MARINE PROPELLERS BARNABY STB PO GSOOQQoe DsXEGESe © CORNELL UNIVERSITY LIERARY. na m ThidBookis not toe aaken’e from the Readiinz Rodém. ' © | $< hig ——_ -_ _— WHEN DONE “ere. RETURN AT ONCE To iii I ian a olin,anx MARINE PROPELLERS. MARINE PROPELLERS BY SYDNEY W. BARNABY, M.I.N.A. AND ASSOC. M. INST. C.E. GOLD MEDALLIST OF THE INSTITUTION OF CIVIL ENGINEERS, Being a Course of Three Lectures delivered at the Royal Naval College, Greenwich, March 1885. E. & F. N. SPON, 125, STRAND, LONDON. NEW YORK: 35, MURRAY STREET; 1885. KB PREFACE, —— IN preparing these lectures for the students of the Royal Naval College, I availed myself of informa- _tion from various sources. Now that they are published verbatim in book form, it becomes a duty as well as a pleasure to acknowledge the assistance thus received. I am indebted first of all—and who that studies the subject of Marine Propulsion is not? —to Professor Rankine. Also to Mr. W. Froude, Mr. Bourne, Mr. White, Professor Osborne Rey- nolds, Mr. Sennett, Mr. Maginnis, and Mr. Seaton. There is, however, much that is new. The curves in Plate II. which enable the dia- meter, pitch, and speed of revolution of a screw suitable for any horse-power and any speed to be determined, are now made public for the first time. For most of the new material, and especially for permission to publish these curves, and the method of producing them, I am indebted to Mr. Thorny- croft. vi PREFACE. It was my privilege to be associated with him in making some 550 experiments with model screws, and a considerable portion of these lectures is the result of knowledge thus obtained. I feel some diffidence in putting forward in my own name information so acquired, as the credit of it is entirely due to Mr. Thornycroft, but after this explanation, any merit which may be found in the following pages will be attributed to the proper source, SYDNEY W. BARNABY. THE HOo.Liigs, CHISWICK MALL, October 12th, 1885. INTRODUCTION. —$——— AFTER these lectures had been delivered it was considered by the Admiralty officers who had heard them, that if Mr. Thornycroft would offer no objection to their publication; much good would be done by giving them a permanent form, and making them generally accessible to naval officers, shipbuilders, and engineers. s That firm might have been quite willing to allow Mr. Barnaby to give to the classes at Greenwich the results of their experimental research, without being prepared to allow a wider circulation. They showed themselves superior to the desire to preserve trade secrets, and gave an immediate consent to the request made to them. The screw-propeller has less comparative atten- tion bestowed upon it than any other part of a ship. The shipbuilder does not study it and experi- ment upon it, because it is part of the engine, and is included in the work allotted to the Marine Engineer. The Marine Engineer is concerned with the viii INTRODUCTION. development of the power of the engine, and better results may often be obtained in the indica- tion of power with a screw ill-suited to give speed to the ship, than with one properly adapted to its . form and desired speed. He is not responsible for the speed of the ship: that rests with the ship- builder, who is often disappointed with results falling much below his expectations. Experiments with screws in actual ships are very costly, and are but rarely made. One notable case is referred to in these lectures where the prelimi- nary model experiments on the /yzs promised results so different from those actually obtained, that it was determined to endeavour to search out the cause of the falling off in speed. Had it not been for these preliminary model ex- periments, the speed actually obtained in the ship would perhaps have been accepted in the usual way, but it turned out that two knots of speed were being lost by badly-proportioned propellers. One of the most interesting parts of these lectures is that relating to the Screw Turbine devised by Mr. Thornycroft. This invention has not yet attracted the atten- tion it claims and deserves. It has, I believe, a great future before it. All that has been done at present is to obtain INTRODUCTION. ix exceedingly high results in speed in boats having only a few inches draught of water. In this respect it may be said with certainty that the stern wheel propeller is doomed. It will be replaced without doubt by this screw turbine in those shallow waters where the stern wheel has hitherto done good service. The more brilliant future to which I think it is destined, relates to large ships which, whether regularly built for war purposes or not, may have to be exposed to artillery fire in war. Armour has been largely employed to protect far more than the propelling and steering mechanism in war ships, but it is gradually being brought down even in France, where the system was invented, so as to cover in the largest ships only a height of about 3 or 4 feet out of the water. In smaller vessels the engines are kept below the water, and are covered by a bomb-proof deck instead of side armour, Marine engines working vertically—as it is best they should work—require so much height that only vessels of considerable draught of water can keep the machinery below water, even when there are twin screws. By using three or four screws, greater security might_be obtained in vessels of moderate draught. ; x INTRODUCTION. Experiments have been made in France, at the instance of Monsieur de Bussy, to ascertain whether multiple screws would so interfere with each other as to give bad results in steaming. Hitherto the experiments have not justified any beyond two screws. But the screw turbine alters the condition of the problem. Interference with mutual action is reduced to a minimum, and is almost completely under control. We may therefore expect to see three or more screws introduced into the large French ships. But this is by no means the most important result to be anticipated. What chiefly distinguishes the regular ship of war from the fast steamship of commerce, is that in the latter, the propelling engines stand high above water, and as there is only one propeller, the steering apparatus is also necessarily above water. If multiple engines and screw turbines existed in such ships, they would have a protection for their vital machinery which would make them almost as defensible as the regular ship of war. It must be for the general interest of mankind, and therefore for the interest of England, that ships built for commerce should have offensive and defensive power, and that standing navies should gradually play a less important part and be less INTRODUCTION. xi necessary for the security of commerce on the seas. There appears to be no reason, why an Atlantic liner should not have three or four engines with screw turbine propellers, the whole of the machinery being under water, and having a light steel deck over to receive cargo or coal. If such vessels existed, the Government would be forced to recognise their importance, and to take measures for incorporating them into a great system of national defence. N. BARNABY, Late Director of Naval Construction. MARINE PROPELLERS. LECTURE I. THE principle upon which nearly all marine pro- pellers work, is the projection of a mass of water in a direction opposite to that of the required motion of the vessel. The only exception to this rule is met with in the case of a few river steamers and ferry-boats, where a chain or rope lying in the bed of the river passes over a drum or wheel in the vessel itself. When a vessel is in motion at a regular speed, the reaction of the mass of water projected back- wards by the propeller is exactly equal to the resistance experienced by the vessel. Simple, and almost axiomatic as this statement appears at first sight to be, it is very important that its full bearing should be grasped. When it is clearly understood that propulsion is obtained by the reaction of a mass of water pro- jected sternwards with a velocity relative to still water, the absurdity is at once seen of attempting B 2 MARINE PROPELLERS. to get a propeller to work without slip. If there is no slip, there is no resultant propelling reaction, except in the limiting case where the mass of water acted upon is infinite. The whole problem, therefore, resolves itself to this :—What is the best proportion between the mass of water thrown astern and the velocity with which it is projected? That is, if the screw-pro- peller is under consideration, the ratio between its diameter and its pitch. In symbols—If W = weight of water acted on, S = slip, = 32°2, Reaction = us & How big shall we make W? How big shall we make S? The considerations which should guide us in the decision will be treated of later on. There are four different kinds of propellers :— The oar, the paddle-wheel, the screw, and the pump. The first and oldest of them, the oar, may be used in two ways. The action may be inter- mittent as in rowing, when water is driven astern during half the stroke and the instrument brought back above the water; or its action may be con- tinuous, as in sculling. When used as in rowing, it is exactly analogous to a paddle-wheel, while MARINE PROPELLERS. 