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COLLEGE SECOND SERIES WITH AN AUTOBIOGRAPHY OF THE AUTHOR LONGMANS, GEE EN, AND CO. 39 PATERNOSTER ROW, LONDON NEW YORK, BOMBAY, AND CALCUTTA 1908 All rights reserved Av •>" ^ BIBLIOGRAPHICAL NOTE. Issued in Silver Library, March 1893; Reprinted July 1895, May 1898, June 1900, December 1903, August 1908. PEEFAOB. THE FAVOUR with which the first series of Professor Helmholtz's Lectures has been received would justify, if a justifi cation were needed, the publication of the present volume. I have to express my acknowledgments to Pro- fessor G. Croome Eobertson, the editor, and to Messrs. Macmillan, the publishers of ' Mind,' for permission to use a translation of the paper on the * Axioms of Modern Geometry ' which appeared in that journal. The article on ' Academic Freedom in German Universities ' contains some statements respecting the Universities of Oxford and Cambridge to which ex- ception has been taken. These statements were a fair representation of the impression produced on the mind of a foreigner by a state of things which no longer exists in those Universities, at least to the same extent. The reform in the University system, which 47^42 vi PREFACE. may be said to date from the year 1854, has brought about so many alterations both in the form and in the spirit of the regulations, that older members of the University have been known to speak of the place as so changed that they could scarcely recognise it. Hence, in respect of this article, I have availed myself of the liberty granted by Professor Helmholtz, and have altogether omitted some passages, and have- slightly modified others, which would convey an erro- neous impression of the present state of things. I have also on these points consulted members of the University on whose judgment I think I can rely. In other articles, where the matter is of prime importance, I have been anxious faithfully to repro- duce the original ; nor have I in any such cases al- lowed a regard for form to interfere with the plain duty of exactly rendering the author's meaning. E. ATKINSON. PeRTE«BERY HlLL, CA.MBEELEY : Dec. 1830. CONTENTS. tBCTTTBE PAQS I. GUSTAV MAGNVS. IN MEMORIAM . , . i II. ON THE ORIGIN AND SIGNIFICANCES OF GEOMETRICAL AXIOMS 27 IIT. ON THE RELATION OF OPTICS TO PAINTING . . 73 i. Form „ 7?, H. Shade 94 in. Colour . . . . . . . . .110 IV. Harmony of Colour 124 IV. ON THE ORIGIN OF THE PLANETARY SYSTEM . .139 V. ON THOUGHT IN MEDICINE 199 VL ON ACADEMIC FREEDOM IN GERMAN UNIVERSITIES . 237 VII. HERMANN VON HELMHOLTZ. Au AUTOBIOGRAPHICAL SKBICH . , 206 GUSTAV MAGNUS. Address delivered in the Leibnitz Meeting of the Academy of Sciences on July 6, 1871. . THE honourable duty has fallen on me of expressing in the name of this Academy what it has lost in Gustav Magnus, who belonged to it for thirty years. As a grateful pupil, as a friend, and finally as his successor, it was a pleasure to me as well as a duty to fulfil such a task. But I find the best part of my work already done by our colleague Hofmann at the request of the German Chemical Society, of which he is the Pre- sident. He has solved the difficulty of giving a pic- ture of the life and work of Magnus in the most com- plete and most charming manner. He has not only anticipated me, but he stood in much closer and more intimate personal relation to Magnus than I did ; and, on the other hand, he is much better qualified than £ II. S GUSTAV MAGNUS. to pronounce a competent judgment on the principal side of Magnus's activity, namely, the chemical. Hence what remains for me to do is greatly re- stricted. I shall scarcely venture to speak as the biographer of Magnus, but only of what he was to us and to science, to represent which is our allotted task. His life was not indeed rich in external events and changes ; it was the peaceful life of a man who, free from the cares of outer circumstances, first as member, then as leader of an esteemed, gifted, and amiable family, sought and found abundant satisfaction in scientific work, in the utilisation of scientific results for the instruction and advantage of mankind. Hein- rich Gustav Magnus was born in Berlin on May 2, 1802, the fourth of six brothers, who by their talents have distinguished themselves in various directions. The father, Johann Matthias, was chief of a wealthy commercial house, whose first concern was to secure to his children a free development of their individual capacity and inclinations. Our departed friend showed very early a greater inclination for the study of mathe- matics and natural philosophy than for that of lan- guages. His father arranged his instruction accor- dingly, by removing him from the Werder Gymnasium and sending him to the Cauer Private Institute, in which more attention was paid to scientific subjects. From 1822 to 1827 Magnus devoted himself en- GUSTAV MAGNUS. 