Columbia mtttbmftp X ^ N A- (Mlwjr of piigHtrianH attJn ^nrgpflna lepartment of ptjgBtologg •flJurrtjajarti bg ttft ••«• WORKS OF PROFESSOR J. A. MANDEL PUBLISHED BY JOHN WILEY & SONS, INC. TRANSLATIONS A Text-book of Physiological Chemistry. By Olof Hammarsten, Emeritus Professor of Medi- cal and Physiological Chemistry in the University of Upsala, with the Collaboration of S. C. Hedin, Professor of Medical and Physiological Chemistry in the University of Upsala. Authorized translation from the Author's enlarged and revised 8th German edition, by John A. Mandel, Sc.D., Professor of Chemistry in the New York University and Bellevue Hospital Medical College. viii+1026 pages. 6 by 9. Cloth, $4.00 net. A Compendium of Chemistry, Including General, Inorganic, and Organic Chemistry. By Dr. Carl Arnold, Professor of Chemistry in the Royal Veterinary School of Hannover. Authorized translation from the eleventh enlarged and revised German edition, by John A. Mandel, Sc.D. xii + 627 pages. 51 by 8. Cloth, $3.00 net. A TEXT-BOOK OF PHYSIOLOGICAL CHEMISTS! BY OLOF HAMMARSTEN EMERITUS PROFESSOR OP MEDICAL AND PHYSIOLOGICAL CHEMISTRY~IN THE UNIVERSITY OP UPSALA WITH THE COLLABORATION OF S. G. HEDIN PROPE890R OP MEDICAL AND PHYSIOLOGICAL CHEMISTRY IN THE UNIVERSITY OP UPSALA JVutljoriseb translation FROM THE A UTHOR'S ENLARGED AND REVISED EIGHTH GERMAN EDITION BY JOHN A. MANDEL, ScD. PBOPE8SOR OP CHEMISTRY IN THE NEW YORK UNIVERSITY AND BELLEVUE HOSPITAL MEDICAL COLLSGX SEVENTH EDITION TOTAL ISSUE, THIRTEEN" THOUSAND NEW YORK JOHN WILEY & SONS, Inc. London: CHAPMAN & HALL, Limited Copyright. 1893. 1898, 1900, 1904, 1908, 1911, 1914, BY JOHN A. MANDEL ¥¥ \3\A- PRISB or BRAUNWORTH l CO. BOOK MANUFACTURER* BROOKLYN, N. V. PREFACE TO THE EIGHTH GERMAN EDITION The revision of this edition has been accomplished with the collabora- tion of Professor S. G. Hedin, and the work has been divided so that Hedin has revised Chapters I, III, VIII, XII and XVI, besides the Index of Authors, while Hammarsten has revised Chapters II, IV, V, VI, VII, IX, X, XI, XIII, XIV, XV, and XVII, besides the General Index. The numerous recent developments in physiological chemistry have made a thorough revision and reconstruction necessary in all the chapters, and in order to prevent a noticeable increase in the size of the work, it was also necessary to change the arrangement of the foot-notes more economically The number of chapters in this edition is XVII instead of XVIII as in the seventh edition, because for several reasons it was found advisable to combine the first two chapters of the seventh edition into one chapter, and at the same time certain parts of the first chapter have been incorporated into other chapters, thus for example the oxidation processes have been introduced into Chapter XVI (on respiration and oxidation). In general the plan of the work remains unchanged. Olof Hammarsten. Upsala, September, 1913. iii TRANSLATOR'S PREFACE TO THE SEVENTH AMERICAN EDITION Workers in Biochemistry are to be congratulated on the appearance of a new edition of Hammarsten's " Physiologischen Chemie." At this time, when so many new and important biochemical facts are being published and when so many older theories and deductions are found more or less erroneous, due to recent investigations using, new methods, it is very fortunate that we have this complete and critical compilation from the master hand of Professor Hammarsten, now in his 73d year. We all owe him a great debt of gratitude for his painstaking work for so many years. I take great pleasure in expressing my indebtedness to my assistant, Dr. A. O. Gettler, for the help he has given me in revising the proof and for making the Indexes. John A. Mandel. New York, June, 1914. v CONTENTS CHAPTER I PAGE General and Physico-chemical 1 CHAPTER II The Proteins 77 CHAPTER III The Carbohydrates 196 CHAPTER IV Animal Fats and Phosphatides 232 CHAPTER V The Blood 250 CHAPTER VI Chyle, Lymph, Transudates and Exudates 345 CHAPTER VII The Liver 381 CHAPTER VIII PlGESTION , 451 vii Tin CONTENTS. CHAPTER IX PAGE Tissues of the Connective Substance 514 CHAPTER X The Muscles 565 CHAPTER XI Brain and Nerves 604 CHAPTER XII Organs of Generation 620 CHAPTER XIII The Milk 643 CHAPTER XIV The Urine 672 CHAPTER XV The Skin and its Secretions 837 CHAPTER XVI Respiration and Oxidation 850 CHAPTER XVII Metabolism 878 Index to Authors 945 General Index 983 PHYSIOLOGICAL CHEMISTRY. CHAPTER I. GENERAL AND PHYSICO-CHEMICAL. I. OSMOTIC PRESSURE. When certain substances are placed in contact with water they dissolve therein and finally a liquid is obtained which contains an equal quantity of the dissolved substance in each unit volume. There exists between the water and the soluble body a certain attractive force. Upon this force depends also the so-called diffusion, which manifests itself when two different solutions of the same or different substances are brought into immediate contact with each other. The dissolved molecules and the water intermingle with each other so that finally the dissolved bodies