3 the action of the scull closely resembles that of the screw. It is supposed that in the ancient galleys, which were propelled by a large number of oars in several tiers or banks, the oars hung vertically, and worked inwards and outwards with a sculling action. They were not removed from the water, but served as props when the vessel was aground; the oars were always propelling the vessel in both parts of the stroke. The rowers generally sat with their faces outwards and forwards. There was great overhang of the sides to allow of several tiers of rowers one above another. One or two mechanical arrangements have been tried for imitating the action of the scull, but the reciprocating motion causes vibration and makes it unsuitable for the application of steam-power. The oar, as used in rowing, is a very efficient instrument. To obtain the maximum efficiency out of it, a constant pressure should be maintained upon the oar, so that the water is started gradually from rest, and the acceleration uniformly increased throughout the whole of the stroke. It is a common thing to see men giving a terrific jerk at the commencement, and then allowing the oar to trail after the water for the rest of the stroke. A glance at a University crew will show that the stroke is kept up with a uniform pressure with no jerk anywhere. The radial paddle-wheel was introduced in 1812, B 2 4 MARINE PROPELLERS, and with the exception that the floats are now generally made to feather, as it is called, it remains much the same as when originally introduced. The screw was brought into successful operation as a propeller, by Ericsson and Smith, in 1836. The Archimedes, a screw vessel of 237 tons burthen, was built by the latter in 1839. The screw used was a single-threaded screw of one complete convolution. A double thread with half a convolution was afterwards tried and found to be an improvement, but the best result was obtained with two threads, and one-sixth of a convolution. Three strings wound spirally round a cylinder make a three-threaded screw. If, instead of strings, flat blades be wound edge- wise round a cylinder, and each blade has an edge soldered to the cylinder, then, if a slice be cut off the cylinder, there will be one piece of blade attached to the cylinder if the screw have one thread, two pieces if two threads, and so on. (Fig. 1.) The pitch of a screw may be defined as the distance it would travel in one revolution if working in a solid nut. One of the last things Robert Griffiths said about the screw-propeller, and he was a man who has made perhaps more experiments, and worked more at the screw, than any one else, was, that ‘four strips of plate iron set at an angle on the * MARINE PROPELLERS. 5 “shaft which would hold the engine to the speed “you required would give you within half a knot “of the best screw ever made.” Now, although I I! am not prepared to endorse this altogether, having tried a propeller of that sort myself, I think it would be safe to say that a uniform pitch screw, of the proper diameter and pitch, of the shape finally used on the Archimedes, will give within half a knot of the best screw ever made. In the early trials, various devices of hook-joints, bevel wheels, &c., were resorted to in order to avoid taking the screw-shaft into the ship below the water. The patentee of the arrangement shown in Fig. 2 says that it may be worked either by horses or by a steam-engine, as may be found most convenient. Guy lines were to be attached to the fore end of the screw-shaft so that the propeller could be made to assist in steering. There is a disadvantage connected with an inclined shaft which has been generally overlooked. The result of depressing the end of a screw- shaft is to cause the pitch of the propeller to vary through every part of the revolution. If the incli- 6 MARINE PROPELLERS. nation is supposed to be 45°, for example, that part of the blade which is intended to have a pitch Fic. 2. =~ MARINE PROPELLERS. 7 of three diameters has a pitch in reality varying from nothing to infinity. It is of course obvious that the pitch of the blades of a screw zz relation to the axis is un- changed by any alteration of the direction of the shaft. It is also clear, that if a screw does not move along, but has a motion of rotation only, the opposition of the water is the same whatever be the direction of the shaft. But if the propeller be allowed to move along, while at the same time it be constrained to move horizontally, the shaft being inclined to the horizontal, then the opposi- tion or resistance of the water is not uniform, but varies over every part of the revolution. It is necessary to come to a clear understanding as to what is meant by the “ pitch” of a screw. If I show you this model of a boat, and ask you whether you considef it well proportioned, you will probably say, “ Well! the length is about 22 inches, and the beam about 3 inches; I should say that was a well-proportioned model.” But you would now be making an assumption. You are assuming that the model is to travel end- wise through the water; but if I were to tell you that it was intended to travel broadside through the water, you would say, “That is another matter altogether. The virtual length is now 3 inches and the beam is 22 inches, that is ot a well-pro- portioned model.” In the same way, a screw may 8 VWARINE PROPELLERS. have a certain pitch in relation to its axis, but if it be placed vertically out through the bottom of a ship, the «7rfwal pitch, or the pitch measured in the direction of motion, is w7/. Now let us examine the phases through which a blade of the screw passes during one revolution. It is convenient and suitable to consider the action of a screw as similar to that of an inclined plane moving past the stern. In Fig. 3, the full line represents the upper blade as a plane moving from port to starboard, the dotted line represents the lower blade as a plane moving from starboard to port. In Fig. 4, the shaft is shown horizontal, and the full line shows the blade going down, the dotted line the blade coming up. In Fig. 5, the shaft is inclined at 45°, the full line shows the blade going down, and the dotted line the blade coming up. Now as the ship moves forward, the water flows to the screw in horizontal lines. The blade, which at one part of the revolution is edgewise to the water, at another is square on to it, and the result is a succession of shocks causing violent vibration. Another way of looking at it is this. A particle of water meeting the ascending blade has its motion Fic. 3. WARINE PROPELLERS. 9 relative to the vessel arrested altogether, while a particle first meeting the forward edge of the descending blade would require to have its velocity infinitely accelerated in a horizontal direction to Fic. 4. Fic. 5. no enable it to escape from under it. This is what is meant by saying that in the above example the pitch varies from nothing to infinity during each revolution. In a torpedo-boat built for the Government by Mr. Herreshoff of the United States, this difficulty was most ingeniously and boldly met. Mr. Herreshoff desired to place his screw com- pletely below the bottom and almost amidships. In order to do so, he inclined his shaft sufficiently to bring it through the bottom of the boat; he then “sprung” it to such an extent that the axis of the screw was nearly horizontal. Although this brought a considerable strain upon the shaft bearings, little inconvenience seems to have been experienced, and the result was that the boat went astern as fast as she went ahead. The 10 MARINE PROPELLERS. boat was a small one, and the shaft of small diameter. An attempt has since been made to place the screw in the same position below the bottom of a Ist Class Torpedo-boat, in the hope thereby to get a good speed astern. But Mr. Herreshoff’s novel expedient could not be adopted with the large diameter of shaft, and the difficulty it was de- signed to meet appears to have been overlooked or insufficiently appreciated. The shaft was taken through the bottom at a considerable inclination, and the vibration and loss of efficiency caused by the varying pitch of the propeller was so great that the screw had to be replaced in the ordinary position. Fic. 6. Woodcroft’s gaining pitch screw was originally proposed, as shown in Figs. 6 and 7. ATARINE PROPELLERS. II The connecting-rod works out through the side above water. Fic. 7. p tw The Earl of Dundonald in 1843 patented a pro- peller with the blades thrown back as shown in Fig. 8, the object being to counteract the supposed centri- fugal action of the water caused by the rotary motion imparted to it by the screw. In 1849, Robert Griffiths patented a self-adjusting propeller, which he thus describes :— If the screw 13 MARINE PROPELLERS. moves with greater velocity than usual, the increased resistance of the leading edge shall correspondingly increase the pitch, thus increasing the resistance and bringing down the revolutions.” In 1851, Woodcroft patented the feathering screw, for manceuvring purposes. The blades are feathered FIG. 9. | TALON aa so as to pass edgewise through the water during one part of the revolution. In 1853, twin screws were proposed to assist in manceuvring. MARINE PROPELLERS. 