3 tirely to the study of natural science at the University of Berlin. Before carrying out his original intention of qualifying as a professor of technology, he spent two years with that object in travelling ; he remained with Berzelius a long time in Stockholm, then with Du- long, Thenard and Gay-Lussac in Paris. Unusually well prepared by these means, he qualified in the University of this place in technology, and afterwards also in physics ; he was appointed extraordinary pro- fessor in 1834, and ordinary professor in 1845, and so distinguished himself by his scientific labours at this time, that nine years after his habilitation, on January 27, 1840, he was elected a member of this Academy. From 1832 until 1840 he taught physics in the Artillery and Engineering School ; and from 1850 until 1856 chemical technology in the Gewerbe Institut. For a long time he gave the lectures in his own house, using his own instruments, which gradually developed into the most splendid physical collection in existence at that time, and which the State afterwards purchased for the University. His lectures were afterwards given in the University, and he only retained the laboratory in his own house for his own private work and for that of his pupils. His life was passed thus in quiet but unremitting activity; travels, sometimes for scientific or technical studies, sometimes also in the service of the State, and » 2 4 GUSTAV MAGNUS. occasionally for recreation, interrupted his work here from time to time. His experience and knowledge of business were often in demand by the State on various commissions; among these may be especially men- tioned the part he took in the chemical deliberations of the Agricultural Board (Landes-Economie Colle- gium), to which he devoted much of his time ; above all to the great practical questions of agricultural chemistry. After sixty-seven years of almost undisturbed health he was overtaken by a painful illness towards the end of the year 1869.1 He still continued his lectures on physics until February 25, 1870, but dur- ing March he was scarcely able to leave his bed, and he died on April 4. Magnus's was a richly endowed nature, which under happy external circumstances could develop in its own peculiar manner, and was free to choose its activity according to its own mind. But this mind was so governed by reason, and so filled, I might almost say, with artistic harmony, which shunned the*immoderate and impure, that he knew how to choose the object of his work wisely, and on this account almost always to attain it. Thus the direction and manner of Magnus's activity accorded so perfectly with his intellectual nature as is the case only with the happy few among 1 Carcinoma recti. GUSTAV MAGNUS. 5 mortals. The harmonious tendency and cultivation of his mind could be recognised in the natural grace of his behaviour, in the cheerfulness and firmness of his disposition, in the warm amiability of his intercourse with others. There was in all this, much more than the mere acquisition of the outer forms of politeness can ever reach, where they are not illuminated by a warm sympathy and by a fine feeling for the beautiful. Accustomed from an early age to the regulated and prudent activity of the commercial house in which he grew up, he retained that skill in business which he had so frequently to exercise in the administration of the affairs of this Academy, of the philosophical faculty, and of the various Government commissions. He retained from thence the love of order, the tendency towards the actual, and towards what is practically attainable, even although the chief aim of his activity was an ideal one. He understood that the pleasant enjoyment of an existence free from care, and intercourse with the most amiable circle of relatives and friends, do not bring a lasting satisfaction ; but work only, and unselfish work for an ideal aim. Thus he laboured, not for the in- crease of riches, but for science ; not as a dilettante and capriciously, but according to a fixed aim and in defatigably ; not in vanity, catching at striking dis- coveries, which might at once have made his name celebrated. He was, on the contrary, a master of faith- 6 GUSTAV MAGNTS. fui, patient, and modest work, who tests that work again and again, and never ceases until he knows there is nothing left to be improved. But it is also such work, which by the classical perfection of its methods, by the accuracy and certainty of its results, merits and gains the best and most enduring fame. There are among the labours of Magnus masterpieces of finished perfection, especially those on the expansion of gases by heat, and on the tension of vapours. Another master in this field, and one of the most experienced and distinguished, namely, Eegnault of Paris, worked at these subjects at the same time with Magnus, but without knowing of his researches. The results of both investigators were made public almost simul- taneously, and showed by their extraordinarily close agreement with what fidelity and with what skill both had laboured. But where differences showed themselves, they were eventually decided in favour of Magnus. The unselfishness with which Magnus held to the ideal aim of his efforts is shown in quite a character- istic manner, in the way in which he attracted younger men to scientific work, and as soon as he believed he had discovered in them zeal and talent for such work by placing at their disposal his apparatus, and the appli- ances of his private laboratory. This was the way in which I was brought in close relation to him, when I found myself in Berlin for the purpose of passing the Government medical examination. GUSTAV MAGNUS. 