muscular fibres of the ven- tricle are contracting and engaged in carry ino- on the systole. During the first part, pressure is being got up, during the second the blood is being propelled, during the third the ventricle continues to remain empty and contracted. By this means the complete emptying of the ventricle is eftectually secured. And others have urged that the closure of the semilunar valves, being entirely due to the reflux spoken of above, follows close upon the emptjing of the ventricle ; in other words that it takes place while the ven- tricle is still contracted. It is very difficult to point out indications on the ventricular cur\-e which indubitably coiTespond to this event. In tracings of the cardiac impulse, and in tracings taken by a lever placed directly on the heart, a notch, followed by a rise, is some- times observed in that part of the curv^e which intervenes between the first large rise and the final sudden fall ; and this secondary rise has been taken to indicate the closure of the semilunar valves; but, if this be the case, the time during which the ventricle remains contracted after the closure of the valves forms a very con- siderable fraction of the whole period of the systole ; and this presents difficulties. Sometimes two such notches and peaks are seen, and the occurrence of the two has been attributed to a want of sjTichronism in the closure of the pulmonar}' and aortic semilunar valves, the latter closing some little time before the former. But it is by no means clear that these notches and peaks are thus due to the closure of the valves ; they may possibly have another origin, they are not always present, and the attempt to fix the time of the closure of the semilunar valves by them cannot be regarded as satisfactory. On the other hand, the second sound of the heart is undoubtedly due to the complete closure and sudden tension of the semilunar valves ; and not only is this second sound separated from the first sound by a distinctly appreciable interval (from which we may infer either that the systole of the ventricle ceases before the complete closure and sudden tension of the semilunar valves or that the first sound does not last so long as the systole itself and is therefore not a muscular sound) but the time elapsing between the beginning of the first sound and the second sound is, as we shall see, remarkably constant. Now we have reason to believe that the quantity of blood expelled at any one beat, and hence the time taken up in its escape, does vary very considerably ; whereas the duration of the actual systole is probably much more constant. 11)0 ENDO-CAEDIAC PRESSUBE. [Book i. Hence we may infer, and the conclusion may be supported by other arguments, that at the actual closure of the semilunar valves, giving rise to the second sound, the ventricle has just finished its systole and is beginning to relax. If this view be correct the time of the closure of the valves is not indicated on the cardiographic tracing by any special mark, but coincides with the commencement of the more sudden and final fall of the lever as at d in Fig. 24. Marey thought that the oscillations seen at cV in his curves and obvious in the auricle and cardiac impulse as well, were due to oscillations of the auriculo-ventricular valve, but in that case they would be inverted in the auricular curve ; whereas they are not. It is difiicult to say what gives rise to them. "We may repeat that many of the details of these curves vary considerably even with the same method of investigation and when the same apparatus is employed. In all probability the character and sequence of the events are modified by various circumstances, such as the rate and rapidity of the beat, the qua,ntity of blood flowing into the heart, and the pressure obtaining in the arteries. Amount of Pressure. Although the instrument of Chauveau and Marey may be experimentally graduated and has been used to measure the amount of pressure in the several cavities of the heart, it is, as we have said, open to objections. Better results may be gained bypassing through the jugular vein into the right auricle and thence into the right ventricle, or through the carotid artery into the left ventricle, a tube open at the end introduced into the heart and connected at the other end with a manometer. Varia- tions of pressure in the cardiac cavities are thus transmitted di- rectly to the mercury column of the manometer in the same way as those of an artery when arterial pressure is measured. The inertia of the mercury column however prevents an exact response to the rapid movements of the heart, and obscures the results ; though by using maximum and minimum manometers, the maximum and minimum pressures of the several cavities may be determined. The prmciple o£ the maximum manometer, Fig. 25, consists in the introduction into the tube leading from the heart to the mercury column, of a (modified cup-and-ball) valve, opening, like the aortic semilunar valves, easily from tlie heart, but closing firmly when fluid attempts to return to the heart. By reversing the direction of the valve, the manometer is converted from a maximum into a minimum instrument. When an ordinary manometer is connected with a ven- tricular cavity, the movements of the mercury do not follow exactly the rapid variations of pressure of the cavity, and the height of the column fails to indicate both the highest and the lowest pressures. In this way in the dog a maximum pressure has been observed ■ in the left ventricle of about 140 mm. (mercury), in the right ventricle of about 60 mm. and in the right auricle of about 20 mm. Chap, iv] 77/ A' VASCULAR MECHANISM. 161 Marey luul ])reviously, by means of his own instrument, determined the pressure in the liorse to bo in tlie left ventricle about 150 rnm., in the riii^lit ventricle only about *iO mm., while that of the right auricle he estiniatiMl at not more than a IVw mm. Fig. 25. The Maximum Manometer of Goltz and Gaule. At c a connection is made with the tube leading to the heart. When the screw damp k is closed, the valve v comes into action, and the instrument, in the position of the valve shewn in the figure, is a maximum manometer. By reversing the direction of v it is converted into a minimum manometer. When k is 02:)ened, the variations of pressure are conveyed along a, and the instrument then acts like an orcUuary manometer. It is interesting to observe that the minimum pressure may fall below that of the atmosphere : thus in the left ventricle (of the dog) a minimum pressure varying from — 52 to — 20 mm. may be reached, the minimum of the right ventricle being from — 17 to — 16 mm., and of the right auricle from — 12 to — 7 mm.^ Part of this diminution of pressure in the cardiac cavities may be due, as will be explained in a later part of this work, to the aspiration of the thorax in the resj)iratory movements. But even when the thorax is opened, and artificial respiration kept up, under which circumstances no such aspiration takes place, the pressure in the left ventricle may still sink as low as — 2-i mm. The minimum ma- nometer, which shews most distinctly the existence of this negative pressure, obviously gives no information as to the exact phase of the beat in which it occurs ; and there is some difference of opinion as to the exact time at which it takes place. Goltz and Gaule, to ^ These numbers are to be considered merely as instances which have been observed, and not as averages drawn from a large number of cases. 152 DURATION OF THE CARDIAC PHASES. [Book i. \vliom "we are indebted for the maximum and minimum manometer, l)elieved that the negative pressure appeared at the beginning of the diastole and indeed that it was caused by the expansion of the ventricle. Were this the case, the ventricle might be regarded not only as a force pumj) driving blood into the arteries, but also as a suction pump drawing blood from the auricles and great veins. Others however find great difficulties in supposing that the ventricular walls can, either by virtue of the elasticity of their fibres, or by the contraction of special dilating fibres, or by becoming suddenly injected with blood through the coronary arteries, actually expand so as to exert any such suction power. And they maintain that the negative pressure seen in the ventricle is merely that same negative pressure due to the sudden emptying of the ventricle which we have already described as serving to close the semilunar valves. When the minimum manometer is used, the lowest limit of negative pressure is not reached until after several beats, indicating that its duration in any single beat must be very brief The negative pressure due simply to the cessation of the flow is in fact almost immediately made away with by the ventricular walls, in theu' continued contraction coming into com- plete contact ; it passes off therefore before any blood can enter into the ventricle from the auricle, and hence can exert no suction power. Admitting this, however, it is still open for us to suppose that after this negative pressure has passed away, a second negative pressure is caused by the expansion of the ventricle in diastole ; and that this, though also brief, does exert a suction power. And indeed the view that the ventricle in expanding can produce such a negative pressure is one which cannot as yet be regarded as definitely disproved. The dnration of the several phases. The time-measurements given in Fig. 21 afford a general idea of the relative duration of the several events in the slowly beating heart of the horse. Thus it is obvious that the longest phase (viz. about yq sec.) is that occurring between the end of the ventricular systole at e to the beginning of the auricular systole at h ; this is often spoken of as the diastole, or as the "passive interval," since during this time both auricles and ventricles are in diastole. The next longest phase is the systole of the ventricles (viz. rather more than -^^ sec), and the shortest (viz. rather less than j^^ sec.) is the systole of the auricles. When we desire to arrive at more complete measurements, we are obliged to make use of calculations based on various data ; and these give only approximate results. Naturally the most interest is attached to the duration of events in the human heart. The datum which perhaps has been most largely used is th3 interval between the beginning of the first and the occurrence of the second sound. This may be determined with approximative correctness, and according to Donders varies from "301 to '327 sec, C'liAi'. iv] TIIK VASCULAR MECHANISM. 153 occupying from 40 to 46 p. c. of the whole period; and being fairly constant for different rates of heart-beat. The observer, listening to the sounds of the heart, made a signal at each event on a recording surface, the diflference in time between tlie marks being measured by means of tlie vibrations of a tuning fork recorded on the same surface. By practice it was found possible to reduce the errors of observation within very small limits. Now whatever be the exact causation of the first sound, it is undoubtedly coincident with the systole of the ventricles, though possibly the actual commencement of its becoming audible may be slightly behind the actual beginning of the muscular con- tractions. Similarly the occurrence of the second sound due to the closure of the semilunar valves may, as we have seen, be taken to mark the close of the ventricular systole. And thus the inten-al between the beginning of the first and the occurrence of the second sound has been regarded as indicating approximatively the duration of the ventricular systole, i.e. the period during which the ventri- cular fibres are contracting. If however we accept the \dew that the ventricle still remains contracted for a brief period after the valves are shut, then the second sound does not mark the end of the systole, and the duration of the systole is rather longer than the "3 sec. given above. The propulsion of the blood into the aorta leads to an expansion of the aorta walls, known as the pulse, which we shall study more fully immediately. This pulse travels, as we shall see, along the arteries at a certain rate : it is later at arterial points more distant from the heart than at points nearer the heart. We can calculate with approximative coiTectness the time it takes for the expansion to travel from the aortic valves to the radial artery at the wrist, for example. Now when we record, as we may do on the same recording surface, the exact moment at which the first sound begins, or at which the lever of the cardiograph begins to rise in the ventricular systole, and also the exact moment at which the expansion of the corresponding pulse at the wrist begins, and measure the interval of time between them, we find that the interval is greater than is required for the expansion of the pulse-wave to travel from the heart to the wrist. The difference gives the measure of the time during which the ventricle by its contraction is getting up an adequate pressure upon its contents, and during which, as yet, blood has not escaped from the ventricular cavity and begun to ex- pand the aorta : the measure in fact of what we called, a little while ago, the first period of the ventricular systole. This may also be estimated by directly measuring the time taken up by the upstroke of the cardiographic tracing, and has been said to be on an average about '085 sec. These measurements however are approximative only and there can be no doubt that the time varies very largely, being dependent on the quantity of blood in the ventricle, on the blood-pressure in the aorta and on the condition of the heart. 154 DURATION OF THE CATtDIAC PHASES. [Book i. During the expansion of the artery and probahly for some httle time beyond, viz. up to the occurrence of what in speaking of the pulse-wave we shall call the dicrotic notch, blood is being propelled from the ventricle. By measuring this time or by deductions from the curve of the cardiac impulse, it has been concluded that the time during which blood is escaping from the ventricle or the duration of the second phase of the ventricular systole, amounts to about 0"1 sec. Deducting these two periods from the total period of 0'3 sec.-j there would be left a period of O'llo sec, marking the third phase of the systole, during which the ventricle, though empty, is con- tinuing its contractions. Upon the view however that the closure of the valves does not mark the end of the systole, this j^hase must be taken as still longer. In a heart beating 72 times a minute, which may be taken as the normal rate, each entire cardiac cycle would last about 0"8 sec, and taking 0"3 sec. as the duration of the systole, the deduction of this would leave 0"5 sec for the whole diastole of the ventricle including its relaxation. At the close of this period, there occurs the systole of the auricles, the exact duration of which it is difficult to determine, it being hard to say when it really begins, but which perhaps may be taken as lasting on an average O'lsec The systole of the ventricle follows so immediately upon that of the auricles, that practically no interval exists between the two events. We may sum up therefore the details of the duration of the more important phases of the cardiac cycle in the following tabular form. sees. sees. Systole of ventricular previous to opening of semilunar valves . O'OSo Escape of blood into aorta . . OlOO i- Continued contraction of the emptied ventricle . . . 0"115j Total systole of the ventricle . . 0'3 Diastole of both auricle and ven- "j tricle or "passive interval" . O'-iOO Y Systole of auricle . . . 0-lOOj Sum of above two, making the diastole of ventricle or "pause" between second and first sound . 0'5 Total Cardiac Cycle .... 08 Or selecting only the important facts out of the -f^ sec. occupying the whole cardiac cycle, f^ sec. or possibly rather more are taken up by the systole, and -f^ sec. or possibly rather less by the diastole of the ventricle. The following diagram may be useful as giving in a graphic form a general idea of the sequence and duration of the seveM ^%c.^^ 'im\"_ f'llAl'. IV.] 77/ A' VASCULAR MECIUy/SAf. 155 cardiac events. It will bo understood of course that the diagram i& intended to sliew merely the ^'eneral relations of" the several events and not to represent exact measurements. Fio. 26. DiAGRAilllATIC EePRESENTATIOX OF THE MOVEMENTS AKD SoUNDS OF TUE Heart during a Cardi.4.c Period. (After Dr Sharpey.) We may repeat that the details given above are at the best approximative only, and, we may add, to a certain extent hypo- thetical. We have given them at such length not on account of their intrinsic importance, or because they are trustworthy data for further calculations, but because the study of them may help the reader in forming a more vivid image in his mind of what is taking place in the heart during a beat. Moreover it must be remembered that the figures quoted are those belonging to what may be considered a normal rate of heart beat. The rate how- ever at which the heart beats varies, as we shall see, under the influence of circumstances, within very wide limits. With regard to the duration of the several phases at different rates of heart beat, the most important fact is perha^js that the pause varies much more than does the systole of the ventricles. A quickly beating heart differs from a slowly beating heart by reason of the pause being shortened, much more than by each systole being of less duration. We may briefly recapitulate the main facts connected with the passage of blood through the heart as follov\s. The right auricle during its diastole, by the relaxation of its muscular fibres, and by the fact that all pressure from the ventricle is removed by the tension of the tricuspid valves, offers but little resistance to the ingress of blood from the veins. On the other hand, the blood in the trunks, of both the superior and inferior vena cava, is under a pressure, which diminishing towards the heart and becoming within 156 DURATION OF THE CARDIAC PHASES. [Book i. the thorax actually negative (as we shall see in speaking of respirations), remains higher than the pressure obtaining in the interior of the auricle; the blood in consequence flows into the empty auricle, its progress in the case of the superior vena cava being assisted by gravity. At each inspiration, this flow is favoured by the increased negative pressure in the heart and great vessels caused by the respiratory movements. Before this flow has gone on very long, the diastole of the ventricle begins, its cavity dilates, the flaps of the tricuspid valve fall back, and blood for some little time flows in an unbroken stream from the venoB cavse into the ventricle. In a short time, however, probably before much blood has had time to enter the ventricle, the auricle is full, and forth- with its sharp sadden systole takes place. Partly by reason of the onward pressure in the veins, which increases rapidly from the heart towards the capillaries, partly from the presence of valves in the venous trunks and at the mouth of the inferior vena cava, but still more from the fact that the systole begins at the great veins themselves and spreads thence over the auricle, the force of the auricular contraction is spent in driving the blood, not back into the veins, but into the ventricle, where the pressure is still ex- ceedingly low. Whether there is any backward flow at all into the great veins or whether by the progressive character of the systole the flow of blood continues, so to speak, to follow up the systole without break so that the stream from the veins into the auricle is really continuous, is at present doubtful ; though a slight positive wave of pressure synchronous with the auricular systole, travelling backward along the great veins has been observed at least in cases where the heart is beating vigorously. The ventricle thus being filled by the auricular systole, the play of the tricuspid valves described above comes into action, the auricular systole is followed by that of the ventricle and the pressure within the ventricle, cut off from the auricle by the tricuspid valves, is brought to bear entirely on the conus arteriosus and the pulmonary semilunar valves. As soon as by the rapidly increasing shortening of the ventricular fibres the pressure within the ventricle becomes greater than that in the pulmonary artery, the semilunar valves open and the still continuing systole discharges the contents of the ventricle into that vessel. As the ventricle thus rapidly and forcibly empties itself, a transient negative pressure makes its appearance in the rear of the ejected column of blood. This in return leads to a reflux of blood towards the ventricle. The first act of this reflux however is, as we have seen, to close the semilunar valves, and even if it be urged that the exit of the ventricular contents does not always end with sufficient abruptness to cause a negative pressure adequate to produce this result, the elastic rebound of the arteries, upon their receiving no fresh blood, has the same effect of closing the semilunar valves, and thus of shutting off the blood in the over- PHAr. IV.] THE VASCrLAR M/XI/A XIS.U. i:.7 distended arteries from the emptied ventricle. Coincidcntly with this closure, the systole as we have seen probably ends and relaxation begins ; then once more the cavity of the ventricle be- comes unfolded and finally distended by the influx of blood from the auricle. During the whole of this time the left side has with still greater cnerg}' been executing the same manoeuvre. At the same time that the vena; cav33 arc tilling the right auricle, the pulmonary- veins are filling the left auricle. At the same time that the right auricle is contracting, the left auricle is contracting too. The systole of the left ventricle is synchronous A\'ith that of the right ventricle, but executed with gi-cater force ; and the flow of blood is guided