13 The form of Griffiths’ screw which is most in use is represented in Fig. 9. I think the principle feature in his propeller is the large boss one-fourth the diameter of the pro- peller, which, while not impairing the efficiency, enables the blades to be fixed in such a manner that the pitch can be readily altered. This is an important consideration, as it is very difficult to fix upon exactly the right pitch in designing a new propeller, and it is extremely convenient to be able to alter the pitch without making a new propeller. The Hirsch screw (see Fig. 10), The features of this propeller are that the pitch increases in the direction of its length, and that the propelling surfaces are so formed as to throw the water somewhat towards the axis, with the view of counteracting the centrifugal force. The outline is curved, possibly with the idea of having less edge resistance, because of its cutting through the water more easily than a straight-edged blade. This is a fallacy, because a blade cannot cut its way gradually into water when it is wholly immersed. Mangin’s screw (Fig. 11) consists of two narrow screws set behind one another on the screw shaft, with a space between them. It is supposed not to rotate the water so much as other screws. Rigg’s screw had a fixed screw or guide blades set behind the revolving screw, with the blades set at the reverse angle, so as to take the rotation 16 MARINE PROPELLERS. out of the water and leave it moving directly astern. Rankine and Napier patented a modification of this idea in the form of a twisted rudder, of which the part above the screw-shaft bends in one direction and the part below in the opposite, Screws have been tried with the pitch in the centre less than the pitch at the circumference, so as to allow the central part to follow up the water as in a nut—the circumferential part doing the most work —the design being to prevent a centrifugal motion being given to the water by the action of the central part of the screw. The Thornycroft torpedo-boat screw, which has been a very successful screw, has an increasing pitch at the middle of the blade, but the pitch gradually becomes uniform towards the roots and towards the tips, the reason being that towards the roots the rota- tion given to the water is already excessive, and it is consequently not advisable to increase it by in- creasing the pitch, and towards the tips, if it is attempted to accelerate the water too much, it escapes round the tips to the back of the blade, “short circuits” it in fact. The tip of the blade does very little good, only you must have a tip. The blades are also thrown back after the fashion of the Dundonald propeller, but, instead of being straight like his, they are convex on the driving face. The object is to counteract centrifugal force, and as the rotation which produces it is greatest MARINE PROPELLERS. 17 at the root and diminishes towards the tips of the blades, the angle to which the blade is inclined to the axis varies in a similar way. We have made a number of experiments at Chiswick with models of propellers which I shall , Fic. 12. ie describe more particularly in another lecture, but I may say that this propeller was superior to any tried. As, however, it is very important to prevent the propeller breaking the surface of the water, and as the draft of the torpedo-boat is small, it has been found a great improvement to use a smaller pro- peller with broad blades (Fig. 12), which can be completely immersed, although the older form, Cc 18 ATARINE PROPELLERS. with long thin blades, if completely immersed, is slightly superior. With regard to the immersion, it appears that provided a screw is sufficiently far below the surface to prevent it from drawing air, any further immersion within the limits that can practically be obtained is of little value. The speed with which water can follow up the blades of a screw, depends upon the head of water over it, but when the immersion is sufficient to exclude air, a head of water equivalent to 30 feet is supplied by the atmosphere ; this is a fact which has been overlooked by many writers, but was clearly pointed out by Professor Osborne Reynolds. We found by experiments on the model of the Thornycroft screw, that the efficiency which is as much as 70 per cent. when properly immersed, falls to about 50 per cent. when breaking the surface of the water. As a result of a change from a diameter of 5 feet 10 inches to 4 feet 6 inches, the speed of the Ist Class Torpedo-boat was increased from 18 to 20 knots, other conditions remaining the same. This is a most important feature in the screw. It is a common thing to see screw-steamers, in their light condition, with the tips of the blades of the pro- peller 2 feet or 3 feet above the surface. This implies an immense loss of efficiency. When steam power has to be applied as an auxiliary to sails, it is best if possible to arrange to lift the screw out of the water. If disconnected MARINE PROPELLERS. 19 and allowed to revolve it still causes considerable resistance,. Last year, Messrs. Thornycroft sent the torpedo-boat Chi/ders out to Australia under steam and sail. The ordinary screws of these boats are so large in proportion to the midship section that they prevent the boat from making any speed under sail. A screw of the kind described by Griffiths, with perfectly flat blades set at an angle, was made, and the blades so atranged that they could be turned round so as to be in the same line as the shaft, thus affording no impediment to progress under sail. So far from realising Griffiths’ prediction, this propeller required just double the horse-power for a given speed, required by the ordinary propeller. When the screw cannot be raised out of the water, a screw with two narrow blades, which can be set up and down in a line with the stern-post, will probably be found to be the best. RACING. The racing of screws is due to either of two causes. If the propeller breaks the surface of the water as the stern rises in a sea-way, it will draw air down, and the resistance is immediately very much reduced. Referring to Plate I., showing the thrust at a given number of revolutions of a pro- peller, in one case completely immersed and also C2 20 MARINE PROPELLERS. when splashing, we see that in the former con- dition it exerts a thrust of 11 lb, at 680 revolu- tions. When it is drawing air, the same thrust is exerted at 1000 revolutions, so that we see that this propeller, if delivering a constant thrust, would vary its revolutions instantly from 680 to 1000 if alternately raised and lowered as in the action of pitching. But it is not only when the screw breaks the surface of the water that it will race. When a vessel is pitching heavily there may be racing, even although the screw does not rise within several feet of the surface. Mr. Froude pointed out that this was probably due to the oscillating motion of water in waves. There is no real motion of translation in waves. The water which is travelling in one direction at the crest returns in the opposite direction in the trough of a wave. This oscillating motion of the water extends to some distance below the surface. A screw therefore finds the resistance of the water alternately augmented or reduced, as it is beneath the trough or crest of a wave, and reduces or increases its speed accordingly. POSITION OF SCREW. It has been proposed, at various times, to place the. screw in the bow, on either side of the bow, on either side amidships, on either quarter, and in MARINE PROPELLERS. 21 a tunnel amidships. In a vessel recently built on the Thames, one screw was placed in the forefoot, and one aft, in the usual position, working on the same shaft. It was intended to realise a speed of 18 to 20 knots. The highest speed obtained has been about g knots. How much of this failure is due to the position of the screws I cannot say, but it is certain that the forward screw is in a very unfavourable position, as it causes a great increase in the surface friction of the hull. There is no doubt that the stern is the best position. As a vessel passes through the water, the fric- tion imparts motion to the layer of water rubbing against the sides and bottom. This layer increases in thickness toward the stern, so that, after the vessel has passed through, a considerable quantity of water is left with a motion in the same direction as the vessel. If the screw works in this water, it is able to recover some of the energy which has been ex- pended by the ship in giving it motion. The speed of this wake, which Rankine estimates may be as much as one-tenth the speed of the vessel, does not depend upon the form, but upon the nature and extent of the surface. It would not be desirable to manufacture or increase the speed of the wake for the purpose of improving the efficiency of the propeller, because this very surface friction proves 22 MARINE PROPELLERS. to be the largest portion of the resistance of the ship at moderate speed, but, as it is a necessity that there should be a wake, it is a distinct advan- tage to place the propeller in it, and allow it to utilise as much as possible of the energy it finds there. It is important not to confound this water, which has had motion given to it by the sides and bottom of the ship, with the wave of replacement ; that is, the water filling in behind the ship. It should be the aim to avoid interfering with this motion as much as possible, as such interference augments the resistance of the ship very consi- derably, even in well-formed ships. It was thought at one time that the further aft the propeller could be placed, the better, but it is now believed that there is a position where the loss caused by the augmented resistance of the hull is more than balanced by the reduction of slip in the screw due to its working more in the water that has been rubbed by the vessel. In the small, high-speed steam-launches, the propeller has been kept outside the rudder with advantage, but this is not practicable in the case of large steamers. All that can there be done is, to make the run fine, so that the water has given out upon the stern of the ship the energy put into it by the bow, before reaching the screw. If a screw-propeller is placed behind a bluff stern, so that its supply of water is imperfect, it MARINE PROPELLERS. 