7 He invited me at that time (I myself would not have ventured to propose it) to extend my experiments on fermentation and putrefaction in new directions, and to apply other methods, which required greater means than a young army surgeon living on his pay could provide himself with. At that time I worked with him almost daily for about three months, and thus gained a deep and lasting impression of his goodness, his unselfishness, and his perfect freedom from scientific jealousy. By such a course he not only surrendered the ex- ternal advantages which the possession of one of the richest collections of instruments would have secured an ambitious man against competitors, but he also bore with perfect composure the little troubles and vexations involved in the want of skill and the hastiness with which 3roung experimentalists are apt to handle costly instruments. Still less could it be said that, after the manner of the learned in other countries, he utilised the work of the pupils for his own objects, and for the glorification of his own name. At that time chemical laboratories were being established according to Liebig's precedent : of physical laboratories — which, it may be observed, are much more difficult to organise — not one existed at that time to my knowledge. In fact, their institution is due to Magnus. In such circumstances we see an essential part of thft inner tendency of the man, which must not by 8 GJSTAV MAGNUS. neglected in estimating his value : he was not only an investigator, he was also a teacher of science in the highest and widest sense of the word. He did not wish science to be confined to the study and lecture-room, he desired that it should find its way into all conditions of life. 'In his active interest for technology, in his zealous participation in the work of the Agricultural Board, this phase of his efforts was plainly reflected, as well as in the great trouble he took in the preparation of experiments, and in the ingenious contrivance of the apparatus required for them. His collection of instruments, which subsequently passed into the possession of the University, and is at present used by me as his successor, is the most eloquent testimony of this Everything is in the most perfect order : if a silk-thread, a glass tube, or a cork, are required for an experiment, one may safely depend on finding them near the instrument. All the appa- ratus which he contrived is made with the best means at his disposal, without sparing either material, or the labour of the workman, so as to ensure the success of the experiment, and by making it on a sufficiently large scale to render it visible as far off as possible. I recol- lect very well with what wonder and admiration we students saw him experiment, not merely because all the experiments were successful and brilliant, but because they scarce' y seemed to occupy or to disturb his GUSTAV MAGNUS. 9 thoughts. The easy and clear flow of his discourse went on without interruption; each experiment came in its right place, was performed quickly, without haste or hesitation, and was then put aside. I have already mentioned that the valuable collec- tion of apparatus came into the possession of the University during his lifetime. He specially wished that what he had collected and constructed as appli- ances in his scientific work should not be scattered and estranged from the original purpose to which he had devoted his life. With this feeling he bequeathed to the University the rest of the apparatus of his labora- tory, as well as his very rich and valuable library, and he thus laid the foundation for the further development of a Public Physical Institute. It is sufficient in these few touches to have recalled the mental individuality of our departed friend, so far as the sources of the direction of his activity are to be found. Personal recollections will furnish a livelier image to all those of you who have worked with him for the last thirty years. If we now proceed to discuss the results of his researches it will not be sufficient to read through and to estimate his academical writings. I have already shown that a prominent part of his activity was directed to his fellow-creatures. To this must be added. 10 GUSTAV MAGNUS. that he- lived in an age when natural science passed through a process of development, with a rapidity such as never occurred before in the history of science. But the men who belonged to such a time, and co- operated in this development are apt to appear in wrong perspective to their successors, since the best part of their work seems to the latter self-evident, and scarcely worthy of mention. It is difficult for us to realise the condition of natural science as it existed in Germany, at least in the first twenty years of this century. Maguus was barn in 1 802 ; I myself nineteen years later ; but when I go back to my earliest recollections, when I began to study physics out of the school-books in my father's posses- sion, who was himself taught in the Cauer Institute, I still see before me the dark image of a series of ideas which seems now like the alchemy of the middle ages. Of Lavoisier's and of Humphry Davy's revo- lutionising discoveries, not much had got into the school-books. Although oxygen was already known, yet phlogiston, the fire element, played also its part. Chlorine was still oxygenated hydrochloric acid; potash and lime were still elements. Invertebrate animals were divided into insects and reptiles ; and in botany we still counted stamens. It is strange to see how late and with what hesita- tion Germans applied themselves to the study of natural GUSTAV MAGNUS. 