are equally divided in the entire quantity of water. Imagine a cane-sugar solution in contact with pure water; the equilibrium or the homogeneity of the system can then be brought about in two ways; namely, the sugar molecule can migrate in part into the water, and sec- ondly, the water can pass into the solution. If the two fluids at the beginning are in immediate contact with each other then the two proc- esses take place simultaneously. The conditions change when the two liquids are separated from each other by a membrane, which allows of the passage of water but not of the dissolved substance (in this case cane-sugar) . In the presence of such a so-called semipermeable membrane the equilibrium can only be established by the water passing into the cane-sugar solution. Semi- permeable membranes have been artificially prepared, and they also occur in nature, or conditions exist which give results like those of the membranes. To the first group belong Tratjbe's so-called precipitation membranes. 1 Such a membrane, for example can be produced by care- fully dropping a concentrated solution of copper sulphate into a dilute 1 Arch. f. (Anat. u.) Physiol., 1867, pages 87 and 129. 2 GENERAL AND PHYSICO-CHEMICAL. solution of potassium ferrocyanide. Thereby the drop of copper sulphate is surrounded by a membrane of copper ferrocyanide, which is imper- vious to copper sulphate as well as to potassium ferrocyanide, but allows water to pass. The drops retain their blue color in the yellow solution but increase in volume, due to the taking up of water, until the tension of the membrane prevents the further increase in size. If the difference in concentration of the two solutions is great enough, the membrane is ruptured by the pressure. In order to give the copper-ferrocyanide membrane a greater rigidity, Pfeffer has suggested forming the precipitate on a porous, rigid wall. 1 For this purpose he makes use of a small, porous earthenware cell which, after careful cleaning, is treated with copper sulphate and potassium ferrocyanide so that the membrane is precipitated on the inner wall of the cell. The membrane thus obtained is impervious to the cane- sugar. If the cell is filled with a cane-sugar solution and then placed in pure water, no sugar leaves the cell, while water passes into the cell, and this continues until the opposite pressure produced prevents the further passage of water. If the cell is completely closed and in. con- nection with a manometer, then on the establishment of an equilibrium the manometer indicates the force with which the inclosed solution attracts water. As the sugar is attracted with the same force by the water as the water is by the sugar and also as the sugar cannot pass through the membrane therefore the sugar exerts a pressure upon the membrane equal to the pressure indicated by the manometer. This pressure is called the osmotic pressure of the enclosed solution. For dilute cane-sugar solutions Pfeffer's determinations show that the osmotic pressure is approx- imately proportional to the concentration and slowly rises with the temperature. Experiments with other semipermeable membranes have also been carried out by de Vries, and these will be discussed on page 5. De Vries' experiments have led to the following result: Solutions of analo- gously constructed bodies having the same molecular concentration give the same osmotic pressure. Van't Hoff first called attention to the analogy which exists between the laws of osmotic pressure of a dissolved substance and of gases, 2 namely, that the osmotic pressure is proportional (or inversely propor- tional to the volume of the solution) to the concentration, and corre- sponds completely with Boyle-Mariotte's law on the relation between the volume and pressure of gases. Also, that equimolecular solutions 1 Osmotische Untersuchungen, Leipzig, 1877. 2 Zeitschr. f. physik. Chem., 1, 481 (1887). OSMOTIC PRESSURE. 3 have the same osmotic pressure, corresponds to Avogadro's law, that equal volumes of different gases under the same pressure contain the same number of molecules. From Pfeffer's results of the osmotic pressure of cane-sugar solu- tions van't Hoff has calculated that it is the same as the pressure exerted by any gas of the same molecular concentration and temperature. In general the following is true: Dissolved bodies exert in solution the same osmotic pressure they would exert if they were gases at the same temperature and in equal volume. Recently Morse, Frazer and collaborators have brilliantly substan- tiated the theory of van't Hoff for solutions of cane-sugar and glucose, by making use of Pfeffer's method but using a very refined technique. 