23 will draw in water at the centre of the driving face and throw it off round the tips of the blades, exactly like a centrifugal pump. The effect upon the ship is then peculiar. Sir Frederick Bramwell tells of a vessel which went astern whichever way the screw was driven. The reason was, that the bluff stern caused the screw to act as described, roducing a loss of pressure upon the stern of the vessel. A screw causes lateral motion to the stern of a vessel, which has to be counteracted by the rudder. This effect is very much greater when going astern than when going ahead, and I think that the cause is not the same in the two cases. When going ahead, Professor Osborne Reynolds has pointed out that the onward motion of the wake is very different at the surface and at the keel. Heagrees with Rankine that the mean-speed in a fine vessel may be 10 per cent. of the vessel’s speed, but thinks it varies from 20 per cent. at the surface to nif at the keel: the upper blade of the screw thereupon experiences more resistance than the lower, and drives the stern of the ship round. When going astern, this explanation does not hold. It will be generally observed that in going astern, the engines will go very much faster than when going ahead, will race in fact, at the same time causing very little effect upon the ship. The propeller is then drawing air, and the upper blades suffer most, so that the lower blades now 24 MARINE PROPELLERS. experience the most resistance, and drive the stern round. This takes place quite independently of the rudder, but Professor Reynolds has pointed out a very peculiar result which follows the reversing of the engine. If a vessel which is in motion has its engine suddenly reversed, and the helm put over before way is off the vessel, the head will fall off in exactly the opposite direction to that it should do from the position of the helm. It is thus explained— Suppose one vessel is in danger of collision with another approaching upon its starboard bow. If the helm is starboarded, and the engines at the same moment reversed in order to stop the way of the vessel, the water is driven away from the fore side of the rudder, and an increase of pressure produced upon the after side, driving the stern to port. The vessel, therefore, turns to starboard, and the danger of collision is increased. It is probable that the inequality in the onward motion of the layers of water forming the wake accounts to some extent for the vibration caused by the screw. Each blade in revolving, meets with an alter- nately diminished and increased resistance as it passes through the layers, and thus causes a series of shocks. It is probable, too, that this affords some explanation of the inefficiency of large screws. This inefficiency is, of course, partly due MARINE PROPELLERS. 25 to increased friction, but the larger the diameter the greater the inequality of motion of the water in which the upper and lower blades work. An ingenious mechanical arrangement was in- vented by Griffiths, by which the blades were able to adjust their pitch to suit the resistance. The blades in passing the upper part of the circle had their pitch reduced, while the opposite blades had their pitch correspondingly increased. The appara- tus would probably not stand much wear and tear. Twin screws possess very many advantages over a single screw, and do not appear to have any less efficiency. In very fine ships, the length of the outside shafting becomes a serious consideration, and the necessary support for it adds considerably to the resistance of the ship. It would probably be an advantage in such cases to allow the discs to overlap,* setting one screw in front of the other, and cutting a hole in the dead wood to allow the _ blades to pass through, as shown in Figs. 13 and teem. The reduced resistance of stern tube and appen- dage would probably more than compensate for any small reduction of efficiency of the screws. For very high-speed vessels, the use of several pro- pellers would enable the weight of the machinery to be kept down. * Screws set with discs overlapping have been fitted in the Buzzard, one of the small coasting steamers belonging to Mr. John Burns. 26 ALARINE PROPELLERS. Fic. 13. MARINE PROPELLERS. 27 The weight of an engine of a given type per I.H.P., varies inversely as the number of revolutions per minute. That is, the greater the number of revolutions the less the weight per I.H.P., because the cylinder capacity is reduced in proportion as FIG. 134. the revolutions are increased, and in similar engines working with the same steam-pressure, the weight per cubic inch of cylinder is nearly a constant quantity. Now the number of revolutions per minute at 28 MARINE PROPELLERS. which a propeller will work at its maximum effi- ciency, varies inversely as the diameter for a given speed. That is, the larger the diameter, the slower should be its rate of turning. The diameter varies as the square root of the I.H.P. for a given speed. Therefore the weight varies as the diameter of the propeller and as the square root of the I.H.P. In symbols— If W = weight of engine, not including boiler, per I.H.P., I Revs.’ We I Revs. « D’ D « /TH.P. “.We«D, 1. W & 4/LELP. To take an example :—If an engine of 900 I.H.P. can be made for 37°3 lb. per I.H.P., the weight per I.H.P. of a similar engine of 1800 I.H.P. would 4/1800 _ 4/900 speed of the engines is such as to allow each screw to run at the revolutions best suited for it. The weight of boilers also is affected when we pass to more than one boiler. A single locomotive boiler may be made to give out from 800 to 1000 I.H.P., but it will not be be 37'°3 x = 52:2 lb, supposing that the MARINE PROPELLERS. 29 possible to obtain this power out of several boilers at the same time. In the first place, there is a difficulty in regulating the supply of water to each boiler; but there is a greater difficulty still. A man can give his whole mind to one boiler, and will work it to its utmost limit, but ask him to do the same with half-a-dozen boilers, and he will certainly fail. The case of the Polyphemus is an example. There were in her ten locomotive boilers, and the horsepower required from each was only 500, but it could not be obtained. Every European navy now is asking for what are called torpedo- boat hunters ; that is, vessels of larger size than a torpedo-boat, and possessing equal or superior speed. We are frequently asked to design en- gines of large power for them, and are generally allowed a weight per I.H.P. based upon the results obtained with torpedo-boat engines of 700 or 800 I.H.P. It is inevitable, that as the power of the engines increases, the revolutions should be reduced and the weight increased, for at these speeds everything, as far as possible, must be designed to work in its best condition, and a large propeller will not work satisfactorily at the same speed as a small one, even if the engine would. By using several small propellers instead of one large one, the engines can be made to run at a high speed, and thus can be made light. 30 MARINE PROPELLERS. Another method would be to gear a number of engines upon one screw-shaft, so that while the engines would run at a high speed, the screw would turn at a slower speed adapted to its large diameter. The expedient of putting a number of engines tandem upon a shaft is only of value for keeping the height of the engines down, to get them under an armoured deck, or below the water-line. MARINE PROPELLERS. 31 LECTURE II. PROFESSOR RANKINE, in a paper on the theoretical limit of the efficiency of propellers,* which I would advise any one intending to pursue the subject to read, lays down a certain theoretical limit towards which the efficiency of propellers may be made to approximate by mechanical improvements, and points out certain causes which make the actual efficiency fall short of that limit. He states that, “If the propelling instrument be so constructed as to act on each particle of water at first with a velocity equal to the velocity of feed, and gradually increasing at an uniform rate up to the velocity of discharge, then the loss of work is the least possible.” It is certain that no actual propelling instrument has ever attained this limit of efficiency. The oar, when a uniform force is applied to it by the oars- man, thus producing a gradual acceleration of the water laid hold of by the blade, approaches more closely to it than the paddle or ordinary screw, and the guide-blade or screw-turbine propeller more closely still. * The ‘ Engineer,’ 1867, vol. xxiii. p. 25; and ‘ Miscel- laneous Scientific Papers, edited by W. J. Millar, p. 544. 