on the left side by the mitral and aortic valves in the same way that it is on the right by the tricuspid valves and those of the pidmonary artery. The Work done. "We can measure ^^'ith ajDproximativc exactness the intraven- tricular pressure, the length of each sj'stole, and the number of times the systole is repeated in a given period, but perhaps the most important factor of all in the determination of the work of the vascular mechanism, the quantity ejected from the ventricle into the aorta at each systole, cannot be accurately determined ; we are obliged to fall back on calculations having many sources of error. The mean result of these calculations gives about 180 grms. (G oz.) as the quantity of blood which is driven from each ventricle at each systole in a full-groMTi man of average size and weight. It is evident that exactly the same quantity must issue at a beat from each ventricle ; for if the right ventricle at each beat gave out rather less than the left, after a certain number of beats the whole of the blood would be gathered in the systemic circu- lation. Similarly, if the left ventricle gave out less than the right, all the blood would soon be crowded into the lungs. The fact that the pressure in the right ventricle is so much less than that in the left (probably 30 or 40 mm. as compared with 200 mm. of mercury), is due, not to differences in the quantity of blood in the cavities, but to the fact that the peripheral resistance which has to be overcome in the lungs is so much less than that in the rest of the body. Various methods have been adopted for calculating the average amount of blood ejected at each ventricular systole. It has been calculated from the capacity of the recently removed and as yet not rigid ventricle, filled with blood under a pressure equal to the calculated average prcs-sure in the ventricle. This method of cour?;c presupposes 158 THE WORK DONE BY THE HEART. [Book i. that the whole contents of the ventricle are ejected at each systole. Volkmann measured the sectional area of the aorta, and taking an average velocity of the blood in the aorta (a very uncertain datum), calculated the quantity of blood which must pass through the sectional area in a given time. The number of beats in that time then gave him the quantity flowing through the area, and consequently ejected from the heart, at each beat. The mean of many experiments on diflferent animals came out '0025 p. c. of the body weight, which in a man of 75 kilos would be 187'5 grms. Yierordt measured the mean velocity and the sectional area in the carotid, and thence, from a measurement of the sectional area of the aorta, and from a calculation of the blood's mean velocity in it, based on the supposition that the mean velocity in an artery was inversely as its sectional area, arrived at the quantity flowing through the aortic sectional area in a given time, and thus at the quantity passing at each beat. Both these calculations are vitiated by the fact that the variations of velocity in the aorta are so great, that any mean has really but little positive value. rick by means of calculations based partly on the data gained by observing the increase of the volume of the whole arm at each cardiac systole, arrived at results much less than either of the above. In one case he estimated the quantity ejected from the heart at each beat at 53 grm., and in a second case at 77 grm. It must be remembered that though it is of advantage to speak of an average quantity ejected at each stroke, it is more than probable that that quantity may vary within very wide limits. Taking, however, 180 grms. as the quantity, in man, ejected at each stroke at a pressure of 250 mm.^ of mercury, which is equiva- lent to 3'21 metres of blood, this means that the left ventricle is capable at its systole of lifting 180 grms. 3'21 m. high, i. e. it does 578 gram-metres of work at each beat. Supposing the heart to beat 72 times a minute, this Avould give for the day's work of the left ventricle, nearly 60,000 kilogram-metres ; calculating the work of the right ventricle at one-fourth that of the left, the work of the whole heart would amount to 75,000 kilogram-metres, which is just about the amount of work done in the ascent of Snowdon by a tolerably heavy man. A calculation of more practical value is the following. Taking tho quantity of blood as -^^ of the body weight, the blood of a man weighing 75 kilos would be about 5,760 grms. If 180 grms. left the ventricle at each beat, a quantity equivalent to the whole blood would pass through the heart in 32 beats, i.e. in less than half a minute. 1 A high estimate is purijosely taken here. Chap. IV.] THE VASCCLAIi M/CCJ/AX/S.U. 159 Variations in the Heart's heat. These are for the most juirt in reality vital iihcnomena, i.e. brought about by events tk-pcnding on chanrrcs in the vital properties of some or other of the tissues of the body. It will be convenient, however, briefly to review them here, though the discussion of their causation must be deferred to its appropriate place. The frequency of the heart, i.e. the number of beats in any given time, may vary. The average rate of the human pulse or heart -beat is 72 a mmute. It is quicker in children than in adults, but quickens again a little in advanced age. It is quicker in the adult female than in the adult male, in persons of short stature than in tall people. It is increased by exertion, and thus is quicker in a standing than in a sitting, and in a sitting than in a lying posture. It is quickened by meals, and while varying thus from time to time during the day, is on the whole quicker in the evening than in early morning. It is said to be on the whole quicker in summer than in winter. Even independently of muscular exertion it seems to be quickened by great altitudes. It is profoundly influenced by mental conditions. The length of the systole may vary, indeed we have reason to think that it does vary considerably, though as a general and broad rule it may be stated that a frequent differs from an infrequent pulse chiefly by the length of the diastole. Donders found the length of the systole as measured by the interval between the fli'st and second sounds to be for ordinary pulses remarkably constant in different persons, varying not more than from '327 to "oOl sec, and being therefore relatively to the whole cardiac period less in slow than in quick pulses. The force of the heat may vary ; the ventricular systole may be weak or strong. When the rate of beat is suddenly increased there is a tendency for the individual beats to be diminished in force, and on the other hand to be increased in force when the rate is diminished. But there is no necessary connection between rate and strength ; both a frequent and an infrequent pulse may be either weak or strong. The character of the heat ma}' vary; the systole may be sudden and sharp, rapidly reaching a maximum and rapidly declining, or slow and lengthened, reaching its maximum only after some time and declining very gradually; the latter being the slow pulse (pulsus tardus) as distinguished from the infrequent pulse (pulsus varus). The jDulse is also sometimes spoken of as being slapping, and sometimes as heaving. But, as we shall see immediately, the features of the pulse are dependent not only on the heart beat but also on the condition of the arteries. 160 YARIATIOXS IN THE HEARTS BEAT. [Book i. The rhythm may be intermittent or in-egular. Thus in an intermittent pulse, a beat may be so to speak dropped : the hiatus occurring either regularly or irregularly. In an irregular rhythm succeeding beats may differ in length, force, or character. SEC. 3. THE PULSE. When the finger is placed on an arten', such as the radial, an intermittent pressure on the finger, coming and going Avith the beat of the heart, is felt. "When a light lever such as that of the sphygmograph is placed on the artery, the lever is raised at each beat, falling between. The pressure on the finger, and the raising of the lever, are expressions of the expansion of the elastic artery, of the temporary additional distension which the artery undergoes at each systole of the ventricle. This intermittent expansion is called the pulse ; it corresponds to the intermittent outflow of blood from a severed artery, being present in the arteries only, and except under particular circumstances, absent from the veins and caj)illaries. The expansion is frequently \T.sible to the eye, and in some cases, as where an artery has a bend, may cause a certain amount of locomotion of the vessel. All the more important phenomena of the pulse may be witnessed on an artificial scheme. If two levers be placed on the arterial tubes of an artificial' scheme, one near to the pump, and the other near to the peripheral resistance, with a considerable length of tubing between them, and both levers be made to write on a recording surface, one im- mediately below the other, so that their curves can be more easily compared, the follo^^-ing facts may be observed, when the pump is set to work regidarly. ^ By this is simply meant a system of tubes, along which fluid can be driven by a pump worked at regular intervals. In the course of the tubes a (variable) resistance is introduced in imitation of the peinpheral resistance. The tubes on the proximal side of the resistance consequently represent arteries ; those on the distal side, veins. F. 11 162 THE PULSE. [Book i. 1. With eacli stroke of the pump, each lever (Fig. 27, 1, and II.) rises to a maximum, la, 2a, and then falls again, thus describing a curve, — the pulse-curve. This shews that the expansion of the 5oAAAAAAAAAAAA/\AAAy Fig. 27. Pulse-curves described by a series of sphygmograpliic levers placed at intervals of 20 cm. frora each other along an elastic tube into which fluid is forced by the sudden stroke of a pump. The pulse--wave is traveUing fi-om left to right, as indicated by the arrows over the primary (a) and secondary {b, c) pulse-waves. The dotted vertical lines drawn from the summit of the several primary waves to the tuning-fork curve below, each complete vibration of which occupies Jjj-sec., allow the time to be measured which is taken up by the wave in passing along 20 cm. of the tubing. The waves a are waves reflected from the closed distal end of the tubing; this is indicated by the direction of the arrows. It wUl be observed that ia the more distant lever YI. the reflected wave, having but a shght distance to travel, becomes fused with the prhnaiy wave. (From Marey.) tubing passes the point on which the lever rests in the form of a wave. At one moment the lever is quiet: the tube beneath it is simply distended to the normal permanent amount indicative CiiAi'. iv.) 77//; iM.sY7v..i/t' Mi:('iiAM,s.\r. ic;; of the mean arterial pressure; at tlic next nionieiit the j)uls(! cx]>ansiou reaches the lever, and the lever begins to rise, and continues to do so until the top of the wave reaches it, after which it falls attain until it is once more at rest, the wave havinjr completely passed by. The rise of each lever is somewhat sudden, but the fall is more gradual, and is generally marked with some irregularities. The suddenness of the rise is due to the suddenness with which the sharp stroke of the pump expands the tube ; the fall is more gradual because the elastic reaction of the walls, whereby the tube returns to its former condition after the expanding power of the pump has ceased, is gradual in its action. 2. The size and form of each curve depend in part on the amount of pressure exerted by the levers on the tube. If the levers only just touch the tube in its expanded state, the rise in each will be insignificant. If on the other hand they be pressed doAvn too firmly, the tube beneath will not be able to expand as it otherwise would, and the rise of the levers will be proportion- ately diminished. There is a certain pressure, depending on the expansive power of the tubing, at which the tracings are best marked. 8. If the points of the two levers be placed exactly one under the other on the recording surface, it is obvious that, the levers being alike except for their position on the tube, any difference in time between the movements of the two levers will be shewn by an interval between the beginnings of the curves they describe, if the recording surface be made to travel sufficiently rapidly. If the movements of the two levers be thus compared, it will be seen that the far lever (Fig. 27, II.) commences later than the near one (Fig. 27, I.), the farther apart the two levers are, the greater is the interval in time between their curves. Comj)are the series I. to VI. (Fig. 27). This means that the wave of expansion, the pulse-wave, takes some time to travel along the tube. By exact measurement it would similarly be found that the rise of the near lever began some fraction of a second after the stroke of the pump. The velocity with which the pulse-wave travels depends chietly on the amount of rigidity possessed by the tubing. The more extensible (N\dth corresponding elastic reaction) the tube, the slower is the wave ; the more rigid the tube becomes, the faster the wave travels. The width of the tube is of much less influence, though ac- cording to some observers the wave travels more slowly in the wider tubes. The rate at which the normal pulse-wave travels in the human body has been variously estimated at from 10 to 5 metres per second. In all probability the lower estimate is the more correct one ; but it must be remembered that in all probability the rate varies very considerably under different conditions. According to all observers the velocity of the wave in passing from the gi'oin to 11—2 1G4 THE rULSE. [Book i. the foot is greater than tliat in passing from the axilla to the wrist (6 m. against 5 m.). This is probably due to the fact that the femoral artery with its branches is more rigid than the axil- lary. So also in the arteries of children, the wave travels more slowly than in the more rigid arteries of the adult ; and the velocity appears to be increased by circumstances which heighten and decreased by those which lessen the mean arterial pressure, since ■with increasing or diminishing pressure the arterial walls become more or less rigid. 4. When two curves taken at different distances from the pump are compared with each other, the far curve will be found to be shallower, with a less sudden rise, and with a more rounded summit than the near curve : compare 5a with la. Fig. 27. In other words, the pulse-wave as it travels onward becomes diminished and tiattened out. If a series of levers, otherwise alike, were placed at intervals on a piece of tubing sufficiently long to convert the intermittent stream into a continuous flow, the pulse-wave might be observed to gradually flatten out and grow less until it ceased to be visible. Care must be taken not to confound the progression of the pulse-wave with the progression of the fluid itself. The pulse- wave travels over the moving blood somewhat as a rapidly moving natural wave travels along a sluggishly flowing river, the velocity of the pulse-wave being 9 metres per sec, while that of the current of blood is not more than half a metre per sec. even in the large arteries, and diminishes rapidly in the smaller ones. Taking the duration of the pulse-wave, that is the time taken by any point in the arterial tract, in expanding and returning to its former calibre, so low as -^^ of a second, it is evident that the pulse-wave started by any one systole, even if it travels so slowly as 5 m. per sec, will before it is completed have reached a point Y^ of 5m. = 2 m. distant from the ventricle. But even in the tallest man the tips of the toes are not 2 m. distant from the heart. In other words, the length of the pulse-wave is much greater than the whole length of the arterial system, so that the beginning of each wave has become lost in the small arteries and capillaries some time before the end of it has finally passed away from the beginning of the aorta. The general causation of the pulse may then be summed up somewhat as follows. The systole of the ventricle drives a quantity of blood into the already full aorta. The sudden injection of this quantity of blood expands the portion of the aorta next to the heart, and thus gives rise to the sudden up-stroke of the pulse-curve. The rapidity of the flow from the ventricle being greatest at its beginning, the maximum of expansion is soon reached, and the aortic walls, even while for a short time blood is still, with diminishing rapidity, issuing from the ventricle, tend by virtue of their elasticity to return to their former calibre. This Chap, iv.] 77//; VASCL'LAA' M Ec II A .\ IS.\f. 1G5 ivturn continues after the flow lias ceased, and the aortic valves soon becoming closed, the elastic force thus brought into play serves to drive the blood onward. The elastic recoil being slower than the initial expansion, the down-stroke of the pulse-curve is more gradual than the up-stroke. Of this jiortion of the aorta, which actually receives the blood cgcoted from the heart, the part immediately adjacent to the semilunar valves begins to exjiand first, and the ex- pansion travels thence on to the end of this portion. In the same way it travels on from this portion through all the succeeding portions of the arterial system. For the total expansion required to make room for the new quantity of blood cannot be provided by that portion alone of the aorta into which the blood is actually received ; it is supjdied by the whole arterial system : the old quantity of blood which is rejilaced by the new in this first portion has to find room for itself in the rest of the arterial space. As the expansion travels onward, hoAvever, the increase of pressure which each portion transmits to the succeeding portion will be less than that which it received from the preceding portion. For the whole increase of pressure due to the systole of the ventricle has to be distributed ov^er the whole of the arterial system, and a fraction of it must therefore be left behind at each stage of its progress ; that is to say, the expansion is continually gro\Wng less, as the pulse travels from the heart to the capillaries ; hence the diminished height of the pulse-curve in the more distant arteries, and its disappearance in the capillaries. Secondary Waves and Dicrotism, In nearly all pulse tracings, the curve of the expansion and contraction of the artery is broken Fig. 28. Pclse-tracing feom cuiotid abtery of healthy man^ (from Moens). X, commencement of expansion of the artery. A, summit of the first rise. C, dicrotic secondary wave. B, predicrotic secondary wave, p notch preceding this. D, succeeding secondary wave. The curve above is that of a tuning-fork with ten double vibrations in a second. 1 It will be understood that in the case of this and the succeeding sphygmo- graphic tracings (for the latter I am indebted to Dr Galabin and Dr Roy) comparisons between the several curves can only be made in a limited manner and with precautions, since the tracings are taken ^^-ith different amplifications, pressures, Ac. — and are some from man, others fi'om animals. They are introduced simply to illustrate points treated of successively in the text. lGt3 THE PULSE. [Book l by two, three, or several smaller elevations and depressions : secondary waves are imposed upon the fundamental wave. In the sphygmographic tracing from the carotid and radial reproduced in Figs. 28 and 29 and in many of the other tracings given, these secondary elevations are marked as B, C, D. When one such Fig. 29. Pulse-cdbve fkom radial of man. Taken with extra vascular pressure of 70 mm. mercury. The vertical curved line L, gives the tracing which the recording lever made when the blackened paper was motionless. The horizontal line forms the abscissa of the tracing. The curved interrupted lines shew the distance from one another in time of the chief phases of the pulse wave. x = commencement and A close of expansion of artery, p, predi- crotic notch, d, dicrotic notch. C, dicrotic crest. D, post-dicrotic crest. /, the post-dicrotic notch. secondary elevation only is conspicuous, so that the pulse-curve presents two notable crests only, the primary crest and the second- ary one, the pulse is said to be "dicrotic"; when two secondary crests are prominent, the pulse is often called "tricrotic," where \ Fig. 30. Anacrotic tulse-tracing from the carotid of rabbit. several "polycrotic." As a general rule, the secondary elevations appear only on the descending limb of the whole wave as in most of the curves given, and the curve is then spoken of as "katacrotic." Sometimes, however, the first elevation or crest is not the highest but CUAl'. IV.] THE VASCULMi MKCIIAMSM. 