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The Ordnance Survey and Geological Faults. IN view of the re-survey of the United Kingdom, it seems to me that if the officers of the Survey were directed to take special notice of the levels of the former survey on both sides of great geological faults, and to compare these levels now so as to ascertain if any appreciable relative change had taken place during the forty or fifty years since the first survey, valuable information as to the motion of these faults, if any, might be obtained.

This idea is mainly suggested to me by the fact that in this neighbourhood a great fault intersects the Old Red Sandstone close to its contact with the Highland schists, it has been traced from Stonehaven on the east coast to Loch Lomond on the west, and seems to give remarkable evidence of being, at least to a certain extent, in motion. The village of Comrie, famous for its "earthquakes," is situated on this fault, and the "earthquakes" are as lively as ever. In the valley of Strathmore farmhouses placed in the proximity of this great dislocation are, or were, celebrated for being "haunted," on account of the noises and tremors by which the inhabitants are from time to time

alarmed.

Most, if not all, British "earthquakes" have been, I think, wisely attributed to similar cau-es.

Of course fifty years is a very minute part of the history of one of these old faults, but if the data of the Ordnance Survey be so accurate as is usually supposed, some trace of shifting might possibly be discovered if the necessary observations were made. Newport, Fife, March 18. JAS. DURHAM.

The Discovery of the Potential.

MR. E. J. ROUTH has lately published a most valuable "Treatise on Analytical Statics." I quote from the second volume, p. 17, the following note :

"The earliest use of the function now called the potential, is due to Legendre in 1784, who refers to it when discussing the attraction of a solid of revolution. Legendre, however, expressly ascribes the introduction of the function to Laplace, and quotes from him the theorem connecting the components of attraction with the differential coefficients of the function. The name, Potential, was first used by Green," etc.

From this note it appears that the discovery of the potential must be attributed to Laplace. This is a wrong opinion, and some fifteen years ago Baltzer proved that the introduction of the function is due to Lagrange ("Zur Geschichte des Potentials," in Journal für die reine und angewandte Mathematik, vol. lxxxvi. p. 213, 1878). Some historical documents in favour of Lagrange's priority have been found, by the writer of these lines, in Todhunter's "History of the Mathematical Theories of Attraction and the Figure of the Earth," and collected in a note at the end of vol. i. of his work, "Il Problema Meccanico della Figura della Terra " (Torino, 1880), where a full account of the early history of the potential is given, with numerous bibliographical indications. OTTAVIO ZANOTTI BIANCO. Private Docent in the University of Turin, March 21.

THE historical note on p. 17 of my "Statics" is chiefly founded on the statements in Todhunter's "History," and in Thonson and Tait's "Natural Philosophy." The references to these two writers are given in the note. Both Dr. Todhunter and Lord Kelvin ascribe the introduction of the function for gravitation to Laplace, and assert that the name of "Potential' was first given to it by Green. My own reading, though not so extensive as theirs, had not led me to form any different opinion. In Nichol's "Cyclopædia of the Physical Sciences" the first introduction is given as due chiefly to Legendre, Lagrange, Laplace, and Poisson. In Chambers's "Cyclopædia" Laplace's name alone is mentioned. Baltzer, as cited by Mr. Bianco, mentions the use of the function by Lagrange in the Mém. de Berlin, 1777. This is earlier than the memoir of Legendre, but as Legendre assigns

the introduction of the function to Laplace, it is difficult to compare the dates. I am at present unable to refer either to the memoir of Lagrange or to the treatise of Mr. Bianco. E. J. ROUTH.

Van't Hoff's "Stereochemistry."