32 MARINE PROPELLERS. There is a certain quantity of work which must be lost under all circumstances, and it is equal to the actual energy of the discharged water moving astern with a velocity relative to still water. As this energy varies as the weight multiplied by the square of the velocity, if we double the quantity of water acted upon, we double the loss from this cause, but if we double the velocity with which the water is discharged, we increase the loss fourfold. This shows the advantage of acting upon a large column of water and leaving it with as small a speed as possible relative to still water. It explains also why the jet propeller, which is forced to act upon a much less area of column than the screw, appears at such a disadvantage when compared with the latter. From the above considerations it would appear that the larger the diameter of a screw and the smaller the slip, the greater the efficiency would be. There is, however, an element which has not yet been considered, which imposes a limit to the size of a screw in order to obtain the best efficiency. This element is the friction of the screw blades. It is well known what a large proportion of the resistance of a ship is caused by the friction of the surface, and a screw is subject to exactly the same conditions. How large the effect of this element may be is shown by the case of H.M.S. /ris. This ship was MARINE PROPELLERS. 33 originally fitted with two four-bladed propellers 18 feet diameter and 18 feet pitch. She obtained a speed with these propellers of 15% knots with an expenditure of 6369 I.H.P. Two blades were then taken from each propeller, reducing the total number from eight to four. The I.H.P. then required for the same speed was 4369, or 2000 less H.P., and this 2000 I.H.P. was employed in driving the four additional blades. This was a very extraordinary and unexpected result. The causes of loss of work in propellers of different kinds may be thus summed up :— First. Suddenness of change from velocity of feed to velocity of discharge. Propellers which suffer from this cause are, the radial paddle-wheel and the common uniform pitch screw; while those which in varying degree avoid it are, the gaining pitch screw, the feathering paddle-wheel, Ruthven’s form of centrifugal pumps, and the oar. Second cause of loss, Transverse motion im- pressed on the water. Propellers which lose in efficiency from this cause are, ordinary screw-pro- pellers, which impart rotary motion ; radial wheels, which give both downward and upward motion in entering. and leaving the water, and oars, which impart outward and inward motions at the com- mencement and end of the stroke respectively. This loss is greatly reduced in the guide-blade propeller as the guides take the rotary motion out D 34 MARINE PROPELLERS. ” of the water and utilise it in so doing. It may be entirely avoided in the turbine propeller. Third cause of loss, Waste of energy of the feed- water. This is experienced by the jet-propeller only, as generally applied, and is one of the causes of its inefficiency. It is not necessary now to enter into any argument as to the superiority of the screw over the paddle-wheel. “Sz argumentum queris, cir- cumspice.’ The paddle-wheel has everywhere been driven out of the field by the screw, except in cases of vessels built for very shallow drafts, for which, until the successful introduction of the screw-turbine, it was alone available. Asa propelling instrument the paddle is not inferior to the screw, and some of the best recorded performances have been obtained with it. Owing, however, to the necessarily slow speed of revolution, the machinery for the paddle-wheel requires to be larger, costlier, heavier, and demands more space than screw engines of the same power. To ascertain the adaptability of the screw for’ towing purposes, an experiment was made in the early days of screw-propulsion. The Rattler and the Adecto, the former a screw, and the latter a paddle-wheel vessel of the same size and power, were lashed stern to stern, The Rattler towed the Adecto astern against the whole power of her engines at the rate of 2°8 knots per hour. MARINE PROPELLERS. 35 The revolutions and power of a screw are about the same whatever the speed of the vessel, and even if the vessel be moored, nearly the full power can be developed. If on the other hand a paddle- vessel is prevented from getting away at her proper speed, the full power of the engines cannot be de- veloped, and this explains why the Rattler had such an advantage; because her engines were developing 300 I.H.P. while the Alecto was only able to develop 140*I.H.P. Vessels intended for towing require propellers of much larger diameter than would otherwise be suitable. Some years ago it was proposed by M. Bazin, a Frenchman, to build a steamer to cross the Channel at a high rate of speed, the greater part of the floating power of which was to be supplied by six large hollow drums or wheels capable of revolving. The object of the design was to reduce the surface friction. The six wheels were caused to rotate by separate engines, while the propulsive power was obtained by screws in the ordinary way. It was supposed that the effect of friction upon the rotating wheels would be got rid of, and the speed of the vessel thereby greatly increased. Mr. W. Froude showed conclusively in one of the ablest investigations he ever made, that the resistance of such a vessel would be greatly in excess of that of aship-shape form. The immersed area of the central part is very large in proportion D2 36 MARINE PROPELLERS. to the displacement, and in addition, the resistance of the wheels to passage through the water is very great. The motion of the wheel through the water may be compared to the motion of a cart-wheel on land. Fic. 14. vb | P As the centre of the wheel moves from a to 4, the point P is stationary, that is to say, the wheel may for the moment be said to pivot about the point P. As the wheels are immersed nearly up to their centre, it is easily seen that so far from there being no surface friction, every portion of the surface except the point P is moving through the water and causing friction ; thus, while the centre moves from a to 4, the point ¢ moves to d, and similarly with any other point. MARINE PROPELLERS. 37 It is not necessary to assume that the stationary point is in the outer circumference. If the rolling floats be making positive slip, the point P will be in a circumference of less diameter than that of the floats, but the same construction holds. It can be proved that the float must make negative slip, and the point P will then be in a proportionably enlarged circumference. Mr. Froude calculates that the frictional resistance alone of the floats will be about half of what it would amount to if the wheels were locked and incapable of revolving. Altogether the form gives exceptionally great resistance. In 1879 a vessel called the Hydromotor was built in Germany, from the design of Dr. Fleischer. She was propelled by the reaction of jets of water. In this vessel, the water is acted upon directly by the steam without the intervention of a pump. The arrangement is as follows :—There is a cylin- der, lined inside with wood, at the bottom of which is a large pipe leading to a nozzle at the bottom of the vessel. A float of nearly the same diameter as the cylinder works up and down in it. The cylinder being now full of water, and the float consequently at the top, steam is admitted by a valve above the float, and driving it down, ejects the water through the nozzle. On reaching the bottom of its stroke, the float opens the exhaust, and the steam passes into the condenser. The vacuum thus created in the cylinder causes the water to rise partly through 38 MARINE PROPELLERS. the nozzle, but principally through a suction-valve in the bottom of the condenser. The cylinder is thus filled with water and the float rises to the top, in doing which it closes Fic. 15. the exhaust and opens the steam - valve, when the operation is repeated. The loss by conden- sation appears to have been less than might have been expected in a cylinder filled alter- nately with steam and with water, but as the cylinder is not entirely emptied at each stroke, a layer of boiling water always remains at the top and adheres to the wooden lining as the float descends. The data obtainable are unreliable, as no proper measured mile trials have been made. All calculations made upon indicated horse-power cards are of little value in this system, as the loss between the boiler and the indicator, which is probably large, is thereby ignored. The only correct basis for comparison with either screw or turbine propulsion, is coal consumption. MARINE PROPELLERS. 39 DESIGN OF PADDLE WHEELS. To find the sectional area of a pair of feathering floats of a paddle wheel for a given vessel at a given speed, working with a given slip in undis- turbed water. First estimate the probable resist- ance of the ship at the given speed, then fix upon a suitable slip—15 to 20 per cent. is a fair average. Then, if R = resistance, S = speed of centre of float relatively to the water, V = speed of the vessel, R Sey Leas If the wheel works in disturbed water, then, If A = area in undisturbed water, A, = » water having forward velocity, V =speed of ship, v = forward velocity of water, : AxV-v. i V-—24 To find the area of floats for radial wheels, pro- ceed as for feathering wheels, supposing the slip to be that of the lower edge of the float. In radial wheels the number of floats should equal the number of feet in the diameter, and 40 MARINE PROPELLERS. the breadth of a float may be # inch or I inch for each foot of diameter. In a feathering wheel, the floats should be half as numerous and twice as broad as the floats of a radial wheel. The width of the wheel should be from one-third to one-half the breadth of the ship. When fully laden the wheel should not be immersed to more than one-fourth its diameter. The size of the wheel is determined by the intended speed of the ship, the slip, and the number of revolutions considered most suitable, generally from 20 to 30 per minute, although sometimes as high as from 40 to 45 per minute. Example. Speed of ship, 15 knots = say 1500 feet per minute. Slip, 16 per cent. = say 300 +s - .’