1 From what has been given, the osmotic pressure of a solution, sepa- rated from the surrounding pure solvent by a semipermeable membrane, exerts its effects in two ways. First the pure solvent tries to enter the solution and secondly the dissolved substance presses upon the membrane with a force equal to the gas pressure. According to whether we consider either one or the other of these ways, the osmotic pressure of a solution can be considered as its ability to attract the solvent, or as a pressure directed toward the outside. This last conception seems prob- ably for the present to be the most acceptable, nevertheless, the fact that the pure solvent enters through the unmovable semipermeable membrane (as in Pfeffer's experiments) is difficult of reconciliation with this mode of explanation. Obviously, and for physiological purposes, it seems best to make use of the former explanation, in which the osmotic pressure is considered as a measure of the force with which a solution attracts the solvent. Pfeffer's above-described method of directly determining the pressure can only be used in exceptional cases, first because the prepara- tion of the semipermeable membrane is connected with difficulties, and second, because there are only a few crystalline bodies for which imper- meable membranes have been found. There are other quicker and easier ways of determining the osmotic pressure. Solutions of non-volatile substances boil at a higher temperature than the pure solvent. This is due to the fact that the dissolved sub- stance, because of the osmotic pressure, holds on to the solvent with a certain force. As in boiling a part of the solvent is separated from the dissolved body, and as the osmotic pressure can be considered as a measure of the attractive power between the solvent and the dissolved substance, then it is clear that solutions which are prepared with the same solvent and have the same osmotic pressure (isosmotic solutions) 1 Amer. Chem. Journ., 37, 425, 558 (1907); 41, 1, 257 (1909). 4 GENERAL AND PHYSICO-CHEMICAL. must also boil at the same temperature. The rise in the boiling-point of a solution above the boiling-point of the solvent (elevation of the boiling-point) is also, like the osmotic pressure, for dilute solutions pro- portional to the concentration. Solutions have a lower freezing-point than the pure solvent, and as in dilute solutions the solvent can be frozen out from the dissolved body, then isosmotic solutions have the same freezing-point. The depres- sion of the freezing-point is also proportional to the concentration. The determination of the elevation of the boiling-point for the esti- mation of the osmotic pressure of animal fluids is applicable only in exceptional cases, because on heating, precipitates often form. The determination of the depression of the freezing-point has been found of much greater use. This can be accomplished in an easy manner by aid of the apparatus suggested by Beckmann. In regard to the use of this method we must refer to more complete works. 1 The above rule that equimolecular solutions of different bodies have the same osmotic pressure is only applicable to non-electrolytes. The electrolytes (bases, acids, salts) show in aqueous solution a much greater pressure (i.e., a much lower depression of the freezing-point) than equi- molecular solutions of non-electrolytes. As is known, Arrhenius has explained this lack of correspondence by the assumption that the mole- cule of the electrolyte is divided or dissociated into so-called ions hav- ing an opposed electric charge. An ion exerts upon the osmotic pressure the same influence as the non-dissociated molecule. The larger the number of dissociated molecules the more does the osmotic pressure of the solution rise above the pressure of an equimolecular solution of a non-dissociated body. The osmotic action of a dissociated body is equal to that of a non-dissociated body which in a given volume contains as many molecules as the dissociated body contains ions plus non-dissociated mole- cules. If we assume that a is the degree of dissociation, i.e., the number of the molecules that are dissociated, then 1— a is the number that is not dissociated. If in the dissociation of a molecule n ions are formed then the relation of the molecules present before the dissociation to the ions + molecules present after the dissociation is 1:(1— a-\-na) or = l:(l-r-[n — l]a). The expression (l+[n — l]a) is generally denoted by the letter i, and can be directly determined by estimating the freezing- point of a solution of known molecular concentration. A gram-molecule aqueous solution (one that contains as many grams per liter as the molecular weight of the substance) of any non-electrolyte freezes at about - 1.86°, or, the depression of the freezing-point A is =1.86°. For example, 1 Ostwald-Luther, Hand- und Hilfsbuch zur Ausfuhrung physik.-chemischer Messung, 3 Aufl., 1910. OSMOTIC PRESSURE. 