THE review of the above by "F. R. J." in NATURE, p. 436, raises some important points in connection with this peculiarly fascinating branch of chemical science. In referring to the recent ingenious and attractive theory of P. A. Guye, that the numerical value of optical activity is dependent upon the relative masses of the four groups attached to the asymmetric carbon atom, and which carries with it the corollary that if two of these four groups are of equal mass the rotatory power will cease, your reviewer states that Guye "was unable to verify this view in all strictness." I think, however, that he hardly emphasises sufficiently that this important corollary has in every case, when put to the test of direct experiment, broken down. As far as I am aware, there is not a single instance of an asymmetric carbon atom attached to four groups qualitatively distinct, being found optically inactive in consequence of two of those groups being quantitatively equal in mass. Indeed some such substances are not merely active but powerfully so. The reviewer considers that this inadequacy of Guye's theory is palliated by the alleged fact that the amount of rotatory power of the esters of an active acid is determined by the weight of the alkyl-group. This point, which is one of the cardinal pillars of Guye's theory, I have recently put to the test of actual experiment, by measuring the rotatory power of a number of the esters of active glyceric acid, which have been prepared by Mr. J. MacGregor and myself. In this investigation we found the most extraordinary verification of Guye's theory, as far as the optical properties of the normal series of methyl, ethyl, and propyl glycerates were concerned; with the appearance of isomerism, however, this regularity ceases, thus the isopropyl glycerate has a markedly lower rotation than the normal one, whilst the normal and secondary butyl compounds have a lower rotation than the isobutyl ester. Nor are these differences consistently explicable by taking into consideration the interatomic distances, as measured by atomic volume, for the molecular volume of the normal propyl glycerate with its greater rotation is less than that of the isopropyl compound with its smaller rotation, whilst the molecular volumes of the isobutyl and secondary butyl glycerates are almost exactly equal, although the rotation of the former is much greater than that of the latter.

The reviewer, in referring to the rotation exhibited by the salts of active acids, states that in the case of tartaric acid all the salts "display in solution the same rotatory power, irrespective of the atomic weight of the metal," and is apparently satisfied that "the clue to this anomaly is furnished by the electrolytic theory of Arrhenius," according to which "it is the ion CO(CHOHL CO, which is alone responsible for the rotation." The reviewer has in this endorsed the method of special pleading adopted by the advocates of this theory, in which the metallic tartrates have been summoned as witnesses, whilst only the testimony of those favourable to the theory has been admitted. Thus one of the commonest of the metallic salts of tartaric acid-tartar emetichas a rotation which differs entirely from that of the other tar trates, and thus conclusively negatives the dogma that the rotation of the solutions of metallic salts is independent of the particular metal which has replaced the hydrogen of the acid. Fresh light has been thrown on this point in the course of an investigation, which I have recently carried out with Mr. Appleyard on the rotatory power of the metallic salts of active glyceric acid, and which has shown that the specific rotatory power of the glyceric acid has one value when deduced from the rotations of its alkaline salts (lithium, ammonium, sodium,'and potassium), another value when deduced from the salts of the alkaline earths (calcium, strontium, and barium), and a third from the salts of the magnesium group of metals (magnesium, zinc, and cadmium). Now it so happens that almost the only salts of tartaric acid which have had their rotation determined are those of the alkaline metals, which also in the case of glyceric acid yield practically the same rotation. Hence if only the rotations of the alkaline glycerates had been determined, the same erroneous conclusion would have been arrived at concerning the rotation of glyceric acid. Whatever may be the ultimate interpretation put upon these new results, and I prefer for the present to ab

stain from any generalisations, it is obvious that the notion of the rotatory power of saline solutions being independent of the particular metal present in the salt is altogether untenable. PERCY F. FRANKLAND.

University College, Dundee, March 11.

THE notice referred to by Prof. Percy F. Frankland was written, and the proof returned to the printer, before the end of last year. Since then two researches have been published -by Purdie and Walker, and by Frankland and Appleyardin which facts are adduced, apparently irreconcilable with Guye's theory. Had these facts been at my disposal I should doubtless have expressed myself more guardedly.