167 appears on the ascending portion of the main curve as in Fig. 30 and Fig. 33 : such a curve is spoken of as "anacrotic." Of these secondary elevations, the most frequent, conspicuous and important is the one wliich appears some way do^\Ti on the descending limb and is marked C on most of the curves. It is more or less distinctly visible on all sphygmographic tracings and may be seen in sphygmograms of the aorta aa well as of other arteries. Sometimes it is so slight as to be hardly discemiljle ; at other times it may be so marked as to give rise to a really double pulse (Fig. 31), i.e. a pulse which can be felt as double by the finger ; hence it has been called the dicrotic elevation or the dicrotic wave, the notch preceding the elevation being spoken of as the "dicrotic \i Fig. 31. Two gk.m^es of makked hicrgtism in radlvl pulse of man. (Typlioicl Fever.) notch." Neither it nor any other secondary elevations can be recog- nised in the tracings of blood-pressure taken with a manometer. This may be explained by the fact that the movements of the mercury column are too sluggish to reproduce these finer variations; but dicrotism is also conspicuous by its absence in the tracings given by more delicately responsive instruments. Moreover, when the normal pulse is felt by the finger, most persons find themselves unable to detect any dicrotism. Hence some have been led to mwmffifSfmmHummmmivmHmmmmmmmmMmhmmmmm^mmfmM Fig. 32. Noeiial pulse-curve in the aorta from the dog. maintain that this and the other secondary elevations do not really exist in the normal pulse. But it seems difficult to maintain this view in face of the experiment of Landois, in which the tracing obtained by allo^ving the blood to spirt directly from an opened small artery, such as the dorsalis pedis, upon a recording surface, shewed in an unmistakeable manner the existence of the dicrotic wave. 168 THE PULSE. [Book i. Less constant and conspicuous than the dicrotic wave but yet appearing in most sphygmograms is an elevation which appears higher up on the descending limb of the main wave; it is marked B on some of the curves and is frequently called the 'predicrotio Fig. 33. Axaceotic sphygmograph tracing fkom the ascending aorta (Aneumm). wave ; it may become very jDrominent. Sometimes other secondary waves are seen following the dicrotic wave as at D in Fig. 28; but these are very inconstant and usually even when present incon- sjdIcuous. When tracings are taken from several arteries or from the same artery under different conditions of the body, these secondary waves are found to vary very considerably, giving rise to many characteristic forms of pulse-curve. Moreover in the same arteiy. Fig. C4. Pulse-teacing from the dorsalis pedis. and with the same instrument, the form and even the special features of the curve vary according to the amount of pressure (expressed either in ounces or in mm. of mercury) with which the lever is pressed upon the artery. Figs. 35, 36 shew a series of changes thus brought about by varying the pressure of the lever ; and Fig. 37 shews the effect of this extra vascular pressure on the form of a fully dicrotic pulse. This effect of pressure in fact varies according to the condition of the vascular system. Were we able with certainty to trace back the several features of the curves to their respective causes, an adequate examination of sphygmographic tracings would undoubtedly disclose much valuable information concerning the condition of the body pre- senting them. Unfortunately the problem of the origin of these secondary waves is a most difficult and complex one ; so much so that the detailed intei'pretation of a sphygmographic tracing is still in most cases extremely uncertain. ClIAT. IV.] THE VASCrLAU MIX'llAMSM. 109 Various causes liavo been suggested as bringing about the secondary waves, and much discussion has arisen especially cou- ceniing the dicrotic wave. When the tube of the artiticial scheme bearing two levers is blocked just beyond the far lever, the primary wave is seen to be accompanied by a second wave, which at the i'ar lever is seen close to, and often fused into, the primary wave cTX.' ^O \ Fig. 35. IXFLUEKCE OF CHANGES IN THE PHESSUKE ATPLIEC TO THE EXTERIOR OF TUE VESSEL ON THE FOUH OF THE CURVE. a. From the Kii. radialis of healtliy man of 27 years of age with an extra arterial pressure equal in a to 70 mm., in a' to 50 mm., in a" to 30 mm. mercafy. (Fig. 27, VI. a), but at the near lever is at some distance from it (Fig. 27, I. a), being the farther from it, the longer the interval between the lever and the block in the tube. The second wave is evidently the primarj^ wave reflected at the block and travelling backwards towards the pump. It thus of course passes the far lever before the near one. And it has been argued that the dicrotic wave of the pulse is really such a reflected wave, started either at the minute arteries and capillaries, or at the points of bifurcation of the larger arteries, and travelling backwards to the aorta. But if this were the case the distance between the primary crest and the dicrotic crest ought to be less in arteries more distant from the heart than in those nearer, just as in the artificial scheme the reflected wave is fused with a primary 170 THE PULSE. [Book i. wave near the block, but becomes more and more separated from it, the farther back we trace it. Now this is not the case with the dicrotic wave. Careful measurements shew that the distance between the primary and dicrotic crests is either greater *s* *• Fig. 36. Normal pulse-curve feom carotid op rabbit ; shewing influence on height and form of curve of changes in the extra vascular pressui-e which was in a 20 mm., in h 30 mm., in c 40 mm., and d 50 mm. of mer- cury. or certainly not less in the smaller or more distant arteries than in the larger or nearer ones. This feature indeed proves that the dicrotic wave cannot be in any way a retrograde wave. Again, the more rapidly the primary wave is obliterated or at least diminished on its way to the periphery the less conspicuous should be the dicrotic wave. Hence increased extensibility and increased elastic reaction of the arterial walls which tend to use up rapidly the primary wave, should also lessen the dicrotic wave. But as a matter of fact these conditions are favourable to the prominence of ('ii\r. i\.J THE VASCVLMl MKCllAMSM. the dicrotic wave. Besides the imiltiludinons peri] hcr.d division would render one large pcripherically reflected wave inipiissible. But in addition to retlccted waves, other waves whii;li may be called "waves of oscillation," make their appearance when a fluid is driven through a system of tubes, by means of an intennitteut force. And dilVerent origins have been assigned to secondary waves of this description. \ vi ^' ^V^\. V'V' ' v.^Jv^->\^'■ Fig. 37. Dicrotic pulse-curve due to loss of blood. From carotid of rabbit vritb extra-vascular pressures in a of 50 mm., h of -iO mm. c of 20 mm., and d of 10 mm. of mercury. Thus when the rapid flow of a fluid along a tube is suddenly checked at a point of its course the inertia of the fluid ^^ill carry the column of fluid still forwards so as to leave behind it a diminution of pressure. This diminution will appear on a graphic record of the pressure as a depression or notch ; and will be followed by a secondary rise as a reflux of fluid takes place towards the point where the pressure has become diminished. Both the depression and the secondary rise will travel as a wave along the tube, being frequently followed by other smaller waves of similar character and similar origin. Waves thus originating have been appealed to as explaining the secondary waves of the pulse-curve. Thus at the moment when the ventricle, ha\dng emptied itself, ceases to throw any more blood into the aorta, the blood which was last ejected being carried forward by its inertia gives rise to a diminution of pressure in the ventricle and at the root of the aorta. The aortic w^alls forth-\\ith contract upon this diminished pressui-e, and a reflux of blood towards the semilunar valves takes place, leading to the appearance of a depression or notch in the pulse-curve, which is jiropagated forwards along the aorta. This reflux closes the semi- lunar valves and at the same time leads to a recovery of pressure 172 THE PULSE. [Book i. which similarly appears on the pulse-curve as an elevation succeed- ing the notch. Then again it has been argued that in any section of the arterial tract, the inertia of the walls and of the contained blood, in each expansion of the section, carries them on in their movement of expansion some little time after the actual expanding force has ceased to act. This leads to a falling back or contraction, which again by reason of the same inertia overshoots its mark, and thus through a series of oscillations, of which the first is the most conspicuous, the artery settles down to its normal calibre before the next expansion reaches it. The extent of such oscillations is determined, not only by the character of the walls but by the specific gravity of the contained fluid. In the artificial scheme with the same elastic tubing the secondary waves thus caused are much greater with mercury than with water, and disappear almost wholly when air is employed. Such waves of oscillation may be supposed to be generated in different degrees, in each and every section of the arterial tract ; the waves due to a cessation of the flow are on the contrary generated at the point where the inter- mittence is effected, and may be seen in rigid as well as in elastic tubes ; but these latter waves also are profoundly modified by the nature of the walls of the tubes along which they are transmitted. Lastly, it has been maintained that these secondary waves are of active not passive origin; that is, that they are caused by a rapid muscular contraction of the arterial walls following up so to speak the arterial beat. We have dwelt at so great a length on these secondary waves of the pulse-curve because of the importance attached to them in clinical medicine ; but it would be hardly profitable to enter more fully into the discussion of these several contending views. As an instance of the difficulty of the subject and the insufficiency of our knowledge, we may point out that observers are not yet agreed as to which part of the curve corresponds to the closure of the semilunar valves. Thus some maintain that this event corresponds to and indeed is indicated by the dicrotic wave, the dicrotic notch representing the reflux towards the ventricle, and the dicrotic elevation a new forward movement reflected from the closed valves. But under this view, though it seems the more probable, the predicrotic wave presents a difficulty; and indeed others maintain that the moment of closure of the semilunar valves is indicated by this the predicrotic, and not by the dicrotic wave. Until this and other points are finally settled, all interpretations of modifications of the pulse-curve must remain uncertain and un- satisfactory. The following facts however may be borne in mind as not only of practical importance, but as necessary data for any judgments concerning the pulse-curve. CiiAi'. IV.] 77/ A' WlSCrLAJ: MKCUAMSM. 173 1. \\'luiti'ver (lie origin of the dicrotic wave, its features may 1)1' modified by changes taking ]»hice in the peripheral (arterial) ilistricts without any alteration in the central (cardiac) events. Thus dicrotism may become conspicuous in one artery while re- maining indistinct in others. 2. The prominence of the dicrotic wave, though favoured by a sudden strong ventricular systole, is especially assisted by a diminution of blood-pressure. Thus it is a marked characteristic of the pulse in many cases of fever (Fig. 31) where blood-pressure is low. So also it may be brought on at once in an artery in which it was previously insignificant by sudden lowering of the blood- pressure as is shewn in Fig. 88. It may similarly be induced by A. ,1 Mf^AMM Fig. 33. Tracing fuom b.u>ial in max ; shewing change in form of pulse-curve accompanying a sudden fall in tlie lilood- pressure. The pulse, at first not markedly dicrotic, rapidly hecomes so, and then passes on into the condition known as hyperdicrotism, where the dicrotic notch leaches a level lower than that from which tlie primary rise started. section of the vaso-motor nerves belonging to the branches of the artery; this, as we shall presently see, diminishes the peripheral resistance, through an expansion of the minute arteries, and so leads to a lowering of the blood-pressure in the main arteries. The prominence of the dicrotic wave is further dependent on the amount of extensibility and elastic reaction of the arterial Avails, Hence the dicrotic wave is not well marked in arteries which have become rigid by disease or old age. "We may add that an anacrotic pulse, in which a crest followed by a notch is visible on the ascending portion of the curve, before the maximum of expansion is reached, though it may sometimes be produced temporarily in healthy persons, is generally associated with diseased conditions, usually such in which the arteries arc abnor- mally rigid. It has been interpreted as due to the pressure in the aorta rising even after the first rapid rush from the ventricle. Under 174 TUE PULSE. [Book i. normal conditions, as "we have already seen, the maximum expansion is soon reached, but in cases where the arterial walls are unusually rigid and the heart at the same time not abnormally weak, the ventricle may continue to empty itself against a resistance which increases rapidly, with the amount of blood passing into the aorta, so that in spite of the diminishing rapidity with w^hich the blood is leaving the ventricle the insufficient distensibility of the vessels causes the pressure in their interior to continue to rise until nearly the end of the outflow from the heart. An anacrotic pulse also frequently accompanies hypertrophy and dilation of the left ventricle. The pulse then is the expression of two sets of conditions : one pertaining to the heart, and the other to the arterial system. The arterial conditions remaining the same, the characters of the pulse may be modified by changes taking place in the beat of the heart ; and again, the beat of the heart remaining the same, the pulse may be modified by changes taking place in the arterial walls. Hence the diagnostic use of the pulse-characters. It must however be remembered that arterial changes may be accompanied by com- pensating cardiac changes, to such an , extent, that the same features of the pulse may obtain under totally diverse conditions, provided that these conditions affect both factors in compensating directions. Venous Pulse. Under certain cu-cumstances the pulse may be carried on from the arteries through the capillaries into the veins. Thus when the salivary gland is actively secreting, the blood may issue from the gland through the veins in a rapid pulsating stream. The nervous events which give rise to the secretion of saliva, lead at the same time, by the agency of vaso-motor nerves, of which we shall presently speak, to a dilation of the small arteries of the gland. This dilation of the small arteries diminishes the peripheral resist- ance by allowing more blood to pass through them with less friction; in consequence the elasticity of the arterial walls is brought into play to a less extent than before, and this may in certain cases go so far, that as in the case of the artificial apparatus, where the elastic tubing has an open end (see p. 129), not enough elasticity is brought into action to convert the intermittent arterial flow into a con- tinuous one. A similar venous pulse is also sometimes seen in other organs. Careful tracings of the great veins in the neighbourhood of the heart shew elevations and depressions, which appear due to the variations of intracardiac pressure, and which may perhaps be spoken of as constituting a "venous pulse" ; but at present they need further elucidation. In cases of insufficiency of the tricuspid valves, the systole of the ventricle makes itself felt in the great veins ; and a distension travelling backwards from the heart be- Chap. iv.J THE VASCULAll MPXIIAMSM. 175 comes very visible in the veins of the neck. This is sometimes spoken of as a venous pulse. Variations of pressure in the great veins due to the respiratory movements are also sometimes spoken of as a venous pulse ; the nature of these variations will be explained in treating of respi- ration. 11. THE VITAL PHENOMENA OF THE CIRCULATION. So far the facts with which we have had to deal, with the ex- ception of the heart's beat itself, have been simply physical facts. All the essential phenomena which we have studied may be re- produced on a dead model. Such an unvarying mechanical vascular system would however be useless to a living body whose actions were at all complicated. The prominent feature of a living mechanism is the power of adapting itself to changes in its in- ternal and external circumstances. In such a system as we have sketched above there would be but scanty power of adaptation. The well-constructed machine might work with beautiful regu- larity; but its regularity would be its destruction. The same quantity of blood would always flow in the same steady stream through each and every tissue and organ, irrespective of local and general wants. The brain and the stomach, whether at work and needing much, or at rest and needing little, would receive their ration of blood, allotted with a pernicious monotony. Just the same amount of blood would pass through the skin on the hottest as on the coldest day. The canon of the life of every part for the whole period of its existence would be furnished by the inborn diameter of its blood-vessels, and by the unvarying motive power of the heart. Such a rigid system however does not exist in actual living beings. The vascular mechanism in all animals which possess one is capable of local and general modifications, adapting it to local and general changes of circumstances. These modifications fall into two great classes : 1. Changes in the heart's beat. These, being central, have of course a general effect. 2. Changes in the peripheral resistance, due to variations in the calibre of the minute arteries, brought about by the agency of their contractile muscular coats. These changes may be either locol or general. CiiAP. IV.) rill-: vasci'i.m: mi:(:iia.\ism. 177 To flirsi' may he addi'il as subsidiary iiiudirvini,' fvnits: W. C'liau^t'S ii» tlu' pcriitlu'ral rcsistauco of th(! capillai-ics duo to alterations in tho adlu'sivcness of the capillary walls or to «)ther inHuences arisiiiLj out of the as yet obscure relations existing betw(>en the blood within and the tissue without the thin per- meable capillary walls, and depending on the vital conditions of the one or of the other. Such changes causing an increase of ])ori- I)heral resistance arc seen to a marked degree in the patholoo-ical condition known as stasis. 4. Changes in the quantity of blood in circulation. The tw^o fii-st and chief classes of events (and probably the third) are directly under the dominion of the nervous system. It is by means of the nervous system that the heart's beat and the calibre of the minute arteries are brought into relation with each other, and with almost every part of the body. It is by means of the nervous system acting either on the heart, or on the small arteries, or on both, that a change of circumstances affecting either the Avhole or a part of the body is met by compensating or regulative changes in the flow of blood. It is by means of the nervous system that an organ has a more full supply of blood when at work than when at rest, that the stream of blood through the skin rises and ebbs with the rise and fall of the temperature of the air, that the work of the heart is tempered to meet the strain of overfull arteries, and that the arterial gates open and shut as the force of the central pump waxes and w^anes. Each of these vital factors of the circulation must therefore be considered in connection with those parts of the nervous system which are concerned in its action. 12 SEC. 4. CHANGES IN" THE BEAT OF THE HEART. We have already discussed the more purely mechanical pheno- mena of the heart. We have therefore in the present section only to inquire into the nature and working of the mechanism (chiefly at least nervous) by which the beat of the heart is maintained, varied, and regulated. In studying closely the phenomena of the beat of the heart it becomes necessary to obtain a graphic record of various movements. 1. In the frog or other cold-blooded animal, a light lever may be placed directly on the ventricle (or on an auricle, &c.) and changes of form, due either to distension by the influx of blood, or to the systole, will cause movements of the lever, which may be recorded on a travelling surface. The same method may be applied to the mam- malian heart, but difficulties are introduced by the locomotion of the heart caused by the movements of the lungs. 2. Or, as in Gaskell's method, the heart may be fixed by a clamp carefully adjusted round the auriculo-ventricular groove while the apex of the ventricle and some portion of one auricle are attached by threads to horizontal levers placed respectively above and below the heart. The auricle and the ventricle each in its systole pulls at the lever attached to it; and the times and extent of the contractions may thus be recorded. 3. A record of mtracardiac pressure may be taken in the frog or tortoise, as in the mammal, by means of an appropriate manometer. And in these animals at all events it is easy to keep up an artificial circulation. A cannula is introduced into the sinus venosus and another into the ventricle through the aorta. Serum or dilute blood (or any other fluid which it may be desired to employ) is driven by moderate pressure through the former; to the latter is attached a tube connected by means of a side piece with a small mercury manometer. So long as the exit tube is open at the end, fluid flows freely through the heart and apparatus. Upon closing the exit tube at its far end, the force of the ventricular systole is brought to bear on the manometer. ClIAI". IV. Till': V ASCI' I. A U mi;/' II AX ISM. 179 tlio iiiiK'X of wliicli registers in tlio usual way the movenmuts of tho mercury column. J>Ie\voll Martin has suocoedcd in applying a luoililicatioii of this method to tho mammalian heart. 4. Tho movements of tho ventricle may be registered by introducing into it through the auriculo-ventricular oritico a so-called 'perfusion' cannula^ Fig. 39 i. with a double tube, one inside the other, and tying the ventricle on to tho cannula at the auriculo-ventricular groove, or at aiiv level below that which may be desired. The blood or other fluid is driven at an adequate pressure through the tube a, enters the ventricle, and returns by the tube b. If 6 be connected with a manometer as in method 3, the movements of the ventricle may be registered. 