. Circumferential velo- city of wheel = 1800 ‘i 3 Revolutions, 30 per minute. Fic, 16, D x 3°14 X 30 = 1800 ‘, D= to feet. The floats of a feathering wheel are constructed to cleave the water without shock. If a in the above triangle (see Fig. 16) represent the motion of a descending float in a given time if MARINE PROPELLERS. 41 the vessel is stationary, and 4 = the travel of the ship in the same time. Then the actual path of the float is represented by the resultant. The plane of the float entering the water should coincide with this line. It is found in practice, that lines drawn from the summit of the wheel F (see Fig. 17), tothe points of Fic. 17. intersection of the circumference with the water-line B and D, give the direction of the floats with suffi- cient accuracy. Levers about three-fifths of the depth of the float are fixed perpendicularly at their centres Bé,Cc, Dd The centre of a circle, in the circumference of which the ends 4, c, and d of these three levers lie, is the centre of the eccentric necessary to produce the required motion of the floats. 42 MARINE PROPELLERS. MANUFACTURE OF SCREWS. Screws are generally made of cast iron in the mercantile marine, the whole propeller being a single casting. In the Royal Navy they are usually made of gun-metal and the blades cast separate from the boss, to which they are bolted, the holes in the flanges of the blades being elongated so as to allow the blades to be shifted round and the pitch ad- justed. In torpedo-boats the general practice is to make the blades of hammered steel and to key them on to the boss, as shown. The root of the blade is made wedge-shaped as well as the key, the latter being tapered in the direction of its length also. When this key is driven hard in, the blade is held absolutely fast without any projecting bolts or flanges. By making the blades of forged steel, they can be made very thin and sharp, which is a matter of great importance. A forged propeller is made as follows:—A wooden block is first prepared from the drawing. This is built up of layers of wood of equal thick- ness, the section of the blade at each layer being given on the drawing. From this block, an iron one is cast. MARINE PROPELLERS. 43 The blades are first forged flat and made roughly to the proper thickness and shape. They are then hammered on to the cast blocks and given the required twist. The roots are planed, and the blade ground smooth on a grindstone, care being taken that each blade shall weigh the same when finished. They are then keyed into the boss, also of forged steel, the grooves of which have been slotted to the required angle. The propeller is finally put upon a mandril and balanced. In order to do this it is of course necessary that not only shall the blades be of the same weight, but that the centre of gravity of each blade shall be at the same distance from the centre of the boss. When thus carefully balanced, the screw causes no vibration in the boat. SLIP OF SCREW. If v = speed of screw = revs. x pitch, V= » ship, ov _ v x 100 = percentage of apparent slip. The following are the average proportions of the screws of a few of the latest and largest ocean- going steamers. Slip per cent. from — 3 per cent. to 12 per cent. for four blades. Pitch, 1} times the diameter. Diameter, 20°7 feet. Pitch, 27°9 feet. 44 MARINE PROPELLERS. The pitch runs generally from 1 to 14 times the diameter, and is slightly increasing, being 5 per cent. less than the mean on the leading edge, and 5 per cent. more than the mean on the following edge. The surface of the blades is 35 per cent. of the disc area. Thickness at root of blade, $ inch to x inch per foot of diameter, and 2 inches from the tip, the thick- ness is about I inch or 1} inch. Rankine gives the following formula for the thickness of the blade. If D is the diameter of the shaft, De <2 No. of blades x length at root The factor 2 is to be used if the blades are of material having equal strength with the shaft, and 4 if of gun-metal. Having thus found the thickness at the axis, equal say toA C, Fig. 19, draw a straight line from C to the tip of the blade B. This will give the section of the blade at any point. As the top cannot be made quite sharp, it must be thickened up slightly. This method of construction does not give a blade of equal strength throughout, but a blade which, if it breaks at all, will probably break near the tip and leave a portion still available. It is sometimes useful to be able to estimate roughly the pitch of a screw at sight. This may be done by observing at what part of = thickness at axis. MARINE PROPELLERS. 45 the blade an angle of 45° is made with the axis. The pitch is equal to the circumference at this point. The pitch of the small models used for experi- mental purposes was rea- dily and accurately mea- sured in the following manner. A. wooden cylinder was: made having a diameter about two-thirds that of the propeller. A hole was bored through the axis into which the screw-shaft was fixed. A sheet of paper wrapped round the cylinder was cut accu- rately to fit the face of the screw-blade. The direction of the axis should be marked upon the paper. The paper is then taken off the cylinder and unrolled. If the propeller be of uniform pitch, the edge which fitted the face of the blade will form a straight line as y, Fig. 20. FIG. 20. 46 ASILARINE PROPELLERS. If # be the diameter of the cylinder, then 6 _ Pitch a2” £X 3°14" If the blade is not of uniform pitch, the template which fitted it will form a curved line. The pitch at the leading and after edge can be measured separately in the same manner, and the mean pitch found. MARINE PROPELLERS. 47 LECTURE III. IN the first of these lectures I said that the whole problem of screw-propulsion was to fix upon the best diameter of a propeller, and the best ratio of pitch to diameter under given conditions. I now propose to give what hints I can which will assist you in solving this problem. As the only way in which it is possible to arrive exactly at the resistance of a ship is by making experiments with a model, so the only exact way of arriving at the efficiency of a propeller is by experimenting upon a model. I will show directly how this should be done. But it is obvious that when it is required to design a propeller for a given ship, some simpler and more expeditious method than this must be resorted to. It is sufficient in most cases to take an actual propeller which is known to give a good per- formance and to treat that propeller as a model. It is advisable that the ship upon which the propeller you propose to take as your model is fitted, should be somewhat similar in general proportions. Then the following rules will enable you to find the diameter and revolutions suitable. 48 MARINE PROPELLERS. To find the diameter of a propeller for a given I.H.P. and a given speed from the diameter of another smaller similar propeller at a different 1.H.P. and a different speed. The diameter is proportional to the 4/I.H.P. and inversely proportional to the cube of the . Speed. If d = diameter of model, D = diameter of required propeller, 2 =1H.P. of model, P= 4 required propeller, v = speed of vessel with model propeller, V= 5 i ‘ required propeller, Then Dan/d x? x™. Example. If d = 5:0 feet, p = 670 I.H.P., v = 18 knots, P = 1800 L.H.P., V = 20 knots, Then D= =,/3" x pe 5 x. = 7 feet (if model smaller). 70 If the model is larger ratios are reversed. _670 Me =5 feet (if model larger). D= n/p x22 x ® ee 5 feet (if mo ger) MARINE PROPELLERS. 49 I would say here that in designing the machinery for a new vessel the thing to start with is the size of the propeller and not the size of the engines. The engines exist only to drive the propeller, and should be subordinated to it. Having therefore a given speed of vessel and a given horse-power to start with, fix upon the diameter of the propeller, then upon the revolu- tions suitable for the propeller. With these things fixed it is then easy to find the size of the engine. It is an entire reversal of the proper process to say, 1 will run my engine at such and such a speed and make a propeller to suit. Slight variation from the most suitable number of revolutions is admissible, more especially in the direction of increasing the number of revolutions for the sake of lightening the machinery, but the engine should not run at a slower speed than that dictated by the propeller, because, as will be presently shown, the efficiency of the pro- peller decreases very rapidly when it is run too slowly. To find the suitable number of revolutions for a given propeller at a given speed from the revolu- tions of a smaller similar propeller at a different speed. The revolutions per minute are proportional to the speed and inversely proportional to the diameter. E 50 MARINE PROPELLERS. If D = the diameter of given propeller, = es of smaller model, given speed, = speed of model, = revolutions of given propeller, i ss model, Then RerxY xf VWI dsR I D Example, If D = 7 feet, ad = 5 feet, V = 20 knots, v = 18 knots, ry = 400 revs., 20 5 Then R= 400 x = x al 318 revs. 18 If the model used is larger than the given propeller the ratios are reversed. The pitch of the propeller should then be made the same ratio to the diameter as in the model. When a screw has to be designed to suit certain engines and these engines do not run at the number of revolutions which would be best for the propeller, the diameter may be obtained as described and the pitch made such as will give a slip of about 15 per cent. The pitch should never exceed 24 times the diameter. @ MARINE PROPELLERS. 