5 if we find that A for a gram molecular solution of NaCl is 3.40° then we have according to the above 1 : (l+[n — l]o) =1.86 : 3.40. In the dissociation of NaCl two ions are formed, therefore n = 2, and from the above equation the degree of dissociation can be calculated, a =0.83. The degree of dissociation can also be calculated from the electrical conductivity. Only the ions take part in the con- duction of electricity, and the molecular conductivity ( = — i i — — — : : — } * V molecular concent nit ion/ is proportional to the degree of dissociation. The dissociation increases with the dilution and at infinite dilution all molecules are dissociated (a = l). If we desig- nate with n*> the limit value which the molecular conductivity approaches in infinite dilution and with y.v the molecular conductivity at some definite dilution v, then the degree of dissociation at this dilution is a = — . The positively charged ions are called cations, and the negatively charged ones anions. Common for all acids are the positively charged H-ions while the negatively charged OH-ions are common for all bases. Osmotic Experiments with Plant Cells. We often meet the word osmosis in literature without understanding exactly what is meant thereby. As a rule diffusion streams are meant, w-hich are modified by means of the permeability conditions of an inclosing membrane. We now know that the driving force, namely, the streaming, is brought about by the differences in concentration, i.e., by difference in the osmotic pressure on the two sides of the membrane. After Nageli found that certain plant cells, when they were treated with a sufficiently concentrated solution of certain substances, changed their appearance so that the protoplasm retracted, 1 de Vries studied this phenomenon further. 2 He called it plasmolysis. The most important substances for bringing about plasmolysis are the salts' of the alkalies and alkaline earths, varieties of sugars, polyatomic alcohols, and neutral amino- acids. An indispensable condition for bringing about plasmolysis is that the solution must not have any destructive action upon the cells. Xageli gave the correct interpretation of plasmolysis, which is that those bodies which plasmolyze plant cells pass through the cell membrane of the cell, but not through the protoplasmic layer which follows. Instead of this the sub- stance attracts water from the inner parts of the cell. The cell contents surrounded by protoplasm therefore diminish in volume and the protoplasm recedes more or less from the cell membrane. From this it follows that only those solutions whose power of attracting water is greater than that of the cell contents can bring about plasmolysis. As the ability to attract water (or the osmotic pressure) increases with concentration, there must be a limit solution for every substance above which all higher concentra- tions plasmolyze. The limit solution is called isotonic with the cells; 1 Pflanzenphysiol. Untersuch., 1855. 2 Eine Analyse der Turgorkraft, Jahresber. f. Wissensch. Botanik, 14, 427 (1884). 6 GENEKAL AND PHYSICO-CHEMICAL. weaker solutions are called hypotonic, and stronger hypertonic. De Vries, with the aid of equal cells (cells of the epidermis of the lower side of the leaf of the Tradescantia discolor) has, for various substances, determined the concentration of this limit solution. It was found that the limit solution of analogously constructed salts had the same molec- ular concentration. Thus the alkali salts of the type NaCl (haloid salts, nitrate, acetate) plasm olyzed at one molecular concentration and the salts of the type Na2SC>4 (sulphate, oxalate, diphosphate, tartrate) at another concentration. If the plasmolyzing power of a molecule of the first group is equal to 3, then the molecule of the second group equals 4. The concentration of the limit solution varied in de Vries' experiments between the limits corresponding to a NaCl solution of 0.6-1.3 per cent. As above mentioned, only those substances bring about plasmolysis which cannot themselves pass through the protoplasm envelope of the cell content, and these substances only in the case that the concentration is sufficient. If a body is taken up by the protoplasm it produces no plasmolysis, because its tendency to attract water has been satisfied by its own passage into the cell. These substances do not produce plasmolysis in any concentration. If a body slowly passes in, then at first it causes plasmolysis, but this then ceases later. The plasmolytic methods have been used by de Vries, and especially by Overton. 1 Experiments with Blood Corpuscles. Over a hundred years ago Hewson observed that the blood corpuscles were destroyed in water, and that salts in certain concentrations prevented destruction. 2 Ham- burger 3 has carefully and systematically investigated the action of salts of the alkalies and alkaline earths, and concludes that when blood is mixed with certain volumes of solutions of different concentrations of the same salt, all solutions whose concentration lie below a certain limit cause the exudation of haemoglobin. On comparing the molec- ular concentration of the limit solution of different salts it was found that they bore the same relation to each other as the relative figures found by de Vries for the molecular concentration of the plasmolytic salt solutions. From this it probably follows that the protective action of the salts upon the blood corpuscles depends upon the same reason as the plasmolysis. This conclusion is also supported by the fact that those substances which, according to de Vries, in proper concentration cause plasmolysis in living plant cells, can also under similar conditions prevent the exudation of haemoglobin. Those bodies, on the contrary, " Vierteljahwchr. d. Naturf. Gesellsch. zu Zurich, 40, 1 (1895); 41, 383 (1896). 