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Prof. Frankland says: "As far as I am aware, there is not a single instance of an asymmetric carbon atom attached to four groups qualitatively distinct, being found optically inactive in consequence of two of those groups being quantitatively equal in mass; and he complains that I have hardly emphasised this sufficiently. My reason was, that I was not altogether convinced of the fact, as may be seen from the following passage, which I transcribe, and which originally formed a footnote to the notice in question :

"The present reviewer ventures to suggest that cases such as are sought by Guye are to be found in those compounds in which two of the four different groups attached to an asymmetric carbon atom are themselves asymmetric carbon atoms of equal and opposite enantiomorphism. Such compounds would exist in two distinct forms; but as the two opposite enantiomorphic groups would be of equal mass and would be situated at equal distances from the central asymmetric carbon atom to which they are attached (inasmuch as the two opposite enantiomorphic modifications of a compound always have the same molecular volume), the conditions necessary for optical inactivity according to Guye's theory would be fulfilled, and neither of the two forms ought to cause rotation of the polarised ray. Such a case has already been observed in the two inactive, non-racemic trihydroxyglutaric acids described by Emil Fischer (Ber. der deutsch. chem. Ges. 24, p. 4214), although it does not appear to have been hitherto interpreted from this point of view.'

"

I afterwards suppressed this footnote, partly because it seemed to me out of place in such a notice, and partly because the optical activity of the two trihydroxyglutaric acids could be accounted for in another way: namely, by the fact that, as pointed out by E. Fischer, the mirror images of their molecules are congruent with the molecules themselves. But the passage will show why I was indisposed to enter a proved negative against Guye's theory.

As regards the charge of "endorsing special pleading" in the interests of the electrolytic theory of Arrhenius by suppressing the fact that tartar emetic has, in solution, a different rotation from the other metallic tartrates, I may say at once that I was ignorant of this fact. I am not a specialist on the subject of the optical properties of organic compounds, and I merely summarised, doubtless uncritically, the account of Oudemans' law given in van't Hoff's book. Indeed, the brief notice, as its wording everywhere indicated, was a summary rather than a criticism.

I take this opportunity of rectifying an omission. At the time of writing the notice I was not aware that Prof. Crum Brown had, independently of M. Guye, put forward, in the Proceedings of the Royal Society of Edinburgh, views on the influence of the various substituting radicles in modifying the optical rotation of organic compounds. F. R. JAPP. University of Aberdeen, March 18.

Standard Barometry.

THE question of absolute accuracy in barometer readings is one of great importance to meteorologists; but there has been so much uncertainty shown by the accumulated facts relating to the subject, that I think that no one who has carefully studied the matter has felt fully satisfied that strictly comparable international standards had been obtained. An uncertainty of at least o'I mm. was indicated by the various international comparisons of normal barometers which have been carefully made and discussed during the past ten years. I think that at last a definite conclusion has been reached, and that the very recent results published in paper No. 4, Band xvi. of the Repertorium für Meteorologie will be accepted as proving that at St. Petersburg at least normal readings are obtained.

About twenty-five years ago Director Wild, of the Central Physical Observatory at St. Petersburg, established the first normal barometer of the modern form; and as much as twenty years ago he claimed to have obtained practically normal readings. Moreover, he urged that the transfer of these normal readings from place to place by means of portable barometers was impossible within the desired limits of accuracy, and that each country ought to have its own thoroughly investigated normal barometer. This last has been proved by the results obtained by various investigators; and now Prof. Wild offers the proof of the accuracy of his normal barometer in the paper just referred to, which bears the title "Die normal-barometer des Physikalischen Central-Observatoriums zu St. Petersburg.' This paper was presented to the Academy of Sciences on November 4, 1892, and in it Wild gives the results of the intercomparison of three local normal barometers.

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Normal barometer No. I. was mounted at St. Petersburg in 1870, and was fully described in Band iii. of the Repert. f. Meteor.

A second normal barometer was mounted at Pawlowsk (about twenty miles from St. Petersburg) in 1887, and a third normal was mounted at St. Petersburg in 1891, and is known as normal No. II.

In 1887 and 1888 Wild found that the St. Petersburg normal I. and the Pawlowsk normal did not differ by more than o ́OI

mm.

In 1892 the St. Petersburg normals I. and II. were found to agree within the limit of error of observation (less than o'oi mm.).

In 1892 the St. Petersburg Normal II. was dismounted, taken to Pawlowsk, and there compared with the Pawlowsk normal, and the two were found to differ by only oor or o'02 mm. ; that is '004 or '008 inch. It must be added that these comparisons have all been checked by means of comparisons with portable barometers of the highest class.