5, In the apparatus of Hoy, Fig. 39 li., the exit tube is free but the ventricle (the same method may be adopted for the whole heart) is placed in an air-tight chamber tilled with oil or partly with normal saline solution and partly with oil. By means of the tube b the interior Fig. 39. Purely dugrammatic figures of I. Perfusion cannula tied into frog's ventricle, a. entrance, b, exit, tube; a, wall of ventricle ; /3, ligature. II. Eoy's apparatus modified by GaskcU. a, chamber filled with saline solution and oU, containing the ventricle a tied on to perfusion cannula/, b, tube leixding to cylinder c, in which moves piston d, working the lever e. of the chamber a is continuous with that of a small cylinder c in which a piston d secured by thin flexible animal membrane works up and down. The piston again bears on a lever e by means of which its movements may be registered. When the ventricle contracts, and by contracting diminishes in volume, there is a lessening of pressure in the interior of the chamber, this is transmitted to the cylinder, and the piston correspondingly rises, carrying with it the lever. As the ventricle subsequently becomes distended the pressure in the chamber is increased, and the piston and lever sink. In this way variations in the ^'olume of the ventricle may be recorded, without any interference with the flow of blood or fluid through it. JO 2 180 THE CARDIAC MUSCLES. [Book i. The Mechanism of the JS'ormal Beat. The cardiac Muscles. When a frog's heart which has ceased to beat spontaneously is stimulated by touching it with a blunt needle, a beat is frequently called forth ; this artificial beat differs in no obvious characters from a natural beat. The latent period of such an artificial beat is remarkably long, the length varying within very wide limits. Thus the cardiac contraction is more like that of an unstriated than of a striated muscle. The beat is in fact a modified or peculiar form of peristaltic contraction. In the hearts of some animals, the ventricle fonns a straight tube ; and in these the peristaltic character of the beat is obvious ; but in a twisted tube like that of the vertebrate ventricle, ordinary peristaltic action would be impotent to drive the blood onward, and is accordingly so far modified that the peristaltic character of the beat is recognised only when the action of the heart becomes slow and feeble. The cardiac, like the skeletal muscular fibre, after a contraction returns by relaxation to its previous shape, and the whole ventricle (or whole heart) regains after a beat the form natural to its qui- escent state. This diastolic expansion, though increased by, is not dependent on, the influx of fluid into the cavities of the heart. Thus the cavity of the empty quiescent mammalian left ventricle, though smaller than when it is distended with blood as in its normal action, is larger than when it is in systole or when rigor mortis has set in ; moreover if its dimensions be artificially less- ened, as when it is squeezed with the hand, it returns by an elastic reaction to its former volume when the pressure is removed. The cardiac muscles in a healthy condition are, like the skeletal muscles, very elastic. Their elasticity is however soon interfered with by imperfect nutrition ; and a 'contraction remainder' (p. 57) under certain circumstances is readily developed. Under the influences of certain poisons, veratrin, digitalin, &c., the length of the beat is enormously prolonged, and the ventricle is eventually thrown into a remarkable contracted condition, the exact nature of which is perhaps not thoroughly understood, though it is believed by many to be due to a deficiency of elastic reaction. One great feature of the cardiac beat produced by artificial stimulation is the absence of that relationship between the strength of the stimulus employed and the amount of contraction evoked which is so striking in a skeletal muscle (p. 85). The beat with which a heart responds to a stimulus, e.g. a single induction shock, is, if there be any response at all, equally large when a feeble as when a strong stimulus is used, though the strength of the beat evoked either by a strong or a weak stimulus may vary con- siderably ■v\dthin even a very short period of time. Chap. IV. I /'//A' VASCCLA U M i:c IIA MSM. \^\ When a si'foiul iiKliicti(»n shock is st.-iit in at a certain interval after a first, the beat due to the second shock is often lar^o-r tlian the first, the benetieial elleets of a contraction (see p. Ut!) beinj^ even still more manifest in the heart than in an ordinary skeletal muscle. Frequently by successive shocks of equal intensity a 'staircase' of beats of successively increasing amplitude may be proibiced. When a second induction shock follows upon the first too rapidly, it is apparently without elTect; no second beat is produced. So also when a series of rapidly repeated induction shocks are sent in, a certain niuubcr of them are thus 'inetiectual'; the application of the ordinary interrupted current gives rise not to a tetanus but to a rhythmic series of beats. The ' refractory period,' which is so brief in the skeletal muscle (see p. 87), is very prolonged in the cardiac muscle. So also in a spontaneously beating heart, induc- tion shocks sent in at a certain phase of a cardiac cycle, e.rj. the commencement of the systole, are ineffectual, though they produce forced beats when sent in at the other phases of the cycle. As we shall immediately see, the beat of the heart, and even of a part of the heart such as the ventricle, is not a mere muscular contraction but a complex act, in which both nervous and muscular elements intervene ; and it is difficult in all cases to distinguish the action of the one from that of the other. It is probable how- ever that many of the features which we have just described are due to peculiarities of the cardiac muscle. Nervous mechanism of the Beat. The heart of a mannnal or of a wanu-blot ide'd animal ceases to beat almost immediately after being removed from the body in the ordinary way ; and though by special precautions and by means of an artificial circulation of blood, an isolated mammalian heart may be preserved in a pulsating con- dition for a considerable time, our knowledge of the exact nature and of the causes of the cardiac beat is as yet almost entirely based on the study of the hearts of cold-blooded animals, Avhich will continue to beat for hours, or under favourable circumstances even for days, after they have been removed from the body with only ordinary care. M^e have reason to think that the mechanism by which the beat is carried on, varies in some of its secondary featui'es in even the cold-blooded animals: that the hearts, for instance, of the snake, the tortoise and the frog, differ as to the exact manner of canying out the beat, both from each other and from the bird and the mammal ; but we may, at first at all events, take the heart of the frog as illustrating the main and important truths concerning the causes and mechanism of the beat. The heart of the frog, as we have just said, will continue to beat for hours after removal from the body; and the beats are in all important respects identical with the beats executed by the 182 NERVOUS MECHANISM OF THE BEAT. [Book i. heart in its normal condition within the living body. Hence we may infer that the beat of the heart is an automatic action : the muscular contractions which constitute the beat are caused by impulses which arise spontaneously in the heart itself. The beat goes on even after the cavities have been cleared of blood, and indeed when they are almost empty of all fluid, A beat cannot therefore be, as was once thought, a reflex act excited by the entrance of blood into the cavities of the heart. In the frog's heart, as in that of the mammal, there is a distinct sequence of events. First comes the beat of the sinus venosus, preceded by a more or less peristaltic contraction of the large veins leading into it, next follows the sharp beat of the two auricles together, then comes the longer beat of the ventricle, and lastly the beat of the bulbus arteriosus completes the cycle. If the incisions, by which the heart is removed, be made carefully, so as not to injure at all the sinus venosus, the beats will continue after a very short pause, or sometimes without any real interruption, with great vigour for a very considerable time. In order that the frog's heart may beat after removal from the body with the nearest approach in rapidity, regularity and endurance to the normal condition, the removal must be carried out so as to leave the sinus venosus intact. When the incision is carried through the auricles so as to leave the sinus venosus behind in the body, the result is different. The sinus venosus beats forcibly and regularly, having suffered hardly any interruption from the operation. The excised heart, however, remains, in the majority of cases, for some time motionless. Stimulated by a prick or an induction-shock, it will give one, two or several beats, and then come to rest But it will in the majority of cases, the animal having previously been in a vigorous condi- tion, recommence after a while its spontaneous beating, the systole of the ventricle following that of the auricles ; but the rhythm of beat will not necessarily be the same as that of the sinus venosus left in the body, and the beats will not continue to go on for so long a time as will those of a heart still retaining the sinus venosus. When the incision is carried through the auriculo- ventricular groove, so as to leave the auricles and sinus venosus within the body, and to isolate the ventricle only, the results are similar but more marked. The sinus and auricles beat regularly and vigor- ously, with their proper sequence, but the ventricle generally re- mains for a long time quiescent. When stimulated however the ventricle will give one, two or several beats, and after a while, in many cases at least, will eventually set up a spontaneous pulsation with an independent rhythm; and this may last for some consider- able time, but the beats are not so regular and will not go on for so long a time as will those of a ventricle to which the auricles are still attached. CiiAP. IV.] TlIK VASCl'LAU MEClIANIi^M. J.s.'i If a transvcrso incision be carried through tho ventricle at about its u])i)er third, leaving the base of the ventricle still attached to the auricles, the jjortion of the heart left in the body will go on ])ulsating regularly, with the ordinary sequence of sinus, auricles, ventricle, but the isolated lower two-thirds of tlie ventricle will not beat spontaneously at all however long it be watched. Moreover in response to a single stimulus such as an iiuluction-shock or a gentle ])rick it gives, not aa in the case of the entire ventricle or of the ventricle to which the auricles are attached, a series of beats, but a single beat. Lastly, to complete the story we may add, that when the heart is bisected longitudinally, each half continues to beat spontaneously, with an independent rhythm, so that the beats of the two halves are not necessarily synchronous, and this continuance of spontaneous pulsations after longitudinal bisection may be seen in the conjoined auricles and ventricle, or in the isolated auricles, or in the isolated but entire ventricle. Moreover the auricles may be divided in many ways and yet many of the segments will continue beating ; small pieces even may be seen under the microscope pulsating, feebly it is true but distinctly and rhythmically. The various parts of the frog's heart thus fonn, as regards the power of spontaneous pulsation, a descending series : sinus venosus, auricles, entire ventricle, lower portions of ventricle, the last exhibiting under ordinary circumstances no spontaneous pulsations at all. Now ganglia, containing nerve cells, are found in great abun- dance in the sinus venosus, are seen in various parts of the auricles, and occur as the so-called Bidder's ganglia at the junction of the auricles and ventricle, from whence they also spread into the upper part of the ventricle ; in the lower two-thirds of the ventricle they are entirely wanting. It is natural to infer from this that the ganglia are in some way the agents of the spontaneous pulsation. The uncertainty, and in most cases temporary character of the pulsations, occurring with seeming spontaneity, in the auricles or ventricle separated from the sinus venosus, have led many to the opinion that these are not really spontaneous, but of the nature of reflex acts, induced by some obscurely acting stimuli, and that really spontaneous pulsations proceed only from the sinus venosus. And a view has been generally adopted which teaches that the spontaneous beats of the frog's heart are due to rhythmic nervous impulses started in the ganglia of the sinus venosus and spreading thence to other parts, the ganglia of the auricles and of the auriculo-ventricular groove acting in subordination to those of the sinus, or behaving under certain circumstances independently as reflex centres, or performing other functions which we shall have to speak of immediately as of a restraining or inhibitory 184 INHIBITION OF THE BEAT. [Cook i. character. And the same view with possibly some slight modi- fications has been supposed to hold good for the hearts of all vertebrate animals. Facts however are met with which appear to oppose this con- ception. If the " perfusion" cannula previously described be introduced into a frog's ventricle and secured by a ligature carried round the ventricle some little distance below the base, the lower part of the ventricle remains motionless and free from pulsations in the same way as when it has been removed by an incision. If however the cavity be regularly supplied with serum or diluted blood (that of the rabbit being practically the most useful), after a longer or shorter time, this portion of the ventricle begins to pulsate with a more or less regular rhythm and will continue these apparent spontaneous beats for an almost indefinite time. It is usual to explain these pulsations, which may be witnessed even when only the extreme tip of the ventricle is tied on to the cannula, as not really spontaneous but as excited by the senim or dilute blood, supplied under pressure, acting as a stimulus ; such an explanation is however hardly satisfactory. Then again, though it is quite true that the beats of an isolated frog's ventricle are uncertain and temporary, so much so as perhaps to justify the view that they are not really spontaneous, the isolated ventricle of the tortoise beats with such regularity and for so long a time, that it seems almost impossible to avoid the conclusion that in this animal, at all events, the ventricle by itself possesses a real power of spontaneous pulsation. Moreover even in the frog, section at various points, of the nerves with which the ganglia are connected, may be effected and indeed Bidder's ganglia carefully extirpated, without the natural sequence of beat of the several parts being changed. And careful investigation has dis- closed many other facts, which we cannot discuss here but which go far to shew that the generation of the beat of the heart is a very complex matter indeed. While we must admit that the ganglia of the sinus venosus (in the frog, or what corresponds to these in other animals) are prepotent in the work of producing the beat, our knowledge will not at present allow us to make a definite and consistent statement as to what it is they exactly do, or as to the share in generating and carrying out the beat, which is taken by the other ganglia, and their respective nerves, or by the muscular fibres themselves. Inhibition of the Beat. The beat of the heart may be stopped or checked, i.e. may be inhibited by efferent impulses descending the vagus nerve. If while the beats of the heart of a frog are being care- fully registered (Fig. 40) an interrupted current of moderate strength be sent through one of the vagi, the heart is seen to stop beating. It remains for a time in diastole, perfectly motionless CUAI'. IV. Till-: VASCULAi: .Uh'( 'I/AX ISM. 185 iiiul thuviti, 11" the (luniliuii of the curn-iit be short an*»th cases, reaching the niechilhi from the; hrain. In succeethng pages wc sliall have occasion more than onc(! in discuss- ing the erti'cts of stimuhiting a given nerve, to consider liow far tliose eilects are due to a reflex inhibition of the heart; and probably there are few events taking phice in the body which have not a tendency thus to aflect the central vascular pump, though in many cases the tendency is counteracted by interfering agencies. ]jut we nuist be careful to avoid falling into the error of supposing that every arrest, or slowing or weakening of the heart, is due to impulses descending the vagus fibres. In many instances cardinc troubles are due to events originating in the heart it.self, so far indei)endent of the inhibitory processes which we are studying now, that they are in no way whatever counteracted by atropin. Direct stinudation of the cardio-inhibitory centre itself, such as occurs during the destniction of or results from injury to the medulla, also produces inhibition. And the question naturally arises, Has this cardio-inhibitory centre any constant automatic action ? In the dog, and also, though to a far less extent, in the rabbit, section of botli vagi is followed by a quickening of the heart's beat. This result may be inteqireted as shewing that the centre in the medulla exercises a permanent restraining influence on the heart ; that organ in fact being habitually curbed. The argument that the effects of an artificial stimulation of the vagus soon wear off, and that therefore a permanent stimulation of the vagi, leading to permanent inhibitory action, would be impossible, may be met by the reflection that a natural stimulation is, possibly, not wholly identical with artificial stimulation, and its eSects need not necessarily wear off. We need not now stay to discuss the question whether this central action is really automatic, i.e. kept up by molecular pro- cesses originating in certain nerve cells, or reflex, that is, maintained by nervous impulses reaching it along certain or various afferent nen'es. Granting, however, the existence of a centre in the medulla, which either automatically or otherwise is in permanent action, it is obviously open to us to speak of reflex inhibition as being brought about by influences which augment the action of that centre. But we have seen that active nervous centres are subject, not only to augmentative, but also to inhibitory infiuences. Hence the cardio-inhibitory centre might itself be inhibited by impulses reaching it from various quarters. In other words, the beat of the heart might be quickened by a lessening of the normal action of the inhibitory centre in the medulla. It is in fact probable, that many cases of quickening of the heart's beat are produced in this way ; though the matter requires further investi- gation. Accelerator nerves. The heart's beat may in the mammal be quickened, even after division of both vagi, by direct stimulation 190 A CCEL ERA TO R iVER VES. [Book i. of the cervical spinal cord. The effects produced, however, are very complex, and led, on their first being made known, to much discussion, one outcome of which was the discovery of certain nerves of a very peculiar character, which pass from the cervical spinal cord, frequently along the nerve accompanying the vertebral artery, and reach the heart through the last cervical and first thoracic ganglia ; these have been called the ' accelerator nerves.' Their course is different in the rabbit and in the dog, see Figs. 41 and 42, and indeed varies even in the same kind of animal. Stimulation of these nerves with the interrupted current causes a quickening of the heart's beat, in which what is gained in rate is lost in force, for the blood-pressure is not necessarily increased, but may remain the same, or even be diminished ; apparently not only sym.f^or. n.t'a£^. Fig. 41. The last cervical and first thoracic ganglia in the Eabeit. (Left side.) (Somewhat diagrammatic, many of the various branches being omitted.) Tracli. Trachea. Ca. carotid artery. s5. subclavian artery, n. Vag. the vagus trunk, n. rec. the recurrent laryngeal, sym. the cervical sympathetic nerve ending in the inferior cervical ganglion, gl. cerv. inf. Two roots of the ganglion are shewn, racL, the lower of the two accompanying the vertebral artery, A. vert., being the one generally possessing accelerator properties, gl. thor. pr. the first thoracic ganglion. Its two branches communicating with the cervical ganglion surround the subclavian artery forming the annulus of Vieussens. sym. thor. the thoracic sympathetic chain, n. dep. depressor nerve, which, though running by the side of the sympathetic, is really a branch of vagus, from wliich it separates higher up. This is joined in its course by a branch from tlie lower cervical ganglion, there being a small ganglion at their junction, from which proceed nei-ves to form a plexus over the arch of the aorta. It is this branch from the lower cervical ganglion which possesses accelerator properties— hence the course of the accelerator fibres is indicated in the figure by the arrows. UllAl'. IV. ] THE VASCi'LAU M i:C II A MS.]f. 191 is the dia-stolo diminisliod but the systole is actually shortened. Our knowledge of these 'accelerator' nerves is however too im- perfect to be dwelt uj)on here. Other modiiying agents. The beat of the heart may also be moditied by inHuences bearing directly on the nutrition of the lieart. The tissues of the heart, like all other tis.sues, need an adequate supply of blood of a proper quality; if the blood vary in quality or (piantity the beat of the heart is correspondingly alTected. The excised frog's heart, as we have seen, continues to beat for some considerable time, though apparently empty of blood. r. .lym. / sym.^ioreic. Via. 42. The last certic.