51 This may be looked upon as the outside limit. When the engines run very slowly a smaller amount of slip than 15 per cent. should be allowed for. In making experiments with models, it is necessary first to’fix upon the size of model which will be convenient. It must not be of such large size as to give too great a thrust, as the dynamo- metric apparatus is more convenient if moderately small. On the other hand, the scale of the mcdel must be sufficiently large to allow of accurate measurements of the results. About 9 inches diameter is a suitable size, as thrusts not exceeding 25 or 30 lb. will then have to be dealt with. The model is made as follows:—A wooden block is prepared from the reduced propeller drawing, a blade is moulded upon this block in paraffine, and a cast is taken in plaster of Paris. An alloy is run into this cast consisting of tin and aluminium, the latter in small proportions. This is sufficiently soft to allow of scraping and cutting with a knife, while being strong enough to retain its form. It of course does not rust. The cast blade is then filed and burnished and is accurately fitted to the block. The blades are secured in the boss by screws in such a way that the pitch may be varied to any desired extent. Tn our experiments a steam-launch was fitted E 2 52 MARINE PROPELLERS. up with a small shaft to carry the model through the bow, the shaft projecting sufficiently in front of the launch to ensure that the model should work in undisturbed water. This shaft could move very freely in its bearings to and fro, and the end of it was attached by means of a steel pianoforte-wire to a spring, so that the thrust exerted by the propeller could be recorded. This shaft was made to revolve by means of a gut working on toa pulley and driven by a small engine of I or 2 H.P. All that requires to be measured is :— 1. The thrust exerted by the model. 2. The revolutions of the model. 3. The speed of the launch. 4. The turning effort expended in driving the model. 5. Equal intervals of time. It is also necessary to measure the constant friction of the engine and shafting so as to get the true zero for the turning effort diagram. In order to obtain these different measurements we had a dynamometer consisting of a revolving drum driven at a uniform speed by means of clock- work. A piece of paper was wrapped round this drum. A number of pens over the drum were each connected to an electro-magnet in such a way that as long as no current flowed round the MARINE PROPELLERS. 53 magnet the pens were stationary and merely traced straight lines upon the paper as it revolved beneath them. a The moment contact was made, however, the pens gave a little jerk, making a lateral indent in the line. One pen was electrically connected with a small clock, so that it measured intervals of time, making an indent every twelve seconds. A second pen recorded the revolutions of the main engine driving the launch, these revolutions forming a check upon the speed of the launch. A third pen recorded the revolutions of the model, a counter on the shaft: making contact every 50 revolutions. The speed of the launch was measured by running backwards and forwards along a fixed distance on shore of 300 feet. The time of passing the posts was marked by an electric pen actuated by the observer pressing a button. As the observations were taken in a tideway two runs were necessary to determine the speed for every observation, one up stream and one down. Another pen was connected to the spring before mentioned, to which the model shaft was attached, and recorded the extension of the spring. The last pen shows the tension of the gut driving the model, and thus measures the turning effort expended. 54 MARINE PROPELLERS. This tension was obtained by the arrangement shown in Fig. 21, where 72 t= Px. 2l, Turning moment = (T. — T,) x 277 X revs. of 7. O ke-Le - Fic, 21. Ts T The speed of the launch being kept constant at from 4 to 44 knots, a number of observations were taken at different revolutions of the model, and these plotted as shown on Plate I. 1. Thrust line. MARINE PROPELLERS. 55 2. Work done by propeller in foot-lbs. being thrust x speed through the water. 3. Turning effort in foot-lbs. The work done divided by the work expended gives the’efficiency of the propeller. It will be seen that this reaches a maximum at a certain number of revolutions depending upon the propeller. It will be seen too that if run too slowly the efficiency falls very rapidly, but if too fast, not nearly so rapidly. This shows that if a propeller is too large, the efficiency will suffer largely, but a propeller may be made considerably smaller than its most suitable diameter without suffering much loss. The efficiency obtained by the model shown reached a maximum of °7. The result of several trials seemed to indicate that this was rather high. A more probable average for a good propeller is "65. If the propeller be tried at two or three different pitches, the variation being obtained by twisting the blades round on the boss, it can easily be found what ratio of pitch to diameter gives the best result. By trying it also with 2, 3, and 4 blades, the best ratio of surface to disc area can be determined. Having now found a good propeller, and at what thrust and number of revolutions it will work at maximum efficiency, a curve can be made, as shown in Plate II., giving the diameter, pitch, and number 56 MARINE PROPELLERS. of revolutions, for any speed and any horse- power. For instance, the model of the Thornycroft propeller whose performance is shown in Plate L, had a diameter of 9 inches, and gave its maximum efficiency when utilising 4000 foot-lbs.=*121 H.P. at 600 revs. and at 4°06 knots, the speed of the launch. Therefore the diameter for 1 H.P. at 4°06 knots Vfl f° 121 We can now plot the diameter for 1 H1.P. at any speed, because we know the area is inversely proportional to the cube of the speed. Therefore for 20 knots the diameter for one H.P. is a/ 28°85? x £08" = 2°6, and so on for any speed, Sins giving us the curve on Plate II. ‘Now take an example :— Diameter for 430 I.H.P. at 20 knots is 2'6 x 4/430 = 54 inches. This is the actual diameter of the propeller in 1st Class Torpedo-boats. Now take a propeller for the /rzs at 18} knots and 3867 H.P., the maximum H.P. put through one of her screws. From curve 2°85 inches x 4/3867 = 178 inches = 14°8 feet. As the pitch of the 9-inch model was 10°3 inches, = 9x = 28°5 inches. MARINE PROPELLERS. 57 178 inches ; = 204 inches 9 inches 4 Therefore 10'3 inches x = 17 feet pitch. The revolutions can be plotted in the same manner from the performance of the model, remembering, as before stated, that they are pro- portional to the speed, and inversely proportional to the diameter. From the curve we find the revolutions for one I.H.P. at 18} knots is 7800. The corresponding diameter being 2°85 inches. We have therefore for the /ris— 7800 X 2S 125 revs. per minute ; 178 or, more simply, dividing the revolutions found on the curve by the / 1.H.P.— Having made such a diagram as this, all we have to do is:— To find the diameter—Multiply the diameter found on the curve by the square-root of the given horse-power. To find the revolutions—Divide the revolutions found on the curve by the square-root of the given horse-power. * The screws of the /rzs are 16 feet in diameter and have a pitch of 20 feet, but the engines only run at 97 revolutions instead of 125. 58 MARINE PROPELLERS. THE JET PROPELLER. THERE are many reasons why what is called a jet propeller would be preferred in certain cases to a screw or a paddle if an economical result could be obtained from it. The large pumping power available in case of leaks, and the comparative safety of the propelling apparatus from accident, either from shot or from touching the bottom, or from fouling, render it tempting either for warlike or mercantile purposes. There are, however, so many drawbacks connected with it, and the efficiency of the apparatus is neces- sarily so small, that at the present moment I believe there is not a single vessel using the pro- peller for commercial purposes. Two years ago a torpedo-boat 66 feet long, pro- pelled by a centrifugal pump, was built by Mr. Thornycroft, for competition with a similar vessel fitted with a screw. Both vessels were of about the same size and displacement and the I.H.P. developed by each was the same. The speed obtained by the screw was 17°3 knots per hour, and by the hydraulic was 12°6. This latter speed was obtained by the screw-boat with about half the power exerted by the other ; that is to say, there is a loss of power corresponding to about 50 per cent. experienced by the jet pro- peller, compared with the screw. The causes of this loss are not hard to find. In MARINE PROPELLERS. 59 the case of the Waterwitch and other hydraulic vessels, the water is received into the ship through a hole in the bottom in such a way as to suddenly check all the velocity which it has relatively to the ship. In other words, the entering water strikes the ship and has the velocity of the ship impressed FIG. 22. upon it before it gets into the turbine. If the bottom is formed into a scoop, as shown in Fig. 22 and Plate IIL, and the water caused to change its direction gradually, without having its velocity relatively to the ship checked at all, then this cause of loss may be avoided. 