The paper by Prof. Wild is accompanied by illustrations of these various normal barometers. The St. Petersburg normal has recently undergone some alterations, and these are also fully described. Altogether this is perhaps the most important contribution to the subject that has appeared since Prof. Wild's famous memoir of 1873; for we can now rest assured that farther refinement is not required by any practical demands.

It seems to me that now that we are sure of the accuracy of Wild's normal, it is more necessary than ever that we should know with greater certainty its relation to the principal standards of Europe. I desire, therefore, to propose a plan by which a series of comparisons can be carried out for a few places at a very slight expense, and with as much accuracy as portable instruments will permit. In 1883 it became my duty to transport to America, from Hamburg three of the Wild-Fuess portable barometers of the highest grade; and it was of great importance to take every possible precaution against their being injured or their condition altered in any way so as to affect their readings. I devised a mounting on shipboard which was very satisfactory, and gave me no cause for uneasiness regarding the barometers, even in stormy weather. So many barometers are sent out from England to almost every country that I strongly urge the use of a similar arrangement in all cases where it is desirable to retain an assigned barometer correction.

The accompanying sketch shows my manner of mounting the barometers. Two small strips of wood, AA, are screwed to the woodwork running lengthwise of the vessel. They are placed about two feet apart, and are inclined at an angle of perhaps 45°. Small leather straps, say 15 inches long, are fastened to these strips by single screws as shown at BB. A rather soft stuffed flat cushion or pillow is now placed again.st the woodwork (wall) as shown at C. The box containing the barometer is now pressed against the cushion and the two extremities are placed within the grasp of the straps BB. These last are buckled and drawn tight enough to hold the barometer box firmly against the cushion C. The barometer is thus held in such a manner that no ordinary jarring can cause any damage to it, as there is no direct contact with a rigid surface, since the pillow prevents it from touching the wooden strips, and the soft yielding straps have a spring-like effect.

The lower part of the sketch shows the barometer box DD in position, with the barometer shown within it. Of course the cistern is held uppermost. On account of the jarring motion of the ship's screw in rough weather, it is desirable to locate the barometers well amidship, and also have the cistern of the baro

meter directed towards the stern. Barometers can be placed in this manner on ship board by the maker, and can be left to themselves for any length of time. If the person to whom they are consigned is notified of their subsequent arrival at port, he can take them from their hangings on the ship in the best possible condition. Of course this presupposes an arrangement with the officers of the vessel, such that the instruments shall be let entirely alone from the time they are mounted by the consignor until they are received by the consignee.

I think this method of carrying instruments can be very usefully applied in improving our knowledge of the relation of international barometric standards, and at a minimum expense; and I will give a brief outline of a convenient way for accomplishing it. The Deutsche Seewarte at Hamburg, and the Kew Observatory at Richmond (through the London Meteorological Office), are in the best positions for supervising this work, and I venture to express the hope that the matter will be seriously considered.

I will outline the work when carried on from London.

Let two barometers of the best construction, say an Adie Fortin and a Wild-Fuess control barometer, be compared with the Kew normal during a period of a week or more, or long enough to experience considerable variation in the barometer

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instruments to Washington for comparison with the normal there, and then return them to New York and put them on shipboard to be returned to London.

The standard barometers of Australia, India, Brazil, and other countries accessible by sea can be reached from London (or Hamburg) in the same way, and the comparison instruments can be returned to their starting point for additional verification. My own experience in the transportation of barometers assures me that ship captains would gladly give their hearty co operation to a work of this kind, and there would be no charges for carrying the instruments even half round the world and back again.

In offering this suggestion it is not necessary for me to give the details for the complete organisation of such a scheme; but it may be remarked that if it should be undertaken, the personal experience of those who have been over the ground should be utilised in making plans. A single instance will serve to show why this is advisable. Some years ago I carried two barometers from Hamburg to London by sea. I took the German line of steamers and found myself anchored in the middle of the Thames, and had to get ashore as best I could. I greatly feared that I should never get the barometers ashore in a whole condition, as there was necessitated a great deal of scrambling over lighters, &c., and embarkation in an unsteady row boat in order to make a landing. Had I taken the English steamer, all this worry would have been saved. Other similar instances occurred which could have been avoided by one personally familiar with the routes to be travelled. FRANK WALDO.