11 ricience in this century, whilst they had taken so promi- nent a part in its earlier development. I need only name Copernicus, Kepler, Leibnitz, and Stahl. For we may indeed boast of our eager, fearless and unselfish love of truth, which flinches before no authority, and is stopped by no pretence ; shuns no sacrifice and no labour, and is very modest in its claims on worldly success. But even on this account she ever impels us first of all to pursue the questions of prin- ciple to their ultimate sources, and to trouble ourselves but little about what has no connection with funda- mental principles, and especially about practical con- sequences and about useful applications. To this must be added another reason, namely, that the independent mental development of the last three hundred years, began under political conditions which caused the chief weight to fall on theological studies. Germany has liberated Europe from the tyranny of the ancient church ; but she has also paid a much dearer price for this freedom than other nations. After the religious wars, she remained devastated, impoverished, politi- cally shattered, her boundaries spoiled, and arrogantly handed over defenceless to her neighbours. To deduce consequences from the new moral views, to prove them scientifically, to work them out in all regions of intellec- tual life, for all this there was no time during the storm of war ; each man had to hold to his own party, every 12 GUSTAV MAGNUS. incipient change of opinion was looked upon as treach- ery, and excited bitter wrath. Owing to the Eeformation, intellectual life had lost its old stability and cohesion ; everything appeared in a new light, and new questions arose. The German mind could not be quieted with outward uniformity; when it was not convinced and satisfied, it did not allow its doubt to remain silent. Thus it was theology, and next to it classical philo- logy and philosophy, which, partly as scientific aids of theology, partly for what they could do for the solution of the new moral, sesthetical, and metaphysical prob- lems, laid claim almost exclusively to the interest of scientific culture. Hence it is clear why the Protes- tant nations, as well as that part of the Catholics which, wavering in its old faith, only remained out- wardly in connection with its church, threw itself with ST tch zeal on philosophy. Ethical and metaphysical prob- lems were chiefly to be solved ; the sources of knowledge had to be critically examined, and this was done with deeper earnestness than formerly. I need not enume- rate the actual results which the last century gained by this work. It excited soaring hopes, and it cannot be denied that metaphysics has a dangerous attraction for the German mind ; it could not again abandon it until all its hiding-places had been searched through and it had satisfied itself that for the present nothing more is to be found there. GUSTAV MAGNUS. 13 Then, in the second half of the last century, the rejuvenescent intellectual life of the nation began to cultivate its artistic flowers ; the clumsy language trans- formed itself into one of the most expressive instru- ments of the human mind ; out of what was still the hard, poor, and wearisome condition of civil and political life, the results of the religious war, in which the figure of the Prussian hero-king only now cast the first hope of a better future, to be again followed by the misery of the Napoleonic war, — out of this joyless existence, all sensitive minds gladly fled into the flowery land opened out by German poetry, rivalling as it did the best poetry of all times and of all peoples ; or in the sublime aspects of philosophy they endeavoured to sink reality in oblivion. And the natural sciences were on the side of this real world, so willingly overlooked. Astronomy alone could at that time offer great and sublime prospects ; in all other branches long and patient labour was still necessary before great principles could be attained ; before these subjects could have a voice in the great questions of human life; or before they became the powerful means of the authority of man over the forces of nature which they have since become. The labour of the natural philosopher seems narrow, low, and insignificant compared with the great conceptions of the philosopher and of the poet ; it was only those 14 GUSTAV MAGNUS. natural philosophers who, like Ok en, rejoiced in poetical philosophical conceptions, who found willing auditors. Far be it from me as a one-sided advocate of scien- tific interests to blame this period of enthusiastic ex- citement ; we have, in fact, to thank it for the moral force which broke the Napoleonic yoke; we have to thank it for the grand poetry which is the noblest treasure of our nation ; but the real world retains its right against every semblance, even against the most beautiful ; and individuals, as well as nations, who wish to rise to the ripeness of manhood must learn to look reality in the face, in order to bend it to the purpose of the mind. To flee into an ideal world is a false re- source of transient success ; it only facilitates the play of the adversary ; and when knowledge only reflects itself, it becomes unsubstantial and empty, or resolves itself into illusions and phrases. Against the errors of a mental tendency, which cor- responded at first to the natural soaring of a fresh youth- ful ambition, but which afterwards, in the age of the Epigones of the Romantic school and of the philosophy of Identity, fell into sentimental straining after sub- limity and inspiration, a reaction took place, and was carried out not merely in the regions of science, but also in history, in art, and in philology. In the last departments, too, where we deal directly with products GUSTAV MAGNUS. 