'Phil. Trans., 1773, p. 303. 1 Arch. f. (Anat. u.) Physiol., 1888, p. 31; Zeitschr. f. Biol., 26, 414, (1889). OSMOTIC PRESSURE. 7 which do not cause plasmolysis, act in aqueous solution in the same manner upon the blood corpuscles as pure water. This has been espe- cially shown by the investigations of Gryns. 1 Different investigators have attempted to perform plasmoh tic experiments with animal cells, but without any special result. With the microscope one can often observe that the red blood corpuscles shrink under the influence of a strong salt solution, but the limit solu- tion when the shrinking just begins cannot be exactly determined because the changes in volume are so very small. If we summate the changes in volume of many corpuscles, which can be done by centrifuging the blood mixture in a graduated tube, then very small changes can be detected. Such determinations have been made by Hedin, 2 Koeppe 3 and others. It was found that the blood corpuscles swell in a weak salt solution, shrink in a stronger solution, and there is a certain concentration which does not change the volume. By determining the freezkig-point Hedin found that this concentration for NaCl was nearly isosmotic with the serum of the blood corpuscles used. The depression of the freezing- point was about 0.56° and the concentration of the NaCl solution is 0.9 per cent, or about 0.15 normal. The question as to the permeability of the blood corpuscles has been investigated by Hedin, using a method depending upon the following: 4 The depression of the freezing-point of a solution is proportional to its con- centration. A certain amount of the substance to be tested is dissolved in blood. The serum of this treated blood freezes at a lower temperature than before the salt was added. The depression of the freezing-point can be designated as a. Now the same amount of substance is dissolved in serum using the same volume of serum as blood was previously used. The depression of the freezing-point of this serum can be designated as b. From this it is evident that a =6 if the blood corpuscles take up just as much dissolved substance from the blood as an equal volume of serum. If the blood corpuscles take up less than the serum then a> b or-r > 1 , and when they take up more than the serum then a 3 formed at the same time gave the alkaline reaction to the solution. Koeppe 3 as well as Hamburger and v. Lier 4 claim, on the contrary, that an exchange of HC03-ions and Cl-ions takes place between the blood corpuscles and the solution, and Hamburger and v. Lier claim to have shown that the blood corpuscles are permeable only for anions, while the cations do not pass in. Hamburger 5 and his collaborators have also found about the same osmotic phenomena with other free mobile cells such as leucocytes, spermatozoa as with the red blood corpuscles. The osmotic relations have also been tried with intact parts of organs, therefore with cells 1 Pfliiger's Arch., 81, 167 (1900). 2 Sitzungsber. d. med. phys. Gesellsch. zu Wurzburg, 1895. » Pfliiger's Arch., 67, 189 (1897). . 580 (1888). 1 Bioch. Zeitechr., 2, 251 (1907). COLLOIDS. 25 On comparing the concentration of various salts just sufficient for precipita- tion, where at one time the same anion with different cations was tested and another time the same cation with different anions, Pauli has arranged the cations and anions in the following order in increasing precipitation ability: CNS the solution becomes acid, and a small quantity of barium remains in the precipitate, corresponds to Billitzer's theory. This quantity of barium cannot be removed by water, but can be replaced by the corresponding cation by washing with a solution of another salt. According to Billitzer in the mutual precipitation of colloids a quan- tity relation exists which is dependent upon the electrical charges 4 (see also page 22). The fact that the precipitation of colloids is a manifestation of processes which occur in a homogeneous medium, makes the understand- ing of these especially difficult. If, as is generally accepted, we consider 1 Anorganische Fermente (1901), 15. Zeitechr. f. physik. Chem. Soc, 45, 327 (1904); 51, 129 (1905). Mourn. Chem. Soc, 67, 63 (1895). •Zeitechr. f. physik. Chem., 51, 141 (1905). COLLOIDS. 