Princeton, New Jersey, February 20.

Motion of a Solid Body in a Viscous Liquid. THERE is perhaps no branch of mathematical physics which has made greater progress during the last thirty-five years than hydrodynamics. During this period numerous important investigations have been published upon the motion of solid bodies in a frictionless liquid, upon the theory of discontinuous motion, upon the theory of vortex motion and vortex rings, upon the motion of a liquid ellipsoid under the influence of its own attraction, and upon waves and tides. These investigations constitute an enormous increase in the knowledge possessed by the present generation compared with that of its predecessors; they have to a considerable extent exhausted the field of research in the theory of the motion of frictionless liquids; but notwithstanding the importance of the results, the elegance of the methods by which many of them have been obtained, and the skill by which the mathematical difficulties have been surmounted, all the investigations referred to possess the defect of not accurately representing the motion of liquids as they occur in nature.

The reason of this discrepancy between theory and observation is that the ideal substance, which is called a frictionless liquid, has no actual existence, for all liquids which occur in nature are viscous. The viscosity of the mobile liquids, such as water, alcohol, &c., is a small quantity, being in thecase of water equal to a tangential stress of about 014 dynes per square centimetre; whilst in the case of the sticky and greasy liquids, such as treacle and oil, it is much greater. The viscosity of olive oil is about 325 dynes per square centimetre, and is therefore about 232 times as great as that of water.

height. Then let the two barometers be mounted on one of the London Hamburg steamships, in the manner which I have described, and sent to Hamburg, where an employee of the Deutsche Seewarte could be despatched to take down the instruments and carry them to the Seewarte for comparison with the normal barometer. Then the barometers could be taken by a messenger to Lübeck, at an expense of a few shillings, and mounted on a St. Petersburg steamer, which would carry them almost to the door of the Central Physical Observatory, where they could be again taken in charge by a meteorologist, compared for a few days, and then again be mounted on another steamer bound for one of the Scandinavian ports where there is a standard barometer, and finally returned to London by one of the numerous regular steamships. At an expense of a couple of pounds the barometer could be sent from St. Petersburg (or Scandinavia) back to Hamburg via Stettin and Berlin; thus allowing Berlin to enter into the series. The barometers would probably have to be sent by a messenger from Berlin to Hamburg, thus entailing the just mentioned expense. A second comparison at Hamburg would be desirable, and then the barometers could be returned to London by sea, and again compared at Kew.

Similarly, barometers could be sent to New York for comparison with the sub-standard, by Adie, at the Maritime Exchange; although probably the United States Weather Bureau would assume the expense of the three pounds necessary to carry the

The mathematical theory of the motion of viscous liquids was elaborated as long ago as 1845 by Sir G. Stokes, in a paper in which he showed that the effect of viscosity might be represented by certain additional terms in the equations of motion of a frictionless liquid, which contain as a factor a new physical quantity called the viscosity. In a subsequent paper, published in 1850, he applied the above theory to calculate the diminution of the amplitude of the small oscillations of a sphere surrounded by water; and by means of experiments in which this quantity was observed, he calculated the numerical value of the viscosity of water, and found that it was in close agreement with the value found by Poiseulle from experiments on the flow of liquids through capillary tubes. An investigation of a similar character was undertaken by von Helmholtz and Piotrowski about 1863, in which the sphere was suspended by a torsion fibre, and made to perform small torsional oscillations about a diameter.

Almost all calculations relating to small oscillations proceed upon the basis that the squares and products of quantities, upon which the disturbed motion depends, may be neglected. This introduces a great simplification into the work, and enables a variety of problems, which would otherwise be exceedingly intractable,

› be solved by fairly simple methods. There is, however, nother class of problems of great practical importance, in which is not allowable to neglect these quadratic terms, and towards le solution of such problems theory has as yet made little

rogress.