15 of activity of the human mind, and where, therefore, a construction a priori from the psychological laws seems much more possible than in nature, it has come to be understood that we must first know the facts, be- fore we can establish their laws. Gustav Magnus's development happened during the period of this struggle ; it lay in the whole tendency of his mind, that he whose gentle spirit usually en- deavoured to reconcile antagonisms, took a decided part in favour of pure experience as against speculation. If he forbore to wound people, it must be confessed that he did not relax one iota of the principle which, with sure instinct, he had recognised as the true one ; and in the most influential quarters he fought in a twofold sense ; on the one hand, because in physics it was a question as to the foundations of the whole of natural sciences ; and on the other hand, because the University of Berlin, with its numerous students, had long been the stronghold of speculation. He con- tinually preached to his pupils that no reasoning, however plausible it might seem, avails against actual fact, and that observation and experiment must de- cide ; and he was always anxious that every practicable experiment should be made which could give practical confirmation or refutation of an assumed law. He did not limit in any way the applicability of scientific methods in the investigation of inanimate nature, but 16 GUSTAV MAONUS. in his research on the gases of the blood (1837) he dealt a blow at the heart of vitalistic theories. He led physics to the centre of organic change, by laying a scientific foundation for a correct theory of respira- tion; a foundation upon which a great number of more recent investigators have built, and which has developed into one of the most important chapters of physiology. He cannot be reproached with having had too little confidence in carrying out his principle ; but I must confess that I myself and many of my companions formerly thought that Magnus carried his distrust of speculation too far, especially in relation to mathe- matical physics. He had probably never dipped very deep in the latter subject, and that strengthened our doubts. Yet when we look around us from the stand- point which science has now attained, it must be con- fessed that his distrust of the mathematical physics of that date was not unfounded. At that time no separa- tion had been distinctly made as to what was empirical matter of fact, what mere verbal definition, and what only hypothesis. The vague mixture of these ele- ments which formed the basis of calculation was put forth as axioms of metaphysical necessity, and pos- tulated a similar kind of necessity for the results. I need only recall to you the great part which hypo- theses as to the atomic structure of bodies played GUSTAV MAGNUS. J7 In mathematical physics during the first half of this century, whilst as good as nothing was known of atoms ; and, for instance, hardly anything was known of the extraordinary influence which heat has on mole- cular forces. We now know that the expansive force of gases depends on motion due to heat ; at that period most physicists regarded heat as imponderable matter. In reference to atoms in molecular physics, Sir W. Thomson says, with much weight, that their assump- tion can explain no property of the body which has not previously been attributed to the atoms. Whilst assenting to this opinion, I would in no way express myself against the existence of atoms, but only against the endeavour to deduce the principles of theoretical physics from purely hypothetical assumptions as to the atomic structure of bodies. We now know that many of these hypotheses, which found favour in their day, far overshot the mark. Mathematical physics has acquired an entirely different character under the hands of Grauss, of F. E. Neumann and their pupils, among the Germans; as well as from those mathe maticians who in England followed Faraday's lead, Stokes, W. Thomson, and Clerk-Maxwell. It is now understood that mathematical physics is a purely ex- perimental science ; that it has no other principles to follow than those of experimental physics. In our immediate experience we find bodies variously formed n. 0 18 GUSTAV MAGNUS. and constituted ; only with such can we make our observations and experiments. Their actions are made up of the actions which each of their parts contributes to the sum of the whole ; and hence, if we wish to know the simplest and most general law of the action of masses and substances found in nature upon one another, and if we wish to divest these laws of the accidents of form, magnitude, and position of the bodies concerned, we must go back to the laws oi action of the smallest particles, or, as mathematicians designate it, the elementary volume. But these are not, like the atoms, disparate and heterogeneous, but continuous and homogeneous. The characteristic properties of the elementary volumes of different bodies are to be found experi- mentally, either directly, where the knowledge ol the sum is sufficient to discover the constituents, or hypothetically, where the calculated sum of effects in the greatest possible number of different cases must be compared with actual fact by observation and by experiment. It is thus admitted that mathe* matical physics only investigates the laws of action of the elements of a body independently of the acci- dents of form, in a purely empirical manner, and is there> fore just as much under the control of experience as what are called experimental physics. In principle they are not at all different, and the former only con- GUSTAV MAGKUS. 