\l and first thoracic ganglia in the Dog. The cardiac nerves of the Dog. The figure is largely diagramiiiatic, and represents the left side. V. sym. the united vagus and cervical sympathetic nerves, gl. cerv. i. the mferior cervical ganglion, n. v. the continuation of the trunk of the vagus. aim. V. the two branches forming the anuulus of Vieussens round the subclavian artery, art. suhcl., and joining gl. th. pr., the first thoracic or stellate ganglion (the branch running in front of the artery is considered by Schmiedeberg to be an especial channel of accelerator fibres), sym tltorac. the sympathetic trunk in the thorax. r. vert, communicating branches from the cervical nerves running alongside the vertebral artery, the rami vertebrales. n. ree. the recurrent laryngeal, n. c. cardiac branches from the lower cervical ganglion, accelerator nerves of Schmiedeberg. n'. c'. cardiac branches from the first thoracic ganglion, accelerator nerves of Cyon. n". c". cardiac branch fi'om recurrent nerve, r. rcc. branch from lower ceiTical ganglion to the recurrent nerve, often containing accelerator fibres. After a while however the beats diminish and disappear; and their disappearance is greatly hastened by washing out the heart vnih a normal saline solution, which when allowed to flow through the cavities of the heart readily permeates the tissues on account of the peculiar construction of the ventricular walls. If such a 192 MODIFYING AGENTS. [Book i. 'washed out' quiescent heart be fed in the manner described at p. 179, with dihited blood (of the rabbit, sheep, &c.) it may be restored to functional activity. A similar but less complete resto- ration may be witnessed if serum be used instead of blood ; and a heart fed regularly with fresh supplies of blood or even of serum may be kept beating for a very great length of time. In treating of the skeletal muscles we saw that in their case the exhaustion following upon withdrawal of the blood-stream might be attributed either to an inadequate supply of new nutritive material and oxygen, or to an accumulation in the muscular substance of the products of muscular metabolism, or to both causes combined. And the same considerations hold good for the nervous and muscular structures of the heart, though the subject has not yet been sufficiently well Vv^orked out to permit any very definite statements to be made. It seems probable however that an important factor in the matter is the accumulation in the muscular fibres and in the surrounding lymph of carbonic acid, and of the substances which give rise to the acid reaction. When the frog's heart is thus 'fed' with various substances the interesting fact is brought to light that some substances, such, for instance as very dilute lactic acid, lead to increased expansion, and others, such for instance as very dilute solutions of sodium hydrate, to diminished expansion, or to continued con- traction of the quiescent ventricle. It would appear that the muscular fibres of the ventricle over and above their rhythmic contractions are capable of varying in length, so that at one time they are longer, and the ventricle when pressure is applied to it internally dilates beyond the normal, while at another time they are shorter, and the ventricle, with the same internal pressure is contracted beyond the normal. Further, in the frog at least, when the pause between two beats is lengthened the relaxation of the ventricle goes on increasing, so that apparently the ventricle when beating normally is already somewhat contracted when a new beat begins. In other words, the ventricle possesses what we shall speak of in reference to arteries as tonicity or tonic contraction, and the amount of this tonic contraction, and in consequence the capacity of the ventricle, varies according to circumstances. When the frog's ventricle is thus artificially fed with serum or even with blood, the beats, whether spontaneous or provoked by stimulation, are apt to become intermittent and to arrange them- selves into groups. This intermittence is possibly due to the serum or blood being unable to carry on nutrition in a completely normal manner, and to the consequent production of abnormal chemical substances ; and it is probable that cardiac intermittences seen during life have often a similar causation. Various chemical substances in the blood, natural or morbid, may thus affect the heart's beat by acting on its muscular fibres, or its nervous elements, or both, and that probably in various ways, modifying in CuAP. IV.] THE VASCULAR MFCI/AXISJf. 193 different directions the rliytlnn, or the individual contractions, or both. The physical or mechanical circumstances of the heart also affect its beat ; of these perhaps the most important is the amount of the distension of its cavities. The contractions of cardiac muscle, like those of ordinary muscle (see p. 87), are increased up to a certain limit by the resistance which they have to overcome ; a full vcntriele will, other things being equal, contract more vigorously tlian one less full ; though, as in ordinary muscle, the limit at which resistance is beneficial may be passed, and an over- full ventricle will cease to beat at all. Under normal conditions the ventricle probably empties itself completely at each systole. Hence an increase in the quantity of blood in the ventricle would augment the work done in two ways ; the quantity thrown out would be greater, and the increased quantity would be ejected with greater force. Further, since the distension of the ventricle is (at the commencement of the systole at all events) dependent on the auricular systole, the work of the ventricle (and so of the heart as a whole) is in a measure governed by the auricle. The relation of the heart's beat to blood-pressure. When the blood-pressure is high, not only is the resistance to the ventricular systole increased, but, other things being equal, more blood flows (in the mammalian heart) through the coronary artery. Both these events would increase the activity of the heart, and we might expect that the increase would be manifest in the rate of the rhythm as well as in the force of the individual beats. As a matter of fact, however, we do not find this. On the contrary, as Marey has insisted, the relation of heart-beat to pressure may be put almost in the form of a law, that "the rate of the beat is in inverse ratio to the arterial pressure;" arise of pressure being accompanied by a diminution, and fall of pressure with an increase of the pulse-rate. This however only holds good if the vagi be intact. If these be pre\dously divided, then in whatever way the blood-pressure be raised — whether by injecting blood or clamping the aorta, or increasing the peripheral resistance, through that action of the vaso-motor ner^^ es which we shall have to describe directly — or in whatever way it be lowered, no such clear and decided inverse relation between blood-pressure and pulse rate is observed. It is inferred therefore that increased blood-pressure causes a slowing of the pulse, when the vagi are intact, because the cardio-inhibitory centre in the medulla is thereby stimulated, and the heart in consequence to a certain extent inhibited. F. 13 194 INHIBIT 10 F AND BLOOD-PRESSURE. [Book i. The Effects on the Circulation of Changes in the Heart's Beat. Any variation in tlie heart's beat directly affects the blood- pressure unless some compensating influence be at work. The most extreme case is that of complete inhibition. Thus if, while a tracing of arterial pressure is being taken, the beat of the heart be suddenly arrested, some such curve as that represented in Fig. 43 will be obtained. It will be observed that immediately after the last beat, there is a sudden rapid fall of the blood pressure. — v.^^ Fig. 43. Tracing, shewing the influence of Cardiac Inhibition on Blood-Pkes- STJRE. Proii a Babbit. The current was thrown into the vagus at a and shut off at h. It will be observed that one beat is recorded after the commencement of the stimulation. Then follows a very rapid faU, continuing after the cessation of the stimulus. With the returning beats, the mercury rises by leaps until the normal pressure is regained. At the pulse due to the last systole, the arterial system is at its maximum of distension; forthwith the elastic reaction of the arterial walls propels the blood forward into the veins, and there being no fresh fluid injected from the heart, the fall of the mercury is unbroken, being rapid at first, but slower afterwards, as the elastic force of the arterial walls is more and more used up. With the returning beats, the pressure correspondingly rises in successive leaps until the normal mean pressure is regained. The size of these returning leaps of the mercury may seem dispro- portionately large, but it must be remembered that by far the greater part of the force of the first few strokes of the heart is expended in distending the arterial system, a small portion only of the blood which is ejected into the arteries passing on into the veins. As the arterial presstire rises, more and more blood passes at each beat through the capillaries, and the rise of the pressure at each beat becomes less and less, until at last the whole contents C'llAl'. I\.j THE VASCVLAli MI-JJUAMSM. lo; of the vcutriclo ]);iss at each stroke into tlic veins, and the mean arterial pressure is established. To tliis it may be added, that, as we have seen, the force of the individual ])eats may he soniewhat <:^reater after than before iidiibition. Besides, when the mercury nianoineter is used, the inertia of the mercury tends to magnify tlie ettects of the initial beats. ST(M0L/1T/0N V/tCL/S Fig. 44. Vagus Stimulation. Pulse-tracing from the carotid of rabbit, talien by a modification of tlie siihygmograph. The period of Vagus stimulation is marked by the line below. One beat occurs after stimulation has bcgim. Shews the fall of blood-pressure, and the character of the first recommencing beats. Complete an-est of the heart -beats is not necessary to produce a fall of pressure. As is seen in Fig. 45, mere slowing of the beats will lower the mean pressure. And, speaking generally, we may say \f^vYvw^wm^^h Fig. 45. Stimulation of Vagus. Blood-pressure curve taken with mercury manometer. The effect is to slow the rhythm rather than to bring about complete standstill. With the slow pulse the pressure still continues to fall. The beginning of stimulation is marked by a, that if while the force of the individual beats remains constant the frequency is increased or diminished, and vice versa, if while the 13—2 196 INHIBITION AND BLOOD-PRESSURE. [Book i. frequency remains the same the force is increased or diminished, the result in both cases is that the pressure is proportionately increased or diminished. This clearly must be the case ; but obviously it is quite possible that the beats might, while more frequent, so lose in force, or while less frequent, so increase in force, that no difference in the mean pressure should result. And this indeed is not unfrequently the case. So much so, that variations in the heart- beat must always be looked upon as a far less important factor of blood-pressure than variations in the peripheral resistance. An increase in the quantity of blood ejected at each beat must necessarily augment, and a decrease diminish, the blood-pressure, other things remaining the same. But the quantity sent out at each beat, on the supposition that the ventricle always empties itself at each systole, will depend on the quantity entering into the ventricle during each diastole, and that will be determined by the circumstances not of the heart itself, but of some other part or parts of the body. SEC. 5. CHANGES IN THE CALIBRE OF THE MINUTE ARTERIES. VASO-MOTOR ACTIONS. The middle coat of all arteries contains circularly disposed plain muscular fibres. As the arteries become smaller, the mus- cular element becomes more and more prominent as compared with the elastic element, until, in the minute arteries, the middle coat consists entirely of a series of plain muscular fibres wrapped round the elastic internal coat. Nerve-fibres belonging to the sympathetic system are distributed largely to blood-vessels, but their terminations have not as yet been clearly made out. By galvanic, or still better by mechanical stimulation, this muscular coat may, in the living artery, be made to contract. During this contraction, which has the slow character belonging to the contractions of all plain muscle, the calibre of the vessel is diminished. If the web of a frog's foot be examined under the microscope, any individual small artery will be found to vary in calibre, being sometimes narrowed and sometimes dilated. During the narrowing, which is obviously due to a contraction of the muscular coat of the artery, the attached capillary area and the corresponding veins become less filled with blood, and paler. During the stage of dilation, which corresponds to the relaxation of the muscular coat, the same parts are fuller of blood and redder. It is obvious that, the pressure at the entrance into any given artery remaining the same, more blood will enter the artery when relaxation takes place and consequently the resistance offered by the artery is lessened, and less when contraction occurs and the resistance is consequently increased. The blood always flows in the direction of least resistance. 198 VASO-MOTOR NERVES. [Book i. The small arteries frequently manifest what may be called spontaneous variations in their calibre, and these variations are very apt to take on a distinctly rhythmical character. If a small artery in the web of the frog be carefully watched, it will be seen from time to tinie to vary very considerably in width, without any obvious change taking place in the heart's beat or any events occurring in the general vaso-motor system. Similar variations may be witnessed in the vessels of the mesentery of a mammal. The most striking and most easily observed instance of rhythmical constriction and dilation is to be found in the median artery of the ear of the rabbit. If the ear be held up before the light, it will be seen that at one moment the artery appears as a delicate hardly visible pale streak, the whole ear being at the same time pallid. After a while the artery slowly widens out, becomes thick and red, the whole ear blushing, and many small vessels previously invisible coming into view. Again the artery narrows and the blush fades away; and this may be repeated at somewhat irregular intervals several times a minute. The extent and regularity of the rhythm are usually markedly increased if the rabbit be held up by the ears for a short time previous to the observation. Similar rhj'^thmic variations in the calibre of the arteries have been observed in several places, ex. gr. in the saphena artery of the rabbit, in the axillary artery of the tortoise, and in the small arteries of the muscles of the frog ; probably they are widely spread. They may be compared with the rhythmic movements of the veins in the bat's wing and of the caudal vein of the eel. The extent and intensity of the constriction or dilation which may be observed in the frog's web are found to vary very largely. Irregular variations of slight extent occur even when the animal is apparently subjected to no disturbing causes; while as the result of experimental interference the arteries may become either constricted, in some cases almost to obliteration, or dilated until they acquire double or more than double their normal diameter. This constriction or dilation may be brought about not only by treatment applied directly to the web, but also by changes affecting the nerve of the leg. Thus section of the sciatic nerve is generally followed by a dilation which may be slight or which may be very marked, and which is sometimes preceded by a passing constriction ; wdiile stimulation of the peripheral stump of the divided nerve by an interrupted current of moderate intensity generally gives rise to constriction, often so great as almost to obliterate some of the minute arteries. These facts shew that the contractile elements of the minute arteries of the web of the frog's foot are capable by contraction or relaxation of causing constriction or dilation of the calibre of the arteries ; and that this condition of constriction or dilation may be brought about through the agency of nerves. CuAi'. IV. ] THE VASCULAR MKC llAMSM, 199 Vaso-motor nerves. In Avarm-bluudeJ auiumls, though we cannot readily, as in the frog, watch the circulation under the microscope, we have abundant evidence of tlie influence of the nervous system on the calibre of the arteries. Thus in the mammal, division of the cervical sympathetic on one side of the neck causes a dilation of the minute arteries of the head on the same side, shewn by an increased su])])ly of blood to the parts. If the experiment be performed on a rabbit, the effect on the circulation in the ear is very striking. The whole ear of the side operated on is nmch redder than normal, its arteries are obviously dilated, its veins unusually full, innumerable minute vessels before invisible come into view, and the temperature may be more than a degree higher than on the other side. Division of the sciatic nerve in a mammal causes a similar dilation of the small arteries of the foot and leg. Where the condition of the circulation can be readily examined, as for instance in the hairless balls of the toes, especially when these are not pigmented, the vessels are seen to be dilated and injected; and a thermometer j^laced between the toes shews a rise of temperature amounting, it may be, to several degi'ees. The quantity of blood present in the blood-vessels of the mammal may sometimes be observed directly, but has frequently to be determined indirectly. The temperature of passive structures subject to cooling in- Huencos, such as the skin, is largely dependent on the supply of blood, the more abundant the supply the warmer the part. Hence in these parts variations in the quantity of blood may be inferred from varia- tions of temperature ; but in dealing with more active structures there are obviously sources of error in the possibility of the treatment adopted, such as the stimulation of a nerve, giving rise to an increase of temperature due to increased metabolism, independent of vai'iations in blood supply. The quantity of blood may also be determined by the plethysmograph. In this instrument, a part of the body, such as the arm is introduced into a closed chamber tilled with fluid, ex. gr, a large glass tube, the opening by which the arm is mtroduced being secured with a stout caoutchouc membrane. An increase or decrease of blood sent into the arm will lead to an increase or decrease of the volume of the arm, and this will make itself felt by an increase or diminution of pressure in the fluid of the closed chamber, which may be registered and measured in the usual way. We shall have to speak again of a modification of this instrument when we are dealing with the kidney. Division of the brachial plexus produces a similar dilation of the blood-vessels of the front limb. Division of the splanchnic nerve produces a dilation of the blood-vessels of the intestines and other abdominal viscera. Division in the mammal of the hypo- glossal nerve on one side causes a dilation of the vessels in the corresponding half of the tongue. Division of a nerve supplying a muscle causes a large and sudden increase in the venous flow 200 YASO-MOTOR NERVES. [Book i. from the muscle, indicating that the muscular arteries have become dilated; and in the frog this dilation, consequent on section of the nerve, may be actually observed by placing a thin muscle such as the mylo-hyoid under the microscope, and watching the calibre of the small arteries and the circulation of the blood through them while the nerve is being cut. We find in fact that in almost all parts of the body certain ' vascular areas ' stand in such a relation to certain nerves that the division of one of these nerves causes a dilation of the minute arteries in, and consequently an increased supply of blood to, a corresponding vascular area. We may speak of these nerves as 'vaso-motor' nerves, or more correctly, since in the vast majority of cases the nerves in question have other functions than that of governing arteries, as containing vaso-motor fibres, much in the same way as an ordinary spinal nerve is spoken of as containing sensory and motor fibres ; and from what has been said above it is evident that these vaso-motor fibres are found sometimes in sympathetic, sometimes in cerebro-spinal nerves. Since division of a vaso-motor nerve, or nerve containing vaso- motor fibres, leads to the dilation of the arteries of its appropriate vascular area, it is obvious that previous to that division these arte- ries were in a state of permanent constriction, due to a permanent contraction of their muscular coats. This permanent constriction, which may vary considerably in degree (the dilating effects of section of the vaso-motor nerve correspondingly varying in a- mount), is spoken of as ' tone,' ' arterial tone.' Axteries in such a state of permanent constriction as under ordinary circumstances is normal to arteries whose vaso-motor fibres have not been divided and which are otherwise in a normal condition, are said to ' possess tone.' When, as after division of the vaso-motor fibres, the constric- tion gives place to dilation the arteries are said to have 'lost tone;' and when, under various circumstances which we shall study hereafter, the constriction becomes greater than normal, their tone is said to be increased. A very little consideration will shew that this arterial tone is a most important factor in the circulation. In the first place the whole flow of blood in the body is adapted to and governed by what we may call the general tone of the arteries of the body at large. In a normal condition of the body, if not all, at least the great majority of the minute arteries of the body are in a state of tonic, i.e. of moderate, constriction, and it is the narrowing due to this constriction which forms a large item of that peripheral resistance which we have seen (p. 129) to be one of the two great factors of blood-pressure. The normal general blood-pressure, and therefore the normal flow of blood, is in fact dependent on the 'general tone' of the minute arteries. In the second place, changes in local tone, i.e. the tone of any particular vascular area, have very decided effects on the circulation. These effects are both local and general, as the following considerations will shew. Cii.vi'. IV.] 77/ A" VASCl'LAn }n:(JIAXISM. 