When a sphere is constrained to move along a horizontal raight line, but is otherwise free, it is well known that if the urrounding liquid is supposed to be frictionless, its only effect to increase the inertia of the sphere by half the mass of the quid displaced. The sphere accordingly requires a larger npulsive force to start it than if the liquid were absent, but hen once started it continues to move with its velocity of proction. But when the sphere is surrounded by an actual quid, its velocity gradually diminishes until it ultimately comes Orest; and this fact shows very forcibly the necessity of taking he viscosity of the liquid into account in problems of this chaacter. I obtained a few years ago a mathematical solution, hich shows that this effect must necessarily be produced by a iscous liquid, but the solution is an imperfect one, as mathenatical difficulties compelled me to disregard the quadratic

erms.

motion is not symmetrical with respect to an axis, it cannot be expressed in terms of; but if the velocities of the liquid can be found from the hydrodynamical equations, the components of the linear and angular momenta of the liquid can be calculated, and by applying the principle of momentum to the compound system composed of the solid and the surrounding liquid, the equations of motion of the former can be obtained. Since the momentum of the system is obviously a function of the six coordinates of the solid, this principle furnishes a sufficient number of equations for the determination of the motion.

When there is more than one solid, the principle of momentum is insufficient to determine the motion; but if the velocities of the liquid in the neighbourhood of each solid could be found, the force and couple constituents of the resistance could be calculated, and the equations of motion of each solid written down. Lagrange's equations in their ordinary form cannot be employed, as viscous motion involves a conversion of energy into heat; but problems which can be solved by an indirect method can usually be solved by a direct one, and I feel confident that equations analogous to Lagrange's equations exist, by means of which the motion of a number of solids in a viscous It is always a great advantage when the solution of a mathe- liquid can be found without going through the above-mentioned natical problem can be made to depend upon a single function process. A form of Lagrange's equations has already been diswhich satisfies a partial differential equation and certain boundary covered, which is applicable when the viscous forces depend conditions. This is always the case when a solid of revolution upon a dissipation function which is expressible as a homogeneous noves along its axis in a viscous liquid which is initially at rest, quadratic function of the velocities; and the circumstance that or has an independent motion which is symmetrical with respect a dissipation function also exists in the hydrodynamical theory, o the axis. In this particular class of problems, the motion can although it is expressed in a different form, furnishes additional De expressed by means of Stokes's current function in the follow-grounds for believing in the existence of equations of this chang manner :-Let z be measured along, and perpendicularly racter. The discovery of such equations would constitute an o the fixed straight line with which the axis coincides during important advance in the theory of viscous liquids. he motion; let w and u be the velocities of the liquid in these A. B. BASSET. lirections; then :

:

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and is the kinematic coefficient of viscosity.
So far as I am aware, no serious attempt has been made to
obtain a solution of this equation in a suitable form, even when
The solid is a sphere. The equation is well worthy of the
attentive consideration of mathematicians; and although it is an
intractable one, it must be recollected that a general solution is
not required, but only a particular one which is suitable in the
case of a sphere. It will be quite time enough to consider the
possibility of obtaining solutions of a more general character,
when the appropriate one in the case of a sphere has been dis-
covered. It is also important to recollect that in most problems
which are of practical interest, is a small quantity (about *014
in C.G.S. units for water), and consequently an approximate
solution in which is supposed to be small would meet the
exigences of the case.

When a solid body is moving through a liquid, one of the boundary conditions is that the normal velocity of the solid must be equal to the component along the normal of the velocity of the liquid in contact with it. If the liquid is frictionless, this condition is the only one which has to be satisfied; but when the liquid is viscous, a further question arises as to the law which expresses the effect of the tangential stress exerted by the liquid pon the solid. When the motion is very slow (as in the case of problems relating to small oscillations) the experimental evidence is in favour of the hypothesis of no slipping; but when the velocity is considerable, the experimental evidence is not so satisfactory. The partial slipping which takes place under these circumstances must depend partly upon the nature of the liquid, and partly upon that of the surface in contact with it; and the tangential stress to which it gives rise is probably approximately proportional to the square of the relative velocity.