19 tinues the function of the latter, in order to arrive at still simpler and still more general laws of phenomena. It cannot be doubted that this analytical tendency of physical inquiry has assumed another character; that it has just cast off that which was the means of placing Magnus towards it in some degree of antago- nism. He tried to maintain, at least in former years, that the business of the mathematical and that of the experimental physicist are quite distinct from one another; that a young man who wishes to pursue physics would have to decide between the two. It appears to me, on the contrary, that the conviction is constantly gaining ground, that in the present more advanced state of science those only can experi- mentalise profitably who have a clear-sighted know- ledge of theory, and know how to propound and pursue the right questions ; and, on the other hand, only those can theorise with advantage who have great practice in experiments. The discovery of spectrum analysis is the most brilliant example within our recollection of such an interpenetration of theoretical knowledge and experimental skill. I am not aware whether Magnus subsequently ex- pressed other views as to the relation of experimental and mathematical physics. In any case, those who regard his former desertion of mathematical physics as a reaction against the misuse of speculation carried c2 20 GUSTAV MAGNUS. too far, must also admit that in the older mathema- tical physics there are many reasons for this dislike, and that, on the other hand, he received with the greatest pleasure the results which Kirchhoff, Sir W. Thomson, and others had developed out of new facts from theoretical starting-points. I may here be permitted to adduce my own experience. My re- searches were mostly developed in a manner against which Magnus tried to guard; yet I never found in him any but the most willing and friendly recognition. It is, however, natural that every one, relying upon his own experience, should recommend to others, as most beneficial, the way which best suits his own nature, and by which he has made the quickest pro- gress. And if we are all of the same opinion that the task of science is to find the Laws of Facts, then each one may be left free either to plunge into facts, and to search where he might come upon traces of laws still unknown, or from laws already known to search out the points where new facts are to be dis- covered. But just as we all, like Magnus, are op- posed to the theorist who holds it unnecessary to prove experimentally the hypothetical results which seem axioms to him, so would Magnus — as his works decidedly show — pronounce with us against that kind of excessive empiricism which sets out to discover facts which fit to no rule, and which also try carefully GUSTAV MAGNUS. 21 bo avoid a law, or a possible connection between newly discovered facts. It must here be mentioned that Faraday, another great physicist, worked in England exactly in the same direction, and with the same object; to whom, on that account, Magnus was bound by the heartiest sympathy. With Faraday, the antagonism to the phy- sical theories hitherto held, which treated of atoms and forces acting at a distance, was even more pro- nounced than with Magnus. We must, moreover, admit that Magnus mostly worked with success on problems which seemed specially adapted to mathematical treatment; as, for instance, his research on the deviation of rotating shot fired from rifled guns ; also his paper on the form of jets of water and their resolution into drops. In the first, he proved, by a very cleverly arranged experi- ment, how the resistance of the air, acting on the ball from below, must deflect it sideways as a rotating body, in a direction depending on that of the rotation ; and. how, in consequence of this, the trajectory is de- flected in the same direction. In the second treatise, he investigated the different forms of jets of water, how they are partly changed by the form of the aper- ture through which they flow, partly in consequence of the manner in which they flow to it ; and how their resolution into drops is caused by external agitation. 22 GUSTAV MAGNUS. He applied the principle of the stroboscopic disk in observing the phenomena, by looking at the jet through small slits in a rotating disk. He grouped the various phenomena with peculiar tact, so that those among them which are alike were easily seen, and one elucidated the other. And if a final mechanical explanation is not always attained, yet the reason for a great number of characteristic features of the indi- vidual phenomena is plain. In this respect many of his researches — I might specially commend those on the efflux of jets of water — are excellent models of what Goethe theoretically advanced, and in his phy- sical labours endeavoured to accomplish, though with only partial success. But even where Magnus from his standpoint, and armed with the knowledge of his time, exerted himself in vain to seize the kernel of the solution of a difficult question, a host of new and valuable facts is always brought to light. Thus in his research on the thermo- electric battery, where he correctly saw that a critical question was to be solved, and at the conclusion de- clared: 'When I commenced the experiment just described, I confidently hoped to find that thermo- electrical currents are due to a motion of heat.' In this sense he investigated the cases in which the thermo-electrical circuit consisted of a single metal in which there were alternately hard portions, and such as GUSTAV MAGNUS. 