201 Lot us sup])oso that the artery ^1 is in a cundition of nonnal tone, is niitlway betwcLMi extreme constriction antl dilation. Tlie How tliruiif(h ^-l is dctcnnintd by the resistance in A and in the vascular tract whicli it supplies, in relation to the mean arterial pressure, which again is dependent on the way in which the heart is beating and on the peripheral resistance of all the small arteries and capillaries, A included. If, while the heart and the rest of the arteries remain unchanged, A be constricted, the peripheral resistance in A will increase, and this increase of resistance will lead to an increase of the general arterial pressure. This increase of pressure will tend to cause the blood in the body at large to How mure rapidly from the arteries into the veins. The con- striction of A however will prevent any increase of the flow through it, in fact will make the flow through it less than before. Hence the whole increase of discharge from the arterial into the venous system must take place through channels other than A. Thus, as the result of the constriction of any artery there occur, (1) diminished flow through the artery itself, (2) increased general arterial pressure, leading to (3) increased flow tlirough the other arteries. If, on the other hand, A be dilated, while the heart and other arteries remain unchanged, the peripheral resistance in ^ is diminished. This leads to a lowering of the general arterial pressure, which in turn causes the blood to flow less rapidly from the arteries into the veins. The dilation of A however permits, even with the lowered pressure, more blood to pass through it than before. Hence the diminished flow tells all the more on the rest of the arteries. Thus, as the result of the dilation of any artery, there occur (1) increased flow of blood through the artery itself, (2) diminished general pressure, and (3) diminished flow through the other arteries. Where the artery thus constricted or dilated is small, the local effect, the diminution or increase of flow through itself, is much more marked than the general effects, the change in blood-pressure and the flow through other arteries. When, however, the area the arteries of which are affected is large, the general effects are very striking. Thus if while a tracing of the blood-pressure is being taken by means of a manometer connected with the carotid artery, the splanchnic nen-es be divided, a conspicuous but steady fall of pressure is observed, very similar to that which is seen in Fig. 46. The section of the splanchnic nen-es causes the mesenteric and other abdominal arteries to dilate, and these being very numerous, a large amount of peripheral resistance is taken away, and the blood-pressure falls accordingly ; a large increase of flow into the portal veins takes place, and the supply of blood to the face, arms, and legs is proportionally diminished. It will be obsen-ed that the dilation of the arteries is not instantaneous but somewhat gradual, the pressure sinking not abruptly but with a gentle curve. Arterial tone then, both general and local, is a powerful 202 VASO-MOTOR NERVES. [Book i. instrument for determining the flow of blood to the various organs and tissues of the body, and thus becomes a means of indirectly influencing their functional activity. We should accordingly ex- pect to find that the vaso-motor nerves were connected with, and arterial tone regulated by, the central nervous system, in order that the calibre of the arteries of, and the supply of blood sent to, this or that vascular area might be varied according to the varying needs of the economy. And experiment proves this to be the case. We stated that section of the cervical sympathetic in the neck causes dilation or loss of tone in the blood-vessels of the head and face. This is true at whatever point of the course of the nerve from the upper to the lower cervical ganglion, both included, the section be made. No such dilation of the vessels of the head and face takes place when the thoracic sympathetic chain is divided anywhere below the upper thoracic ganglion; but dilation does occur after division of certain of the rami communicantes connect- ing the spinal cord with the cervical sympathetic through the lower cervical or upper thoracic ganglion. Hence it is clear that the normal tone of the arteries of the head and face is maintained by influences (whose exact nature we shall study presently) pro- ceeding from the central nervous system, passing through certain rami communicantes (the exact path being somewhat uncertain or possibly not constant) into the cervical sympathetic, and ascending to the head and face by that nerv^e. In other w^ords, the vaso- motor fibres of the vessels of the head and face may be traced down the sympathetic to the lower cervical ganglion, and thence by rami communicantes into the spinal cord. In a similar manner the vaso-motor fibres of the splanchnic nerves governing the mesenteric and other abdominal arteries can also be traced into the spinal cord, as may also those of the sciatic governing the blood-vessels of the hind limb and of the brachial nerves governing those of the fore limb. In fact all the vaso- motor fibres (with certain special exceptions which will be discussed presently) may thus be traced into the spinal cord ; they are all connected with the central nervous system. There is at present some uncertainty in certain cases as to the exact manner in which the fibres pass from the spinal cord to this or that nerve, as, for instance, along which nerve-roots the vaso-motor fibres eventually joining the sciatic trunk run, whether they all pass on their way into the abdominal sympathetic or no, and the like ; but these are questions which need not delay us now; in whichever way they may be settled, they do not affect the important fact that in some way or other all vaso-motor fibres spring from the central nervous system, and that (with certain special exceptions) what we have called the normal tone of the various vascular areas is maintained by influences proceeding from the central nervous system. Far more important however than the maintenance of a normal Ciww IV.] 71/!^ VASCULAR M fX'IIAXTSir. 203 tone, ■wliicli iiuU'cil inijj^lit Lo at once and for ever arranged fur by the ])roper natural calibre of the elastic blood-vessels, is the power which the central nervous system possesses of varyinj^ the tone of this or that artery or f^roup of arteries, of increasing it or of diminishing it, of ])roducing constriction or dilation in those arteries, and thus, as we have seen, of effecting changes in general or local blood-j)ressure or in both, and consequently of determining a ilow of blood in this or that direction, according to the needs of the economy. And the exercise of this carefully arranged manipulation of the muscular walls of the arteries may be called forth in either direction, in the way of constriction, or in the way of dilation (or of both at the same time, one in one area and the other in others), by means of nervous impulses either originating in the central nervous system itself or stalled by afterent impulses passing up to the central nervous system from some sentient surface. BlushinGT is a familiar instance of vascular dilation brought about by the action of the central nervous system. Nervous im- pulses started in some parts of the brain by an emotion produce certain changes in the central nervous system (the exact nature and locality of these changes we shall discuss presently) which have in turn an effect on the vaso-motor fibres of the cervical sympathetic almost exactly the same as that produced by section of the nerve. In consequence the muscular walls of the arteries of the head and face relax, the arteries dilate and the w^hole region becomes suffused. Sometimes an emotion gives rise not to blushing, but to the opposite, viz. to pallor. In a great number of cases this has quite a different cause, being due to a sudden diminution or even temporary arrest of the heart's beats; but in some cases it may occur wdthout any change in the beat of the heart, and is then due to a condition the very converse of that of blushing, that is, to an increased arterial constriction; and this increased con- striction, like the dilation of blushing, is eff"ected through the agency of the central nervous system and the cervical sympathetic. These are familiar examples, but we have in abundance exact experimental evidence of the effect of afferent impulses in inducing through the central nervous system vaso-motor changes and thus bringing about sometimes constriction, sometimes dilation, some- times the two together. The action of the so-called depressor nerve is a striking instance of reflex dilation as it may be called. If in the rabbit while the pressure in an artery such as the carotid is being registered, the depressor nerve, which is a branch of the vagus running alongside the carotid artery and sympathetic nerve (Fig. 41, n. dep.), be divided, and its central end (?'. e. the one connected with the brain) be stimulated with the interrupted current, a gradual but marked fall of pressure in the carotid is observed, lasting, where the period of stimulation is short, some time after the removal of the stimulus (Fig. 46). Since the beat of the heart is not markedly changed, the fall of pressure 204 VA SO -MO TOR NEE VES. [Book r. must be due to the diminutiou of iDeripheral resistance occasioned by the dilation of some arteries. And there is evidence that the /X/X.-V^, "xy^ Fig. 46. TEAcrxo, shewing the Effect on Blood-peessuee of stimulating the CENTBAL END OF THE DePEESSOB NeRYE IN THE EaBBIT. (To be read from right to left. ) T indicates the rate at which the recording surface was travelling ; the intervals marked corresponds to seconds. C the moment at which the current was thrown into the nerve ; the moment at wliicli it was shut off. The effect is some time in developing and lasts after the current has been taken off. The larger undulations are the respii'atory curves ; — the id ulse- oscillations are very small. arteries thus dilated are chiefly if not exchisively those arteries of the abdominal viscera which are governed by the splanchnic nerve. For if both the splanchnic nerves are divided previous to the experiment, the fall of pressure when the depressor is stimulated is very small, in fact almost insignificant. The inference from this is clear ; the afferent impulses passing along the depressor have so affected some part of the central nervous system that the influences which, in a normal condition of things, passing along the splanchnic nerves keep the minute arteries of the abdominal viscera in a state of moderate tonic constriction, fail altogether, and those arteries in consequence dilate just as they do when the splanchnic nerves are divided, the effect being possibly increased by the similar dilation of other smaller vascular areas. The condition of the splanchnic or other vascular areas may moreover be changed, and thus the general blood-pressure modi- lied, by afferent impulses jjassing along other nerves than the depressor, the modification taking on, according to circumstances, the form either of decrease or of increase. Thus, if in an animal (dog) placed under the influence of urari the central stump of the divided sciatic nerve be stimulated, an increase of blood-pressure, almost exactly the reverse of the de- crease brought about by stimulating the depressor, is obsen^ed. Chat, iv] 77//; VAScuLAi: Mi:ciiAXis.\r. 205 Tliu curve of the l^lood-pressure, after a latent period (luring which no chanf,fe.s are visible, rises steadily without any correspondin;^ change in the heart's beat, reaches a maxinmrn and after a whih; slowly falls at^^ain, the fall sometimes beginning to aj)pear before the stimulus has been removed. There can be no doubt that the rise of ])ressure is due to the constriction of certain arteries ; the arteries in question being those of the splanchnic area certaiidy, and possibly of other vascular areas as well. The effect is not confined to the sciatic; stimulation of any nerve containing af- ferent fibres may produce the same rise of pressure, and so constant is the result that the experiment has been made use of as a method for determining the existence of afferent fibres in any given nerve and even the paths of centripetal impulses through the sjunal cord. If, on the other hand, the animal be under not urari but chloral, instead of a rise of blood-pressure a fall, quite similar to that caused by stimulating the depressor, is observed when an afferent nerve is stimulated. The condition of the central nervous system seems to determine whether the reflex effect on the vaso- motor fibres is in the direction of constriction leading to a rise, or of dilation leading to a fall of blood-pressure. Fio. 47. EisE OF Blood-pressure from stimulation of Nostril with smoke. The respiration and cardiac rhythm are at the same time rendered more slow. The mark s indicates the time of stimulation. Stimulation of a sentient surface in many cases causes a similar rise in blood-pressure as shewn in Fig. 47, where a rise of blood - pressure follows irritation of the nostrils. In this case however the rise in blood-pressure is accompanied by changes in respiration and in the cardiac rhvthm. 206 VASO-MOTOR NERVES. [Book i. In the instances just quoted, the effect of the stimulation of the afferent nerve may be spoken of as a general one ; it is the general blood-pressure which is diminished or increased ; though in the case of the depressor at all events it is chiefly in the splanchnic area that the constriction or dilation takes place. There are however some remarkable cases where a local effect can be readily distinguished from the general effect, because the two are in opposite directions. Thus if in a rabbit under urari, the central stump of the auricularis magnus nerve or of the auricularis posterior be stimulated, the rise of general pressure which is caused by the stimulation of this as of any other afferent nerve, is accompanied by a dilation of the artery of the ear. That is to say, the afferent impulses passing along the auricular nerve while affecting the central nervous system in an ordinary way, so as to cause constriction of many of the arteries of the body (but chiefly probably the splanchnic vessels), at the same time so affect some particular part of the central nervous system, more especially connected "s^dth the vaso-motor fibres governing the artery of the ear, as to lead to the dilation of that vessel. So also in the same animal stimulation of branches of the tibial nerve causes dilation of the saphena artery, together with constriction of other arteries, as shewn by the concomitant rise of pressure. And there are probably innumerable instances of the same kind of action going on in the body during life, for it is evident that the object of the local dilation, viz. the increased flow of blood to the organ, must be assisted if a general constriction is at the same time taking place in other regions. The general effect may not always be obvious, may perhaps be absent, so that the local dilation or constriction, as the case may be, is the only obvious result of the vaso-motor action. When the ear of the rabbit is gently tickled, the effect that is seen is a blushing of the ear, and though this may be in part due, as we shall see, to the action of a local mechanism, the case we have just cited shews that the central nervous system must be largely engaged. When the right hand is dipped in cold water, the temperature of the left hand falls, on account of a reflex con- striction of the vessels of the skin of that hand caused by the stimulus applied to the other. Many more instances might be quoted, and we shall again and again come upon examples. The numerous pathological phenomena classed under sympathetic action, such as the affection of one eye by disease in the other, are probably in part at least the results of reflex vaso-motor action. We have said enough to shew that the calibre of the small arteries, which by determining the peripheral resistance forms one important factor regulating the flow of blood, is subject to in- fluences proceeding from all parts of the body, and that these influences reach the arteries in a reflex manner by means of the Chap, iv.l THE VASCl'LAn MIU'IIAXIS.U. 207 conlral nervous system, the afferent ini])nls('s bciii^' for tlio most priil cai'ried by onlinary sensory nerves, while the etil'erent impulses i)ass along special vaso-motor fibres, whieh, though the centre of the rellex action lies in the cerebro-spinal axis, have a great tondency to run in sympathetic tracts. The atlerent impulses of course need not start from the peri- pheral nerve-endings. They may for instance arise in the brain. Thus, as wo have seen, an emotion originating in the cerel^rum may by vaso-motor action give rise either to blusliing or to pallor. Nay more, changes may be induced in the central nervous system itself without the need of any impulses reaching it from without. When we come to discuss the relations of respiration to the circulation, we shall see reason to think that the vaso-motor action of the central nervous s^^stem may be directly ati'ected by the condition of the blood passing through it, so that if the quantity of oxygen in the blood be reduced, a general arterial constriction takes place, and a rise of blood-pressure follows ; while with a retuiTi of oxygen to the blood, the vessels dilate and pressure falls. And it is more than probable that many substances introduced into the blood, or arising in the blood from natural or morbid changes, may affect blood-pressure by acting directly on the centres in the central nervous system. They may also however act on the jDcripheral structures. We shall return to these phenomena later on. In many ways then, and to a varying degree and extent, the central nervous system can bring about arterial constriction or dilation, general or local. We have now to study the question, What is more exactly the nature of the nervous influences which lead to constriction and dilation respectively ? How do those which cause constriction differ from those which cause dilation ? In the fundamental experiment of the cervical S3"mpathetic, when arterial dilation has followed upon section of the nerve, if the perijDheral stump of the divided nerve be stimulated, the dilation gives place to constriction, the blush is replaced by pallor. If the stimulus be veiy strong the constriction is greater than normal, but by carefully adjusting the strength of the stimulus, the cii'culation may be brought to quite a normal condition, the ' loss of tone ' consequent on the severance of the vaso-motor fibres from the central nervous system may be replaced, and not more than replaced, by an artificial tone generated by the action of the stimulus on the sympathetic nerve. The most natural interpreta- tion therefore of the vaso-motor action in this case is to suppose that the nomial tone of the arteries of the face is maintained by 'tonic' constrictive impulses of a certain intensity which pass from the central nervous system along the sympathetic, and that the dilation of the same arteries is due simply to a diminution or absence of these constrictive impulses, an increased constriction or 208 VASO-MOTOR JERVES. [Book i. pallor being similarly due to an increase beyond what is normal of these same impulses. In other words, the nervous influences leading to arterial dilation and constriction differ in degree only, not in kind, and may be considered as being merely jDhases (of decrease or of increase as the case may be) of the same action. And if we turn to the splanchnic nerve we find a similar interpre- tation equally valid. Stimulation of the splanchnic nerv'e causes constriction of the arteries governed by that nerve, apparently because the stimulation supplies artificially the constrictive im- pulses which, so long as the nerve is intact, pass down it from the central nervous system, giving the requisite tone to its vascular area, and the loss of which by division of the nerve gives rise to dilation. So that were we to stop our inquiries at this point, our explanation of vaso-motor action would be very simple. We might speak of constrictive impulses as passing from the central nervous system to the various vascular areas, to such an extent as to constitute normal tone, but as being susceptible either of in- hibition, complete or partial, thus leading to gi-eater or less arterial dilation, or of augmentation, thus leading to excessive con- striction. But this simple view appears insufficient Avhen we push our studies further. In the first place such a conception does not cover all the facts connected even with the two nerves just mentioned. For the dilation or loss of tone which follows upon section of the cervical sympathetic (and the same is true of the splanchnic) is not permanent ; after a while, it may be not until after several days, it may be sooner, the dilation disappears and the arteries regain their usual calibre. This recovery is not due to any regeneration of vaso-motor fibres in the sympathetic, for it may be observed when the whole length of the nerve including the superior cervical ganglion is removed. When recovery of tone has thus taken place, dilation or increased constriction may be occasioned by local treat- ment : the ear may be made to blush or to pale by the application of heat or cold, by gentle stroking or rough handling and the like ; but neither the one nor the other condition can be brought about by the intervention of the central nervous system. So also the spontaneous rhythmic variations in the calibre of the arteries of the ear of which we spoke on p. 198, though they cease for a time after division of the cervical sympathetic, eventually reapj)ear, even if the superior cer\dcal ganglion be removed. And the analogous rhythmic variations of the veins of the bat's wing have been proved experimentally to go on vigorously when all connection with the central nervous system has been severed; they may continue in fact in isolated pieces of the wing. From this it is clear that what we have spoken of as the tone of the vessels of the face, though influenced by and in a measure dependent on the central nervous system, is not simply the result of an effort of that system. The CiiAr. IV.] THE VASCULAR MECHANISM. 