27 the colloid BOlution as a homogeneous fluid of suspended solid or fluid particles, then in the " solution " there occur at least two special con- stituents] separated from each other — the colloid particles and the sol- vent. This is expressed as follows: the system contains two phases. The solvent is often more correctly called the dispersion means and the colloid particles called the disperse phase. If to such a system a new sul stance is added, then the reaction which follows, depends essentially upon the division of the new substance between the two phases. In regard to the possible division two cases will be presented: 1. The process can be similar to the division of a soluble substance between two solvents. If a substance is brought in contact with two solvents at the same time, then it divides itself so that the relation between the concentration in the two solvents remains the same but independent of the total quantity of the dissolved substance. If the quantity of substance in each 100 cc. of the two solutions 1 and 2 is Cl designated bv ci and c-2, then it follows that — =k where k is a constant. 1 C-2 The first example where this law was shown to be correct was the divi- sion of succinic acid between water and ether (Berthelot and Jung- fleisch -'.). This law was also shown to be true for the division of a gas between a gaseous and a fluid phase, i.e., for the absorption of a gas in a fluid (Henry's law of absorption). The conditions for the cor- rectness of this law are that the temperature remains the same in experi- ments with different quantities of substance as well as that the substance has the same molecular size in the two phases. 2. In those cases where finely divided solids take up dissolved sub- stances or gases the division is generally not independent of the total quantity of the dissolved substance or of the gas. This is often called adsorption. 3 For example, if we are dealing with the adsorption of a dissolved substance by a finely divided solid occurring in a solution, then a greater percentage is taken up from a dilute solution than from a concentrated one. On increasing concentration the adsorbed fraction becomes continuously less so that the absolute quantity taken up reaches a maximum which corresponds to the greatest adsorption ability of the solid body. This is expressed by the formula — = k, where Ci and c 2 indicate the concentra- tion of the solid body and in the solution; n and k are constants and indeed, n is 'Nenut, Zeitschr. f. physik. Chem., 8, 110 (1891). 2 Ann. Chim. phys. (4>. 26. 396 (1872). 3 It must be remarked that in the older literature oftentimes no difference was made between adsorption, and absorption, in which case both processes were included under the name absorption. 28 GENERAL AND PHYSICO-CHEMICAL. always > 1. (If n = \ then the formula would be —=k and we would be dealing with a so-called solid solution.) Appleyard and Walker l have studied the adsorption of organic acids from aqueous and alcoholic solutions by means of silk; the divi- sion was found to correspond to the above formula for adsorption. Freundlich 2 has also carefully tested the adsorption of crystalloids by carbon. From these experiments it was shown that the equilibrium could be quickly attained from both sides, i.e., that the process was readily reversible. The above-given formula was found sufficiently accurate for the case w r here only the total quantity of the dissolved (to adsorb) substance varied. The series in which the organic acids were adsorbed by silk, as found by Appleyard and Walker, were pratically the same as with carbon. The influence of temperature was slight. According to Kuster, 3 the combination between starch and iodine is to be considered as an adsorption compound, and Biltz 4 finds for the division of AS2O3 between iron hydroxide (1) and water (2) the for- mula — = 0.631. The theoretical foundations for the adsorption phenomenon are not especially clear. Generally the adsorption is considered as con- nected with segregation and surface tension phenomenon. At the con- tact surface between a solid body and solution a surface tension exists which is considered as positive, i.e., this attempts to diminish the contact surface. The surface energy used thereby tends to be a min- imum potential energy. As the product from size of surface and surface tension are the same, and as the first cannot change, the surface energy can only be diminished by a reduction of the tension. If, therefore, the tension is diminished by increasing the concentration of a sub- stance dissolved in a fluid, then this substance tries to collect itself at the surface in greater concentration than in other parts of the fluid (Ostwald, 5 Freundlich 6 ). In regard to the surface tension of solid- fluid we only know that it is positive, but can otherwise show great differences (Ostwald, 7 Hulett 8 ). According to this theory the facts are that certain solid substances possess the ability of adsorbing dis- 1 Journ. Chem. Soc, 69, 1334 (1896). 2 Debar die Adsorption in Losungen, Leipzig (1906). » Ann. d. Chem. u. Pharm., 283, 360 (1894). * Ber. d. d. chem. Gesellsch., 37, 3138 (1904). •Lehrh. d. allg. Chem., 2. Aufl., 2. Bd., 3. Teil, 237 (1906). 8 Ueber Adsorption in Losungen, 50-51. 7 Zeitschr. f. physik. Chem., 34, 495, 1900. •Ibid., 37, 385 (1901). COLLOIDS. 