60 MARINE PROPELLERS. In such a case, if the vessel is towed along with the turbine removed, the water is scooped up, passes through the casing of the turbine, and flows out at the nozzles. The water then would leave the nozzles with a velocity relative to the ship equal to the speed of the ship, and with no velocity relative to still water except such as was given by the friction of the passage. The second cause of loss is due to the small quan- tity of water acted upon, and the consequently high velocity with which it has to be discharged. The loss of work due to this cause varies as the square of the velocity of slip, as has been already explained. The reason why the quantity of water acted upon is of necessity small is that the size of the orifice which it is advisable to make in a ship’s bottom is necessarily restricted by structural con- siderations, and must be very small indeed com- pared to the size of a screw’s disc. Then again, the weight of water admitted into the ship is a serious consideration, as it represents so much loss of displacement. The third cause is the loss by the friction of the water in the pipes and passages, and by the sudden changes in direction which it is necessary to give the water in passing in through the bottom, and out through the sides in a fore-and-aft direction. For these reasons the hydraulic propeller is essentially wasteful. MARINE PROPELLERS. 61 In the screw and turbine competitive torpedo- boats the total efficiency of the propelling machinery was proved to be, screw 0°5 and turbine 0°254. I will now describe the propeller which is repre- sented by the model on the table, and which is called the screw-turbine propeller, being a sort of cross between a screw and a turbine. It will be seen that it has guide-blades behind the screw, as proposed by Rigg, but there is one very important feature in this propeller which was not in that of Rigg. It will be necessary first to recapitulate what I have already said about the advantage of gradually impressing the required velocity upon the water. When this is done—and this is a very important point to bear in mind—the loss from the slip is only one-half that experienced when the full velocity of discharge is impressed suddenly. If one propeller imparts the acceleration gradu- ally and another imparts it suddenly, the first one may havea final velocity of discharge of double that of the second, with the same efficiency, and therefore the propeller which accelerates gradually need act upon only half the quantity of water that its com- petitor does. In other words, the same reaction and efficiency. will be obtained from the propeller with the gradual acceleration as the other, although it have only half the disc area. 62 MARINE PROPELLERS. This causes it to be eminently suited for vessels of shallow draught. Now in what way does it differ from other increasing-pitch propellers, for all such propellers have this object more or less inview. They all fail, as may be easily shown. Suppose an ordinary increasing-pitch propeller, enclosed in a casing. (See Fig. 23.) Fic. 23. A certain quantity of water comes out of the casing at the final velocity of discharge, but however much water comes out at one end in a minute, the same quantity must go in at the other in the same time, and therefore it must go inat the same speed that it comesout. The propelling apparatus there- fore must accelerate the stream previously to its entry into the tube, and before being touched by the blades. Thus the advantage of the increasing pitch is lost. In the case of the screw-turbine, Fig. 24, the size of the channel is so proportioned as to exactly suit the speed of the water passing through it. Thus at MARINE PROPELLERS. 63 the fore end of the casing is a large opening which will admit a certain quantity of water at a velocity equal to that of the ship. Fic. 24. At the after end is a smaller channel, which will allow of the exit of the water at the accelerated velocity which has been imparted by the screw- blades in passing through it. The long tail is simply a prolongation of the boss to allow of the streams of water uniting gradually without forming eddies. As the greatly increasing pitch causes consider- able rotation of the water, the guide-blades are so formed as to direct the water into a straight line aft. The whole of the transverse motion caused by the propeller is thus utilised without loss. When this model was experimented upon, the thrust of the revolving blades was measured sepa- rately from the thrust of the fixed guides. The latter was found to be quite considerable ; 64 MARINE PROPELLERS. in the case of the model shown, as much as one- third of the total thrust. In the launch illustrated by the model on the table and by Plate IV., a further device was re- sorted to, in order to reduce the draught. A tunnel is formed in the bottom of the boat, the top of which rises above the surface, but the ends are submerged. In this tunnel a screw-turbine propeller 16 inches diameter is placed. As the boat has only 12 inches draught of water one-fourth of the diameter of the propeller is above the water level. As soon as the propeller starts, however, water is drawn up into this tunnel and the air is expelled, after which the tunnel remains full of water and the propeller works completely submerged. There is no loss.of power involved in lifting the water this 4 inches, because in falling it gives out the work employed in raising it. There is an incidental convenience in this arrange- ment. An air-tight door is placed at the summit of the tunnel, which can be taken off from inside the boat. As soon as air is admitted the water falls to the level of that outside and the propeller is partially emerged, thus offering peculiar facilities for exami- nation and for allowing it to be cleared if fouled. In the case of twin screws this operation can be performed upon one propeller while the other is still kept going slowly. Five large steamers, 140 feet by 21 feet, and MARINE PROPELLERS. 65 I foot 9 inches draught of water, are being built upon this principle by Mr. Thornycroft for the Nile expedition. They will be propelled by two screw-turbines of 32 inches diameter, raised in tunnels in the manner described.* A launch built last year, 56 feet long and 15 inches draught of water, attained a speed of 16} knots with one screw-turbine 20 inches diameter. * Since the delivery of these lectures, one of these vessels has been tried upon the measured mile, and obtained a speed of 15+ knots an hour. LONDON: PRINTED BY WILLIAM CLOWES AND SONS, LIMITED, STAMFORD STREET AND CHARING CROSS. F 7 / Lf, i Z yr Pel i 7 THUAN TORUTITrATENT-TIrUrecoen: OS DLAVDEST DITAT ST TV? WeEATCOrTT OTT Tt oO TITS ® Power eaperded in fiot-pounds, + Usetiul work in foot-pounds,; © Thrust in pounds. Datted lines shew same propeller splashing the wate: Fold out 20,000 ® @ i 15,000 é + 7 3 ® we LS, rs °O WS Cz - P<} / ° q 7 se ict / et J ex species ems / £ : . / % - v / & Zz. 0-€ S 7 & / Q I / 3 if = S e / : Ss / = 10,000 Z O-£ : 7 / x / 7 > % a ° / -7 & x A / a od ~~ @ ” ob ne] x e cher x S / Er Q < oh lee q ! a Z f 04 Ww 7 QS x + x 8 ts + Fe / +4 7 4 7 y + 7 ¢ / 7 30.0:3 / 7 ea Z + v4 / 5,000 a & / 5 ea wf S & ee at 20 ae /” Rg / 2 Lue 4) Set ol ee 7 ty 7 “lec Y ee — . t -~ = e S = “7 {0 0:1 ve baa ef a Ty 7) | | | 500 600 700 800 200 1000 1100 Plate 1 Revolutions per Minute. THORNYCROFT PATENT PROPELLER. 3 BLADES. DIAR 9 INS MEAN PITCH 10-3 INS ® Power capended inv tivt-pounds, + Usetiil work in foot -pounds, © Thrust in pounds. Datted lines shew same propella splashing the wate: ‘yattadOWd ANIGUNL MANOS HO J3qviG-aGINS HLIM dallid HONNYT Wyals 1885. BOOKS RELATING TO APPLIED SCIENCE PUBLISHED BY E. & F.N. SPON, LONDON: 128, STRAND. NEW YORK: 35, MURRAY STREET. | — o ' A Pocket-Book for Chemists, Chemical Manufacturers, Metallurgists, Dyers, Distillers, Brewers, Sugar Refiners, Photographers, Students, etc., etc. By THOMAS BAYLEY, Assoc. R.C, Sc. Ireland, Ana- lytical and Consulting Chemist and Assayer. “Third edition, with .. additions, 437 pp., royal 32mo, roan, gilt edges, 5s. Oo ae SYNOPSIS OF CONTENTS y\'). ‘ “Atomic Weights and Factors—Useful Data—Chemical Calculations—Rules for Indirect Analysis— Weights and Measures — Thermometers and Barometers— Chemical Physics — Boiling Points, etc.—Solubility of Substances—Methods of Obtaining Specific Gravity—Con- eversion of Hydrometers—Strength of Solutions by Specific Gravity—Analysis—Gas Analysis— ‘Water Analysis—Qualitative Analysis and Reactions—Volumetric Analysis—Manipulation— Mineralogy — Assaying — Alcohol — Beer — Sugar — Miscellaneous Technological matter relating to Potash, Soda, Sulphuric Acid, Chlorine, Tar Products, Petroleum,’ Milk, Tallow, Photography, Prices, Wages, Appendix, etc., etc. : The Mechanician: A Treatise on the Construction and Manipulation of Tools, for the use and instruction of Young Engineers and Scientific Amateurs, comprising the Arts of Blacksmithing and Forg- ing ; the Construction and Manufacture of Hand Tools, and the various Methods of Using and Grinding them ; the Construction of Machine Tools, and how to work them; Machine Fitting and Erection ; description of .. 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