209 muscular walls of the arteries arc not mere passive instruments worked by the cercbro-spinal axis through the cerv'ical syinpa- thetic; obviously they have an intrinsic tone of their own, de- })endent possibly on some local nervous inechauism, though in the car at least no such mechanism has yet been found ; and it seems natural to suppose that when the central ner\'ous system causes dilation or constriction of the vessels of the face, it makes use, in so doing, of this intrinsic local tone. But if so, then the simple view entertained above, that arterial dilation and constric- tion are simply determined by the decrease or increase of tonic constrictive impidses passing directly from the central nervous system, is not a comijlete re23resentation of the facts. In the second place, if wc turn from the sympathetic or splanchnic to other nerv^es containing vaso-motor fibres, we meet ^vith still gi-eater difficulties. To take, for instance, a nerve sup- plying a muscle, such as that going, in the frog, to the mylo-hyoid muscle. Here, as in the cervical sympathetic, section of the nerve produces dilation, but that dilation is even more transient than in the case of the sympathetic ; the vessels speedily return to their former calibre. And then it is found that stimulation of whatever strength of the peripheral portion of the divided ner^'e brings about not constriction but dilation. A similar dilation is seen when the nerve of a mammalian muscle is stimulated, and probably occurs in the case of all muscular nerves. There are therefore in the body ners^es, stimulation of which, as w^ell as mere section, always brings about arterial dilation. There are other nerves in the body of a mixed character, intermediate between the cervical sympathetic on the one hand, and the muscular nerves on the other, stimulation producing now constriction, now^ dilation. Such a nerve is the sciatic of a mam- mal. We have already seen that section of this nen'e produces dilation of the vessels of the foot ; but the dilation so caused after a few days disappears ; the foot on the side on which the nerve was divided becomes not only as cool and pale, but frequently cooler and paler than the foot on the sound side. If the peripheral por- tion of the divided nerve be stimulated with an interrupted cmTent, immediately or very shortly after division, the dilation due to the division gives place to constriction ; the sciatic acts then quite like the cervical sympathetic, except perhaps that this artificial con- striction cannot be maintained for so long a time, and is very apt to be followed by increased dilation. If however the stimulation be deferred for some days, until the dilation has given place to a returning constriction, the effect is not constriction but dilation; the nerve then acts, as far as its vaso-motor fibres are concerned, like a muscular nerve and not Kke the cervical sympathetic. In fact, by variations in the attendant circumstances, and in the mode of stimulation, into the details of which we cannot enter now, stimulation of the divided sciatic may at the will of the experi- F. 14 210 , VASO-MOTOR NERVES. [Book i. menter be made to produce either arterial dilation or arterial con- striction. In all the above cases section of the nerve produces dilation, whether the subsequent stimulation causes constriction or dilation; the dilation after section may be sometimes not very marked, but is always present to some extent or other. But there are certain nerves, section of which produces no marked changes in the vascular areas to which they are distributed, and yet stimulation of which brings about dilation often of an extreme character. A striking example of this is seen in the so-called nervi erigentes. The erection of the penis is, putting aside the subsidiary action of muscular bands in restraining the outflow through the veins, chiefly due to the dilation of branches of the pudic arteries, whereby a large quantity of blood is discharged into the venous sinuses. Erection may in the dog be artificially produced by stimulating the peripheral ends of the divided nervi erigentes, which are branches from the first and second and sometimes from the third sacral nerve passing across the pelvis. On applying the interrupted current to the peripheral ends of these nerves, the corpora cavernosa at once become turgid. And yet simple section of these nervi erigentes will not in itself give rise to erection. A similar case is presented by the submaxillary gland. As will be explained more in detail in treating of secretion, this gland is supplied by two nerves, by branches of the chorda tympani reaching it along its duct, and by branches of the cervical sym- pathetic reaching it along its arteries. Neither section of the chorda tympani nor section of the cervical sympathetic produces any very marked effect in the circulation of the gland. Yet stimu- lation of the former will bring about a most striking dilation, of the latter a no less striking constriction, of the arteries of the gland. How can we construct a view of the action of vaso-motor nerves which will be consistent with all these various facts ? In the first place, we must admit the existence of a local tone in the several vascular areas, independent of the central nervous system. In such cases as the corpora cavernosa of the penis, and the submaxillary gland, this independence is umnistakeable ; in other regions it is not at first sight so apparent, but, as we have already urged, must be admitted even for these. In the second place, as is strikingly shewn by the case of the submaxillary gland, there are nerves which, since stimulation of them always causes dilation, may be called vaso-dilator nerves, and nerves which, since stimulation of them always causes constriction, may be called vaso-constrictor nerves. Examples of the first are^ seen in the nervi erigentes, the chorda tympani, the nerves of muscles, &c. ; of the second, in the cervical sympathetic, the splanchnic, &c. Or to be more exact, we may say that the vaso- motor fibres of the former are vaso-dilator, of the latter, vaso-con- strictor. HnAr. IV.] Till-: VASCULAR MECHANISM. 211 In the tliinl ])hice, llic cases of tlic corpora cavernosa of the penis and the submaxillary gland sugt^^cst the idea that dilation is the result of the complete or partial loss of local tone, that in fact vaso-dilators act by iuhibitiiif^, and vaso-constrictors by augmenting, the activity of the local mechanism (whatever it be) which gives rise to the local tone. The erection of the penis which follows stimula- tion of the nervi erigentes, and the injection of the submaxillary gland which follows stimulation of the chorda tympani, present a very close analogy to the inhibition of the heart by stimulation of the vagus. Just as the rhythmic contraction of the cardiac fibre is stopped by the vagus, so th-e tonic contraction of the arterial fibre (and this tonic contraction is indeed at bottom an obscure rhythmic contraction) is stopped by the chorda or the nervi erigentes. And it seems to be very natural to draw the conclusion that dilation is in all cases mere inhibition, and constriction in all cases mere augmen- tation, of local tone. But tempting as this view is, and useful perhaps as it may be as a working hypothesis, it must not be regarded as definitely proved. It is Cjuite possible that dilation may be brought about in different w^ays in different cases ; and so also with con- striction. Further, the occm'rence of dilation after simple section of a nerve raises an interesting question. Do the arteries in such a case dilate because the veiy section of the nerve acts as a stimulus to vaso-dilator fibres, or because the local tone is insufficient to keep up an adequate arterial constriction unless it be supplemented by additional tonic impulses reaching the local mechanism from the central nervous system, which supplement is lost by section of the nerve ? Obviously, if mere section behaves as a stimulus to vaso- dilator fibres of such a potency as to give lise to a dilation lasting hours or it may be days, all evidence of 'tonic' impulses proceeding from the central nervous system is done away with. We can then only speak of dilation and constriction as being the result of the action of vaso-dilator and vaso-constrictor fibres respectively, both worked in a reflex manner by the central nervous system. Into the dis- cussion whether such an interpretation of the effects of simple section is justified by facts or not, and into the allied controversy concerning the reason why the vaso-motor effects of stimulating the efferent fibres of the sciatic and other nerves vary so much under different circumstances, we cannot enter here. We must content ourselves with the general conclusion that though local tone may exist independently of the central nervous system, the condition of the various vascular areas, in the living bod}' in a normal condition, is arranged and modified to meet passing or permanent needs, by the central nervous system, through the agency of vaso-motor nerves, and that these vaso-motor nei'\'es in some cases, since they are used to give rise to dilation only, may be spoken of as vaso-dilator nerves, or as containing vaso-dilator fibres, in other cases may similarly be called vaso-constrictor, and in yet a third class of cases be regarded U— 2 212 VASO-MOTOE CENTRES, [Book i. as mixed in character, since according to circumstances they give rise either to dilation or to constriction. The course of vaso-motor fibres. Leaving out of consideration local vaso-motor mechanisms, such as those which may be sup- posed to exist in the submaxillary gland, we may make the general statement that vaso-motor influences may be traced back to the spinal cord. The exact paths taken by the vaso-motor fibres have not however as yet been fully worked out. Most observers are agreed that the fibres leave the spinal cord by the anterior roots of the spinal nerves; but in the majority of cases at all events as far as the mammal is concerned, the fibres do not run in a direct course to their destination in company with the ordinary motor fibres passing to the same structures as themselves. Thus the vaso-motor fibres of the hind limbs do not pass directly with the anterior roots into the sciatic nerve but, largely at all events, turn aside, to join through the rami communicantes the abdominal sympathetic ; and it is only after they have traversed a certain length of sympathetic nerve that they again return to the spinal nerves, enter into the sciatic plexus, and thus become part of the nerves of the leg. So also the vaso-motor fibres for the forelimb pass in large measure from the anterior roots of the upper dorsal nerves to the thoracic sjnupathetic chain and thence by the first thoracic ganglion to the brachial plexus and so on to the fore- limb. And we have already seen that the vaso-motor fibres for the head and face, pass from the lower cervical or l^^r-dorsal spinal cord to the first thoracic or to the last cervical ganglion and by the cervical sympathetic upwards. When, as in the case of the submaxillary gland, the presence of distinct and antagonistic vaso-constrictor and vaso-dilator nerves is conspicuous in the same organ, the dilator fibres are generally found running in a cerebro-spinal and the constrictor fibres in a sympa- thetic nerve, but we cannot at present say that such a contrast is invariable. We cannot as yet trace out such distinct courses for the dilator and constrictor fibres of either the fore or hind limb ; and in the tongue while dilator fibres run into the lingual nerve, constrictor fibres appear in the hypoglossal which is no less clearly a spinal nerve than the fifth of which the lingual is a branch. Vaso-motor centres. There remains the important question, What part of the central nervous system is it which intermediates as a nervous vaso-motor centre or centres either of purely reflex or of partly reflex and pa^rtly automatic action, between various affer- ent impulses and the efferent vaso-motor impulses leading either to dilation or constriction ? We have seen that stimulation of the central stump of the divided sciatic gives rise, in an animal under urari, to an increase of general blood-pressure, brought about chiefly, if not entirely, by an augmentation of constrictive impulses passing along the splanch- nic nerves. This increase of blood-pressure is manifested, with tA^y^ CiiAr. iv.J THE VASCULAR MECHAXISM. 213 (in satisfactory exporimcnts) undimiiiisliod inttinsity, even wlien the whole of the brain, down to a certain limit in the medulla oblon^^ata, has been removed. But it" the removal be carrietl beyond this limit, or if a small area of the medulla oblongata lying above the calamus scriptorius be removed, the effect on the general blood- prcssm-e of stimulating the central stump of the sciatic — we might add, of any otlier aftcrcut nerve — is comparatively insignificant. The simi>k'st view to take of these facts is to suppose that this small portion of the medulla oblongata acts as a vaso-motor centre, by the action of which ordinary afferent impulses coming from the sciatic or any other afferent ner\'e, arc transformed into vaso-motor impulses of constrictive (or as in the case of an animal under chloral, of dilating) effect and so discharged along the splanchnic nerves. The lower limit of this region -which wc may call the medullary vaso-motor centre has been placed in the rabbit at a horizontal line drawn about 4 or 5 mm. above the point of the calamus scriptorius, and the upper limit at about 4mm. higher up, i.e. about 1 or 2 mm. below^ the corpora quadrigemina. When trans- verse sections of the brain are cai'iied successively lower and lower down, an effect on blood-j)ressure in the way of lowering it and also of diminishing the rise of blood-pressure resulting from stimulation of the sciatic, is first obsen-ed when the upper limit is reached. On carrying the sections still lower, the effect of stimulating the sciatic becomes less and less, until when the lower limit is reached no effects at all are observ'ed. The centre appears to be bilateral, the halves being placed not in the middle line but more sideways and rather nearer the anterior than the posterior surface. It may perhaps be more closely defined as a small prismatic space in the forward prolongation of the lateral columns after they have given off their fibres to the decussating pyramids. This space is largely occupied by a mass of gi^ey matter, called by Clarke the antero-lateral nucleus, and containing large multipolar cells. Whether this medullary vaso-motor centre has any distinct automatic action, whether it may be regarded as continually gene- rating out of its own molecular oscillations, and discharging along the vaso-motor fibres, impulses whereby the general arterial tone is maintained, is a question w^hich, like the allied question mooted on p. 188, need not be discussed here. Granting even the existence of such automatic functions, they must be of secondary importance. As w^e have already urged, the great use of the whole vaso-motor system is not to maintain a general arterial tone, but to modify according to the needs of the economy the condition of this or that vascular area. The impulses passing down the vaso-motor fibres of the cervical sympathetic and of many other nerves may similarly be traced back to this same reerion of the medulla oblongata. Whether all vaso- 214 YASO-MOTOR CENTRES, [Book i. motor fibres are actually in functional connection with it may perhaps be doubted; but at all events the fibres passing to so many vascular areas, and those of such magnitude and importance, are by means of it brought into functional relationship with so many afferent nerves of the body, that it may fairly be spoken of as the general vaso-motor centre. But the use of this phrase must not be understood to imply that this small portion of the medulla oblongata is the only part of the central nervous system which can act as a vaso-motor centre. In the frog reflex vaso-motor effects may be obtained by stimu- lating various afferent nerves after the whole medulla has been removed, and indeed even when only a comjDaratively small portion of the spinal cord has been left intact and connected, on the one hand, with the afferent nerve which is being stimulated and, on the other, with the efferent nerves in which run the vaso-fibres v>'hose action is being studied. In the mammal such effects do not so readily appear, but may with care and under special conditions be obtained. Thus in the dog, when the spinal cord is divided in the dorsal region, the arteries of the hind limbs and hinder part of the body become dilated. This one Vv^ould naturally expect as the result of their severance from the general medullary vaso-motor centre. But if the animal be kept in good condition for some time, a normal or nearly normal arterial tone is after a while re-esta- blished ; and the tone thus regained may be modified in the direc- tion certainly of dilation, and possibly, l3ut this is by no means so certain, of constriction by afferent impulses reaching the lumbar cord. Erection of the penis through the nervi erigentes may then be still brought about by suitable stimulation of sensory surfaces, and dilation of various vessels of the limbs readily produced by stimulation of the central stump of one or another nerve. These remarkable results, which though they are most striking in connection with the lumbar cord hold good apparently for the dorsal cord also and indeed for all parts of the spinal cord, naturally suggest a doubt whether the explanation just given above of the effects of section of the medulla oblongata, is a valid one. When we come to study the central nervous system, we shall again and again see that the immediate effect of operative interference with these delicate structures is a temporary suspension of nearly all their functions. This is often spoken of as ' shock ' and may be regarded as an extreme form of inhibition. And the question may fairly be put whether the effects of cutting and injuring the structures which we have spoken of as the medullary vaso-motor centre, are not in reality simply those of shock. The case of the dog with the divided dorsal cord, and other similar cases, clearly prove that parts of the spinal cord, other than the particular region of the medulla oblongata of which we are speaking, may act as vaso-motor centres. And we may very fairly at least put forward the view, that the vascular dilation which follows upon CiiAP. iv.J THE VASCULAR MKClIAyiSM. 