29 solved bodies, and for this reason the ads >rbed substance lowers the surface tension of the solid-fluid, and indeed, the more the greater con- centration in which it occurs. That especially carbon and colloid sub- stances are adsorption bodies lies in the fact that they have an especially large surface due to their finely divided state or porosity, which there- fore, cet. par., must give them a great surface energy. That proteins, on precipitation, carry down other bodies with avidity is well known; inorganic hydrogels also take up dissolved substances with energy. The curves obtained for the latter process by van Bem- melen x show a close analogy with the characteristic curves for the adsorption compounds. It often occurs that the body taken up homo- geneouslv saturates the hydrogel, in which case — = k, and a sort of solid solution is the result. In certain cases, undoubtedly, chemical combinations with quite positive conditions are formed. The precipitation of colloids by electrolytes has also been discussed by Freundlich 2 from the standpoint of the adsorption hypothesis. Thus, for the precipitation ability of an electrolyte, the electric charge of the precipitating ion comes first into consideration and secondly, the ability of the precipitating colloid to adsorb the same. According to Moore and Roaf 3 the salts of the red corpuscles are retained as adsorp- tion compounds (adsorpates) by the proteins. Thus far only the adsorption of crystalloids has been considered. Colloids are also taken up by solid substances or by other colloids. Still in these cases the conditions are more complicated than in the above- mentioned adsorption phenomena, as the combinations formed are in special cases irreversible or gradually become irreversible. It is well known that carbon takes up colloidal colored substances, and we have numerous exam- ples of the combination of dissolved colloids with solid colloids in technology. Biltz 4 has been able to show that many dyeing processes are to be considered as adsorption phenomena, and later Freundlich and Losev 5 have measured the adsorption of basic and acid pigments by carbon and also by fibers (wool, silk, cotton), and have shown the correspondence of the two processes. With the basic pigments, which were used as salts, a splitting occurred into a pigment base, which was taken up by the fibers as well as by carbon, and an acid which quantitatively remained behind. This is similar to the cleavage which precipitating electrolytes undergo in the precipitation of the suspension colloids (see page 26). 1 Zeitschr. anorg. Chem., 23, 111, 321 (1900). 2 Zeitschr. f. Chem. u. Ind. d. Koll., 1, 321 (1907). 3 Bioch. Journ., 3, 55 (1908). 4 Ber. d. d. chem. Gesellsch., 37, 1766 (1904); 3S, 2963, 2973, 4143 (1905). 5 Zeitschr. f. physik. Chem., 59, 284 (1907). 30 GENERAL AND PHYSICO-CHEMICAL. Tanning is also brought about by adsorption processes, as the prepared skins adsorb the tanning substance. 1 The precipitation of portein by adding finely divided solids (carbon* kaolin 2 ) or by suspended solids (mastic 3 ) precipitated in the liquid, as well as the action of protective colloids as already mentioned are also due to adsorption processes. The precipitation of protein, which occurs on shaking the protein solution with liquids, in which the protein is not soluble, is also to be considered as a surface tension action (Ramsden 4 ). Bechhold, 3 in his above-mentioned experiments on the filtration of colloids, has observed conditions which he considers as adsorption phe- nomena. Under certain circumstances a colloid can prevent the filtra- tion of another colloid. A filter which was permeable for colloidal AS2S3, but retained colloidal Prussian blue, did not allow a clear mixture of the two to pass through. The particles of AS2S3, were adsorbed by the particles of Prussian blue, and could therefore not pass through the filter. Gels. We have often mentioned gels or jellies (page 14). Only certain colloids can occur in the form of gels. Certain gels are spon- taneously formed in sufficiently concentrated solutions (silicic acid, certain metallic hydroxides) and these do not redissolve in water. Other gels, like gelatin and agar, are formed on cooling of the hot, concentrated solutions, and are again soluble in water. According to Hardy 6 the gel formation of gelatin is to be considered as a segregation process whereby a separation into two fluids occurs, one of which solidifies. The two phases are only differentiated by the microscope, and the chemical testing of the theory fails because of the cir- cumstances that the two phases cannot be analyzed separately. In opposi- tion to this Pauli claims that the gel passes through all of the intermediary steps into the corresponding sol and is therefore homogenous in the same sense as these. 7 When gels are freed from water by evaporation or in other ways, they show a special ability to take up water, which is brought about by different processes which are included in the ordinary term imbibition. The views on this imbibition are indefinite. Surface phenomena play a role here. According to van Bemmelen 8 the water is not chemi- 1 See Zeitschr. f. Chem. u. Ind/d. Koll., 2, 257 (1908). 