23 had been softened by heat; or those in which the parts in contact had very different temperatures. He was convinced that the thermo-electrical current was due neither to the radiating power, nor to the conduc- tivity for heat, using this expression in its ordinary meaning, and he had to content himself with the ob- viously imperfect explanation that two pieces of the same metal at different temperatures acted like dis- similar conductors, which like liquids do not fall in with the potential series. The solution was first furnished by the two general laws of the mechanical theory of heat. Magnus's hope was not unfulfilled. Sir W. Thomson discovered that alterations in the conductivity for heat, though such as were produced by the electrical current itself, were indeed the sources of the current. It is the nature of the scientific direction which Magnus pursued in his researches, that they build many a stone into the great fabric of science, which give it an ever broader support, and an ever growing height, without its appearing to a fresh observer as a special and distinctive work due to the sole exertion of any one scientific man. If we wish to explain the importance of each stone for its special place, how difficult to procure it, and how skilfully it was worked, we must presuppose either that the hearer knows the entire history of the building, or we must explain it to him, by which more time is lost than I can now claim. 24 GUSTAV MAGNUS. Thus it is with Magnus's researches. Wherever he has attacked, he has brought out a host of new and often remarkable facts ; he has carefully and accurately observed them, and he has brought them in connection with the great fabric of science. He has, moreover, bequeathed to science a great number of ingenious and carefully devised new methods, as instruments with which future generations will continue to discover hidden veins of the noble metal of everlasting laws in the apparently waste and wild chaos of accident. Magnus's name will always be mentioned in the first line of those on whose labours the proud edifice of the science of Nature reposes ; of the science which has so thoroughly remodelled the life of modern humanity by its intellectual influence, as well as by its having subju- gated the forces of nature to the dominion of the mind. I have only spoken of Magnus's physical labours, and have only mentioned those which seemed to me characteristic for his individuality. But the number of his researches is very great, and they extend over wider regions than could now be grasped by any single inquirer. He began as a chemist, but even then he inclined to those cases which showed remarkable phy- sical conditions ; he was afterwards exclusively a physicist. But parallel with this he cultivated a very extended study of technology, which of itself would alone have occupied a man's life. GUSTAV MAGNUS. 25 He has departed, after a rich life and a fruitful activity. The old law that no man's life is free from pain must have been applied to him also ; and yet his life seems to have been especially happy. He had what men generally desire most ; but he knew how to ennoble external fortune by putting it at the service of unselfish objects. To him was granted, what is dearest to the mind of a noble spirit, to dwell in the centre of an affectionate family, and in a circle of faithful and distinguished friends. But I count his rarest happi- ness to be that he could work in pure enthusiasm for an ideal principle ; and that he saw the cause which he served go on victoriously, and develop to unheard of wealth and ever wider activity. And in conclusion we must add, in so far as thoughtfulness, purity of intention, moral and intellec- tual tact, modesty, and true humanity can rule over the caprices of fortune and of man, in so far was Magnui the artificer of his own fortune ; one of the most satis- factory and contented natures, who secure the love and favour of men, who with sure inspiration know how to find the right place for their activity ; and of whom we may say, envious fact does not embitter their successes, for, working for pure objects and with pure wishes, they would find contentment even without external successes. ON THE OKIGIN AND SIGNIFICANCE OP GEOMETBICAL AXIOMS. Lecture delivered in the Docenten Verein in Heidelberg, in the year 1870. THE fact that a science can exist and can be de- veloped as has been the case with geometry, has always attracted the closest attention among those who are interested in questions relating to the bases of the theory of cognition. Of all branches of human knowledge, there is none which, like it, has sprung as a completely armed Minerva from the head of Jupiter ; none before whose death-dealing Aegis doubt and in- consistency have so little dared to raise their eyes. It escapes the tedious and troublesome task of collect- ing experimental facts, which is the province of the natural sciences in the strict sense of the word; the 28 ORIGIN AND SIGNIFICANCE OF sole form of its scientific method is deduction. Con- clusion is deduced from conclusion, and yet no one of common sense doubts but that these geometrical principles must find their practical application in the real world about us. Land surveying, as well as ar- chitecture, the construction of machinery no less than mathematical physics, are continually calculating re- lations of space of the most varied kind by geometrical principles ; they expect that the success of their con- structions and experiments shall agree with these calculations ; and no case is known in which this ex- pectation has been falsified, provided the calculations were made correctly and with sufficient data. Indeed, the fact that geometry exists, and is cap- able of all this, has always been used as a prominent example in the discussion on that question, which forms, as it were, the centre of all antitheses of philo- sophical systems, that there can be a cognition of principles destitute of any bases drawn from ex- perience. In the answer to Kant's celebrated ques- tion, 'How are synthetical principles a priori possible?' geometrical axioms are certainly those examples which appear to show most decisively that synthetical principles are a priori possible at all. The circumstance that such principles exist, and force themselves on our conviction, is regarded as a proof that space is an a priori mode of all external perception, GEOMETRICAL AXIOMS. 