When the motion is symmetrical with respect to an axis, the stresses due to viscosity can be calculated as soon as the value of is known, the resistance which the liquid exerts on The solid can be found, and the equation of motion written down and integrated. This process is, however, an exceedingly tedious one; but it can always be dispensed with in the case of a single solid by employing the principle of momentum. When the

SCIENCE IN THE PUBLIC SCHOOLS AND
IN THE SCIENTIFIC BRANCHES OF THE
ARMY.

ΟΝ

N Friday last Mr. Campbell Bannerman received a deputation on this subject in his room in the House of Commons. There were present Sir Henry Roscoe, the Head Master of Rugby School, the Principal of Cheltenham College, the Head Master of Clifton College, Sir B. Samuelson, Prof. Jelf, and Mr. Shenstone. Lord Playfair, Sir John Lubbock, and Sir Henry Howorth would also have been present, but they were prevented by other engagements. The following is a brief account of the proceedings :

Sir Henry Roscoe, in introducing the deputation, said that he had introduced a deputation on this subject to Mr. Stanhope about five years ago, and that if the suggestions then made had been adopted the present deputation would not have been necessary. After some remarks which showed the injustice of the present system to the more scientific lads, he pointed out several methods by which this injustice might be removed.

The Head Master of Rugby, Dr. Percival, expressed his strong feeling of the importance of the subject alike to the service, the cadets, and the schools, and said he wished to see both modern languages and science duly encouraged; re thought they might both be made compulsory, as he believed that early education should rest on a wide basis, and that specialising should only be encouraged later. Alluding to the work in science done at the Royal Military Academy, Dr. Percival mentioned that he knew of one cadet who, owing to the absence of any higher teaching there at the earlier stages, was lately learning science which he, the cadet, was well fitted to teach.

The Principal of Cheltenham College, Mr. James, confessed that his own interests and convictions on educational matters were those of a linguist rather than those of a man of science; but practical experience showed him that the present system told most unfairly against scientific boys who entered Woolwich; science was being gradually edged out. Many other head masters of public schools felt with the deputation. He thought also that the present system tended to the disadvantage of the smaller schools, where science was often exceedingly well taught. He hoped that in making any changes the authorities would be careful to consider the interests of linguistic boys, and

would not add to the number of subjects taken up at entrance, for boys were already overburdened in their preparation.

The Head Master of Clifton College, Mr. Glazebrook, said that this was a question on which the public schools had a strong claim to be heard, since an increasing number of boys passed direct from them to Woolwich-the proportion last July being about four-fifths of all the candidates. But the discouragement of science was not so serious to the great schools as to the smaller and less expensive schools, where as a rule science is well taught, but not German. He thought it undesirable that these latter should be debarred from competition. It was not only by the assignment of marks that science was now discouraged, but also by the system of instruction. Boys who went up to Woolwich tolerably proficient in chemistry were put back to the elements, and at the end of their first year knew less than when they entered. Such boys were naturally inclined to complain that science at Woolwich was a farce, and to urge their friends at school to take up another subject which was treated more seriously.

Further remarks were made by Sir B. Samuelson, who especially advocated the encouragement of all types of boys from the public schools, by Prof. Jelf, and by Mr. Shenstone. Statements were made by the Director-General of Military Education and the Inspector-General of Fortifications; the latter officer emphasised the importance of German and of electricity, and said many cadets were markedly deficient in the latter subjects when they left Woolwich. In concluding, Mr. Campbell- Bannerman expressed his obligation to the deputation, and his sense [of the importance of the matter brought under his notice, which would

have his most careful attention.

It will be seen from this report that the position of cadets of scientific ability at the Royal Military Academy is, as we pointed out some time ago, far from satisfactory, and that this view is now not only held by men of science but also by many head masters and by distinguished members of the military profession, who on this and on other occasions recently have spoken clearly on the subject.