2 Bioch. Zeitschr., 5, 365, 1907. • Ibid., 2, 219 (1906); 3, 109 (1906). • Zeitschr. f. physik. Chem., 47, 343 (1904). 1 Ibid., 60, 299 (1907). • Ibid., 33, 326 (1900). ■> Bioch. Zeitschr., 18, 367 (1909). 'Zeitschr. anorg. Chem., 13, 233 (1896); 20, 185 (1899). COLLOIDS. 31 cally combined in definite proportions, hut the quantity continually changes with the temperature and the vapor pressure. On the other hand, the imbibition stands in close relation to the osmotic pressure which is evident, if we define the osmotic pressure of a substance as its ability to attract water. The relation between imbibition and osmotic pressure is still closer in those cases when the Substance finally is dissolved in water. If a hydrogel is placed in a salt solution instead of in pure water, the imbibition phenomena essentially change. This was first studied by Hofmeister, 1 using gelatin plates. The process is rather com- plicated, as salt is taken up by one side of the gelatin plate and water by the other, and the taking up of water is influenced by the quantity of salt taken up. It has also been found that when gelatin plates are treated with solutions of increasing concentration of the same salt, the taking up of salt increases at first with the salt concentration, then becomes slower, and attempts to reach a maximum and then remains almost stationary. As long as the taking up of salt increases, the quan- tity of water passing into the gelatin also increases; when the salt fails to pass then the water also ceases to pass. It has also been found that the maximum of salt absorption for sulphate, tartrate and citrate can be attained with much lower molecular concentrations than with chloride, nitrate and bromide. From this it follows that the sulphate, tartrate and citrate have a retarding action upon imbibition within certain limits of concentration, while the chloride, nitrate and bromide have an accelerating action. Pauli 2 has investigated the influence of salt solutions upon the solid- ification and melting-point of gelatin. If the salts are arranged in the order of their ability to lower the solidification point of gelatin we come to the series sulphate, citrate, tartrate, acetate (water), chloride, chlorate, nitrate, bromide, iodide. This series corresponds well with that of Hofmeister. Acids and alkalies exert a special influence upon gelatin, as they both, in very dilute solutions, strongly accelerate imbibition (Spirq, 3 Wo. Ostwald 4 ). From the previously mentioned investigations of Lillie, on the osmotic tension of gelatin solutions, it was found that the addition of acids and alkalies increased it (page 17). Since Graham's fundamental experiments it was believed that col- loidal sols could not diffuse into gels while crystalloids could pass just 1 Arch. f. exp. Pathol, u. Pharm., 28, 210 (1891). 2 Pfluger's Arch., 71, 333 (1898). 3 Hofmeister's Beitriige, 5, 276 (1904). 4 Pfluger's Arch., 108, 563 (1905). 32 GENERAL AND PHYSICO-CHEMICAL. as quickly into gels as into pure water. Nevertheless, Spiro * has observed that dissolved ovalbumin as well as haemoglobin could pass into gelatin plates. On the other hand K. Meyer 2 as well as Bechhold and Zeigler 3 have found that the distance passed by a crystalloid in gelatin may be much shorter than in pure water. In such experiments no doubt adsorp- tion processes must be considered. m. CATALYSIS. When two bodies which can act chemically upon each other are brought together the reaction generally takes place so fast that it can- not be measured. In other cases, by special means, we can observe how the reaction gradually proceeds. When cane-sugar is inverted by weak acid, the decrease in the rotation of the solution can be fol- lowed with the polariscope; and when an ester is decomposed by alkali the quantity of still free alkali can be determined by titration. The quantity of substance measured in gram-molecule per liter (mole) which is decomposed in the unit of time, is called the reaction velocity of the system. The so-called law of mass action, as proposed by Gtjld- berg and Waage, states that the reaction velocity is every moment proportional to the molecular concentration of the reacting bodies. A mixture cf alcohol and acetic acid is transformed into acetic ether and water, especially in the presence of some mineral acid. If the molec- ular concentration of the alcohol and acid be designated by C A and C s , then according to the law of mass action the reaction velocity is vi=ki.C A -C s , where &i indicates a constant which is independent of the quantity of reacting substances and the time limit is so short that the concentration can be considered as constant. This reaction, like many others, is reversible, #i.e., two reactions occur simultaneously: one between the alcohol and acetic acid, producing acetic ether and water, and second, between acetic ether and water, re-forming alcohol and acetic acid. This is expressed as follows: C 2 H 5 .()H+HO.CO.CH3^C2H 5 .O.CO.CH3+H 2 0. The velocity of reaction when it passes from left to right is called V\. If the velocity in the reverse reaction is called v