215 sections of the so-called medullary vaso-motor centre, comes about because section of or injury to this region exercises a strong iidiibitory intluenee on all the vaso-niotor centres situated in the spinal cord below. Owing to the special function of the medulla oblongata in carrying on the all-important work of respiration, a mammal whose medulla has been divided cannot be kept alive for any length of time. Wo cannot therefore put the matter to the simple experimental test of extirpating the supposed medullary vaso-motor centre and seeing what happens when the animal has completely recovered from the effects of the operation : we have to be guided in our decision by more or less indirect arguments. We must not attempt to discuss the matter fully here, but may say that, after all due weight has been attached to the play of inhibitory impulses, there still remains a balance of evidence in favour of the view that the region of the medulla of which we are speaking does act as a general vaso-motor centre. It is not however to be regarded as the .single vaso-motor centre, whither afferent impulses from all parts of the body must always travel before they can start vaso- motor impulses along this or that nerve. We are rather to suppose that the spinal cord along its whole length, contains, interlaced with the reflex and other mechanisms by which the skeletal muscles are governed, vaso-motor centres and mechanisms of varied com- plexity, the details of whose functions and topography have yet largely to be worked out. As in the absence of the sinus venosus the auricles and ventricle of the frog's heart may still continue to beat, so in the absence of the medulla oblongata, these spinal vaso- motor centres provide for the vascular emergencies which arise. As however in the normal entire frog's heart, the sinus, so to speak, gives the word and governs the work of the whole organ, so the medullary vaso-motor centre rules and co-ordinates the lesser centres of the cord, and through them presides over the chief vascular areas of the body. It is possible moreover that the me- dullary centre is specially connected with the splanchnic nerves and thus with the capacious vascular area of the abdominal viscera, and in consequence possesses an additional importance. By means of these vaso-motor central mechanisms, by means of the head centre in the medulla, and the subsidiary centres in the spinal cord, the delicate machinery of the circulation, which determines the blood supply, and so the activity of each tissue and organ, is able to respond by narrowing or widening arteries to the ever-varying demands and to meet by compensating changes the shocks and strains of daily life. Vaso-motor nerves of the Veins. Although the veins are provided with muscular fibres, and are distinctly contractile and although rhythmic variations of calibre due to contractions may be seen in the great veins opening into the heart, in the veins of 216 VASCULAR CONSTRICTION AND DILATION. [Book i. the bat's wing, and elsewhere, and similar rhytlimic variations, also possibly due to active rhythmic contractions, but possibly also of an entirely passive nature, have been observed in the portal veins, very little is known of any nervous arrangements governing the veins. When in the frog the brain and spinal cord are destroyed, very little blood comes back to the heart as compared with the normal supply, and the heart in consequence appears almost blood- less and beats feebly. This has been interpreted as indicating the existence of a normal tone in the veins dependent on the central nervous system. When the latter is destroyed, the veins become abnormally distended and a large quantity of blood becomes lodged and hidden as it were in them. The Effects of Local Vascular Constriction or Dilation. Whatever be determined ultimately to be the modus oj^erandi of vaso-motor mechanisms, the following fundamental facts remain of prime importance. The tone of any given vascular area may be altered, positively in the direction of augmentation (constriction), or negatively in the way of inhibition (dilation), quite independently of what is going on in other areas. The change may be brought about by (1) a stimulus applied to the spot itself, and acting either directly on some local mechanism, or indu-ectly by reflex action through the general central nervous system ; (2) by a stimulus applied to some other sentient surface, and acting by reflex action through the central nervous system ; (3) by a stimulus (chemical, arising in or carried by the blood) acting directly on the central nervous system; (4) by some part of the central nervous system acting on the vaso- motor centre, as in emotions. The effects of local dilation are local and general. The local effects are as follows. The arteries in the area being dilated, offer less resistance than before to the passage of blood. Consequently, more blood than usual passes through them, filling up the capillaries and distending the veins. Owing to the diminu- tion of the resistance, the fall of pressure in passing from the arteries to the veins will be less marked than usual ; that in the small arteries themselves will be lowered ; that in the corresponding veins heightened. The lowering of the pressure in the arteries means that their elastic coats are not put to the stretch as much as usual ; i.e. their elasticity is not called into play to the same extent as before. Now, as has been seen, every portion of the arterial wall has its share in destroying the pulse by converting the Chap. lY.] THE VASC'l'LAR MJ:CnAXIS}r. 217 intorniittcnt into a continuous flow, rienco, tho dilated arteries, their elasticity not bein(( called into jjlay so much as before, will not contribute their usual share towards destroying the ptdsations which reach them at the cardiac side. The ])ulsations will travel thniu(,di them less chanj^fed than before, and may, in certain cases, j)ass rii^dit on into the veins. This is frefiuently seen in tho sub- maxillary gland, when the chorda tympani is stimulated. The channels being wider, resistance being less, and the force of the heart behind remaining the same, more blood than before passes through the area in a given time ; or, put diflierently, the same quantity of blood passes through the area in a shorter time. The blood, consequently, as it passes into the veins is less changed than in the normal condition of the area. Usually the flow is so rapid that the oxy-hffimoglobin of the corpuscles is deoxidised to a much less extent than usual, and the venous blood still possesses an arterial hue. On the other hand, since more blood passes in a given time, there is an opportunity for an increase in the total interchange between the blood and the tissue. Thus the total work may be greater, though the share borne by each quantity of blood is less. The general effects of dilation are briefly these. Supposing that the total quantity of blood issuing from the ventricle remains the same, that is to say, supposing that the quantity of blood put into circulation is constant, the sui^plus passing through the dilated area must be taken away from the rest of the circulation. Con- sequently the fulness of the dilated area wtlII lead to an emptying of the other areas. This is seen very clearly when the dilated area is a capacious one. At the same time, local dilation causes a local diminution of peripheral resistance. This in turn causes a lower- ing of the general arterial pressure ; to this we have already called attention. The effects of local constriction, similarly local and general, are naturally the reverse of those of dilation. In the vascular area directly affected, less blood passes through the capillaries in a given time, and in consequence less total interchange between the blood and the tissues takes place, though each unit volume of blood which does pass through is more deeply affected. The blood-pressure in the corresponding arteries is increased, and, if the area be large, tho pressure in even distant arteries may be heightened. Thus, to indicate results in a general manner, local dilation en- courages a copious flow of blood through the area where the dilation is taking place, and, by reducing the blood-pressure, hinders the flow of blood into other areas. Local constriction, on the other hand, lessens the flow of blood in the particular area, and by heightening the blood-pressure tends to throw the mass of the blood on to other areas. Hence the great regidative value of the vaso-motor system. By augmenting or inhibitory influences (con- strictor or dilating) applied either to peripheral mechanisms or to 218 VASCULAR CONSTRICTION AND DILATIOX. [Book i. cerebro-spinal centres, and called forth by stimuli either intrinsic and acting through the blood, or extrinsic and acting through nervous tracts, the supply of blood to this or that organ or tissue may be increased or reduced : the surplus or deficit being carried away to, or brought up from, either the rest of the body generally or some other special organ or tissue. SEC. C. CHANGES IN THE CAPILLARY DISTRICTS. We have already seen (p. 116) that the capillary channels vary very much in width from time to time ; but the capillaries do not, like the arteries, jDossess a distinct muscular coat, and the mechanism by which they are brought now to a dilated now to a constricted condition has not been worked out so thoroughly as in the case of the arteries. On the one hand there can be no doubt that the changes in their calibre are in part of a passive nature. They are expanded when a large supply of blood reaches them through the supplying arteries, and, by virtue of their elasticity, shrink again when the supply is lessened or withdrawn. On the other hand there is an increasing amount of evidence that the capillary walls are really contractile. The constituent epithelioid cells have been seen to change their form under the inflvience of stimuli ; and there is much reason for believing that the calibre of a capillary canal may var}', quite independently of the arterial supply or the venous outflow, in consequence of changes in form of the epithelioid cells, allied to the changes in a muscle- fibre or muscle-cell which constitute a contraction. Though the matter requires further investigation, it is probable that these active changes play an important part in determining the quant it}'' of blood passing through a capillary area ; but there is as yet no evidence that they, like the coiTesponding changes in the arteries, are governed by the nervous system. Over and above these changes of form, the capillaries and minute vessels also possess other active properties, which cause them to play an important part in the work of the circulation. They are concerned in assisting to maintain a vital equilibrium between the intra-vascular blood and the extra-vascular tissue, an 220 CHANGES IN THE CAPILLARIES. [Book r. equilibrium which is the central fact of a normal capillary circula- tion, of a normal interchange between the blood and the tissue, and thus of a normal life of the tissue. The existence of this equi- librium is best shewn when it is overthrown or modified, as in inflammation and allied conditions. If an irritant, such as a drop of chloroform or a little diluted oil of mustard, be applied to a small portion of a frog's web, a frog's tongue, or some other transparent tissue, the following changes may be observed under the microscope. The first effect that is noticed is a dilation of the arteries, accompanied by a quickening of the stream. The capillaries become filled with corpuscles, and many passages, previously invisible or nearly so on account of their con- taining no corpuscles, novtf" come into view. The veins at the same time appear enlarged and full. The increase of width is most marked in the arteries, next so in the veins, and least of all in the capillaries. If the stimulus be very slight, this may all pass away, the arteries gaining their normal constriction, and the capil- laries and veins returning to theu' normal condition ; in other words, the effect of the stimulus in such a case is simply a tem- porary blush. Unless however the chloroform or mustard be applied with especial care the effects are much more profound and lasting. In the case of the frog's web a condition is set up known under the name of stasis. This has been considered as merely a phase of in- flammation, since in the frog's v^eb in which inflammation has been largely studied, the agents which produce inflammation frequently produce stasis. But in the frog's tongue and elsewhere true inflam- mation may be set up and produce all its results without any stasis making its appearance ; and though the two conditions are in several respects similar, they appear to be distinct: stasis being the result of the profounder action of the irritant and the forerunner of local death or necrosis. It is this stasis which particularly illustrates the points to which we wish to call attention. Y/hen as the result of the irritant, the initial blush passes into stasis, the following events may be observed. The quickening of the stream gives way to a slackening; this is not due to any returning constriction of the arteries, for they still continue dilated. It will further be observed that the red corpuscles, instead of being in the larger capillaries and smaller arteries and veins confined to the axial stream, are diffiised and indeed crowded over the whole vndth of the channels. The capillaries and veins get more and more crowded with corpuscles, the white corpuscles being scattered UTegularly among the more numerous red ones ; and though the channels get wider and wider, becoming frequently even enormously distended, the stream becomes slower and slower, until at last the movement of the blood in the affected area ceases altogether. The phase of accelerated flow has given place to stasis. The capillaries, veins and small arteries are choked with corpuscles, and it may now be remarked that the red corpuscles seem to run Chap, iv.] THE VASCULAR MICCIIAXISM. 221 to^C,fetlier, so that their outlines arc no l()n;(er (li.stinpfuisliablc; they aj)pcar to have become fused into a homogeneous mass. Kxcejit in cases where the stimulus proiluees permanent mischief, this peculiar condition after a while subsides. The outlines of the corpuscles become once more distinct, those on the venous side of the block gradually drop awa}' into the ucighbouring currents, little by little the whole obstruction is removed, the current through the area is re-established, and though the arteries and capillaries remaiu dilated for some considerable time, they eventually return to their normal calibre. The stasis, the arrest of the current hero seen, is not due to any lessening of the heart's beat; the arterial pulsations, or at least the arterial flow, may be seen to be continued down to the affected area, and there to cease very suddenly. It is not due to any increase of peripheral resistance caused by constriction of the small arteries, for these continue dilated rather than constricted. It must therefore be due to some new and unusual resistance occurrino- in the capillary area itself. The increase of resistance is not caused by any change confined to the corpuscles themselves ; for if after a temporary delay one set of corpuscles has managed to pass away from the affected area, the next set of corpuscles is subjected to the same delay and the same apparent fusion. The cause of the resist- ance must therefore lie in the capillary walls, or in the tissue of Avhich they form a part. We are driven to conclude that the walls of the capillaries (and of the other vessels) exert in health a certain attraction on the corpuscles, maintain a certain adhesiveness between them and themselves, thereby determining the normal flow, with its axial stream and plasmatic layer, and offering a normal resistance to the pressure of the arterial system; and that, in stasis, for reasons which we cannot as yet explain, this attraction, this adhesiveness is largely and progressively increased. Hence the early disappearance of the distinction between the axial stream and plasmatic layer, the tarrying of the corpuscles in spite of the widen- ing of theu^ path, and finally their agglomeration and fusion in the even enormously distended channels. That the increased adhesion is due to the vascular walls and not primarily to the cor[Dusclcs themselves is further shewn by the fact that if in the frog, an artificial blood of normal saline solution to which milk has been added be substituted for normal blood, a stasis may by initants be induced in which oil-globules play the part of corpuscles, and by their aggregation bring about an arrest of the flow through the capillaries. In true inflammation the course of events is different. The vessels become dilated, but the loss of distinction between the axial stream and the jDlasmatic layer does not occur. On the contrary the plasmatic layer appears even more striking on account of the large number of white corpuscles which gather in it and become adherent to the inner surface of the walls of the veins and venous 222 CHAXGES IX THE CAPILLARIES. [Book i. capillaries. In the normal circulation only a few white corpuscles are from time to time seen in this situation slowly moving on in jerks ; but now the walls of the veins seem to be more and more thickly lined with white corpuscles, which are at first com- pletely stationary. At the same time white corpuscles become also very abundant in the capillaries. Very soon these white corpuscles may be seen, either through stomata at the junctions of the epithelioid cells forming the lining of the vessels, or by temporary breaches which are rapidly repaired, making their way through the walls of the veins and capillaries, and escaping into the surrounding tissues. Through the walls of the capillaries and smaller veinleis, red coi-puscles pass as well as white. And this takes place to such an extent that very soon the tissue around the veins and capillaries becomes crowded with white corpuscles, and to a less extent "svith red corpuscles which have made their way out of the vessels. At the same time a large quantity of coagulable lymph, which since it appears also to have passed from the blood- stream through the walls of the blood-vessels is spoken of as exu- dation, makes its appearance in the interstices of the inflamed tissue. While however these changes are going on there is not, as in stasis, a delay and final arrest of the blood-stream. On the contrar}^ the flow through the Avidened channels continues during the whole time to remain accelerated. By comparing the outflow from the veins of the inflamed foot of a dog, with the outflow from the veins of the healthy foot, it has been ascertained that a larger quantity of blood passes through the inflamed foot than through the healthy foot in the same time. We must not however pursue this subject of inflammation any further. We have simply brought it forward as affording another illustration of the action of the walls of the blood-vessels; for, though the matter is perhaps not definitely settled, it seems pro- bable that the aggTegation, in inflammation, of the white corpuscles upon the lining surface of the vessels is due to a special attraction which the blood-vessels exert on the white corpuscles, vdthout pro- ducing that general adhesion of all the corpuscles which is the mark of stasis, and that the migration of the corpuscles is also at least facilitated by similar intrinsic changes in the vascular walls. We cannot say at present whether the vascular walls are also capable of modif}dng the passage of the fluid parts as distrag-uished from the corpuscular elements of the blood, though we know by experiment that the flow of fluid through capillary tubes may be modified on the one hand by changes in the substance of which the tubes are composed, and on the other hand by changes iu the chemical nature (even independent of the specific gravity) of the fluid which is used. We have said enough to shew that the peri- pheral resistance in the capillaries (and consequently all that depends on that peripheral resistance) is not merely a matter of the mechani- cal friction of the blood arainst the smooth walls of the blood-vessels, CiiAi'. iv.J rilE VASCULAR M IX'IIA X ISM. 223 but is concerned with the vital condition of the tissues. Wlien the tissue is in health, a certain resistance is offered to the passage of blood through the capillaries, and the whole vascular mechanism is adapted to overcome this resistance to such an extent that a normal circulation can take place. When the tissue becomes affected, the disturbance of the equilibrium between the tissue and the blood may as in inflammation so modify the flow as to lead to the abnormal escape from the blood of various constituents, or as in stasis so augment the resistance that the passage of the blood becomes difficult or impossible. And it is quite open to us to suppose tliat there are conditions the reverse of stasis, in which the resistance may be lowered below the normal, and the circulation in the area quickened. Thus the vital condition of the tissue becomes a factor in the maintenance of the circulation ; and it is possible, though not yet proved, that these vital conditions are directly under the dominion of the nervous system. It is perhaps hardly necessary to observe that the considerations urged above are quite distinct from what is sometimes spoken of under the name of 'capillary' force, as an agent of the circulation. If by capUlary force it is intended to refer to the rise of fluids in capillary tubes, it is e^"ident that since such phenomena are the results of adhesion, capillarity can only be a greater or less hindrance to the flow of blood, seeing that this is propelled by a force (the heart's beat) which has been proved by experiment to be equal to the task of dri%-ing the blood from ventricle to auricle through the capillary regions. If by capdlary force it is meant that the tissues have some vital power of withdrawing the fluid parts of the blood from the small arteries and thus of assisting an onward flow, it becomes necessary also to assume that they have as well the power of returning the fluid parts to the veins. Both these assumptions are imnecessary and without foundation. SEC. 7. CHANGES IN THE QUANTITY OF BLOOD. In an artificial scheme, changes in the total quantity of fluid in circulation will have an immediate and direct eftect on the arterial pressure, increase of the quantity heightening and decrease diminishing it. This effect will be produced partly by the pump being more or less filled at each stroke, and partly by the j)eri- pheral resistance being increased or diminished by the greater or less fulness of the small peripheral channels. The venous pressure will under all circumstances be raised with the increase of fiuid, but the arterial pressure will be raised in proportion only so long as the elastic walls of the arterial tubes are able to exert their elasticity. In the natural circulation, the direct results of change of quan- tity are obscured by compensatory arrangements. Thus experi- ment shews that v/hen an animal with normal blood-pressure is bled from one carotid, the pressure in the other carotid sinks so long as the bleeding is going on^ and remains deioressed for a brief period after the bleeding has ceased. In a short time how- ever it regains or nearly regains the normal height. This recovery of blood-pressure, after haemorrhage, is witnessed so long as the loss of blood does not amount to more than about 3 per cent, of 1 Chiefly in consequence of free opening in tlie vessel from wlaicli the bleeding is going on, cutting oH a great deal of the peripheral resistance, and so leading to a general loweiing of the blood-pressure. Chap, iv.] TIIK VASCULAR MECIIAKIHM. 225 the Ixnly-weight. Bovoiul lli.il, a lurj^^' ;iii(l IVcipiciilly :i sudilcn (liinLTfrous jxTUKiiu'iit dfjUH'Ssioii is obsrrvi'd. Tlio R'stonition ot" the jiressure after the cessation of thn bleedin*,' is too r;i|)id to peniiit lis to snp))ose that tlie (luaiitity of thiiil ill the blootl-vessels is repaired by tlie withdrawal of lyiiijili from the extra-vaseiilar elements of the tissues. In all probability the result is gained by an increased action of the vaso-motor nerves, increasing the peri|)heral resistance, the vaso-motor centres being tlirown into increased action by the diminution of th