The main defects of the present system seem to be:(1) That science and German, two subjects which ought to go hand in hand in the early education of officers of the scientific branches, are at present brought into distinct conflict; (2) that in effect so great a bonus is given to German in the course of work at the Royal Military Academy as to be likely very soon to drive science out of the entrance examination, and to a corresponding extent out of the public schools; (3) that the standard of work of the cadets in science, and particularly in electricity when they leave the Royal Military Academy, is lower than it ought to be in very many cases.

Of these defects the last, which is doubtless largely the outcome of the first two, is probably the most important, and it will never be remedied so long as the authorities cling to the idea that a sufficient knowledge of several branches of science can be given to the cadets, even when they are quite new to such studies, in the moderate amount of time that can be spared for them during the comparatively brief course of work at the Royal Military Academy. That this idea is wrong we have pointed out again and again. If those who are responsible for the education of the cadets at Woolwich really desire that the cadets shall attain to a higher standard in science, they must not only encourage the admission of lads of scientific ability, but they must either set apart much more time to such work at the Academy, and give opportunities for, and more encouragement to, advanced work on the part of those who take up the subject, and do well in it at the entrance examination; or, if the giving of more time to science at the Royal Military Academy is impracticable, as is very possibly the case, they must so alter the conditions of the entrance examination as to secure that the cadets shall learn their elementary chemistry and heat at school, and be able to devote their science work at Woolwich wholly to electricity, which is technically of such great importance to

them, but to which at present they can only give a pr.: of their time.

By doing this the authorities of the Academy v only advance the interests of the service, they w 1 avoid that discouragement of the more scientific: and of the teaching of science in schools which mittedly a result of the present system as a whole

In conclusion, we would urge strongly what was p out by Sir Henry Roscoe on Friday, that it is not scientific knowledge but scientific ability which is w and that it is only by giving due weight to science & entrance examination and afterwards that this a secured.

CLIMBING PLANTSA

THIS forms the fourth part of A. F. W. Schurre "Botanische Mittheilungen aus den Tropea, is devoted to the description and illustration various adaptations for climbing exhibited by Brazilian plants observed on the spot. Fol.. Darwin, the author distinguishes four different c of climbing plants, according to the manner in they climb; but his four classes are not quite the s Darwin divided them into those having stems. twine spirally round a support; those which cam means of irritable organs; those which climb by of hooks; and those which climb by means of Darwin's investigations, it will be remembered, chiefly directed to the elucidation of the pheno exhibited by twiners, and such plants as climb be of tendrils. Schenck treats in a general way of all classes of climbers; and his work is more in the of a text-book than an account of experimental ree He divides climbing plants into Spreizklimmer, W.kletterer, Windepflanzen, and Rankenpflanzen, sponding nearly to the hook, root, twining, and te climbers of Darwin and others. But the Spre mer include all climbing plants that neither twres possess either irritable climbing organs or clinging ! whether armed or unarmed. Thus the least organ climbing plants are those having weak, slender, stems and branches which grow up among other and rest upon them without any other meas port; whilst the most perfectly developed dir plants are those provided with highly sensitive n.-" tendrils, such as the Cucurbitaceae and the Pas It is difficult to find an exact English equivale "Spreizklimmer," but "incumbent climbers employed to designate this class. Twiners rexit? the sun, as the hop (Humulus Lupulus), or agains sun, as the scarlet-runner bean (Phaseolus but Schenck agrees with Darwin and other that they are not sensible to contact. It is only be classed as tendril-climbers that exhibit this pr and this irritability is developed both in caulomes. phyllomes-that is in branches and in leaves, more ir modified for the purpose. In England there three woody climbers, namely: the ivy, a rou2-7 the honeysuckle, a twiner; and Clematis ali ne stalk climber; but in Brazil, and in other countries, they are exceedingly numerous, and great variety of adaptations to this end. Dr Sch however, does not confine himself to Bratwa. Þ* He briefly reviews all the types that have come ar observation. Plants climbing by means of tend table organs), conceived in the widest, classified according to the organs, o par organs, by means of which they climt P takes the leaf-climbers, which climb by m

1 "Beiträge zur Biologie und Anatomie ler Lien In P Brasilien einheimischen Arten." Mit 7 Tafel. Va (Jena: Gustav Fischer, 1892.)

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