29 ft appears thereby to postulate, for this a priori form, not only the character of a purely formal scheme of itself quite unsubstantial, in which any given result experience would fit ; but also to include certain pe- culiarities of the scheme, which bring it about that only a certain content, ' and one which, as it were, is strictly defined, could occupy it and be apprehended by us.1 It is precisely this relation of geometry to the theory of cognition which emboldens me to speak to you on geometrical subjects in an assembly of those who for the most part have limited their mathematical studies to the ordinary instruction in schools. Fortunately, the amount of geometry taught in our gymnasia will enable you to follow, at any rate the tendency, of the principles I am about to discuss. I intend to give you an account of a series of recent and closely connected mathematical researches which are concerned with the geometrical axioms, their 1 In his book, On tlie Limits of Philosophy, Mr. W. Tobias main- tains that axioms of a kind which I formerly enunciated are a misunderstanding of Kant's opinion. But Kant specially adduces the axioms, that the straight line is the shortest (Kritik der reinen Vernunft, Introduction, v. 2nd ed. p. 16) ; that space has three di- mensions (Ibid, part i. sect. i. § 3, p. 41) ; that only one straight line is possible between two points (Ibid, part ii. sect. i. ' On the Axioms of Intuition '), as axioms which express a priori the conditions of intuition by the senses. It is not here the question, whether these axioms were originally given as intuition of space, or whether they are only the starting-points from which the understanding can develop such axioms a priori on which my critic insists. 30 ORIGIN AND SIGNIFICANCE OF relations to experience, with the question whether it is logically possible to replace them by others. Seeing that the researches in question are more immediately designed to furnish proofs for experts in a region which, more than almost any other, requires a higher power of abstraction, and that they are vir- tually inaccessible to the non-mathematician, I will endeavour to explain to such a one the question at issue. I need scarcely remark that my explanation will give no proof of the correctness of the new views. He who seeks this proof must take the trouble to study the original researches. Anyone who has entered the gates of the first ele- mentary axioms of geometry, that is, the mathematical doctrine of space, finds on his path that unbroken chain of conclusions of which I just spoke, by which the ever more varied and more complicated figures are brought within the domain of law. But even in their first elements certain principles are laid down, with respect to which geometry confesses that she cannot prove them, and can only assume that anyone who understands the essence of these principles will at once admit their correctness. These are the so- called axioms. For example, the proposition that if the shortest line drawn between two points is called a straight line, there can be only one such straight line. Again, it is GEOMETEICAL AXIOMS. 21 an axiom that through any three points in space, not lying in a straight line, a plane may be drawn, i.e. a surface which will wholly include every straight line joining any two of its points. Another axiom, about which there has been much discussion, affirms that through a point lying without a straight line only one straight line can be drawn parallel to the first ; two straight lines that lie in the same plane and never meet, however far they may be produced, being called parallel. There are also axioms that determine the number of dimensions of space and its surfaces, lines and points, showing how they are continuous ; as in the propositions, that a solid is bounded by a surface, a surface by a line and a line by a point, that the point is indivisible, that by the movement of a point a line is described, by that of a line a line or a surface, by that of a surface a surface or a solid, but by the movement of a solid a solid and nothing else is described. Now what is the origin of such propositions, un- questionably true yet incapable of proof in a science where everything else is reasoned conclusion? Are they inherited from the divine source of our reason as the idealistic philosophers think, or is it only that the ingenuity of mathematicians has hitherto not been penetrating enough to find the proof? Every new votary, coming with fresh zeal to geometry, naturally 32 OEIGIN AND SIGNIFICANCE OF strives to succeed where all before him have failed. And it is quite right that each should make the trial afresh ; for, as the question has hitherto stood, it is only by the fruitlessness of one's own efforts that one can be convinced of the impossibility of finding a proof. Meanwhile solitary inquirers are always from time to time appearing who become so deeply en- tangled in complicated trains of reasoning that they can no longer discover their mistakes and believe they have solved the problem. The axiom of parallels especially has called forth a great number of seeming demonstrations. The main difficulty in these inquiries is, and always has been, the readiness with which results of everyday experience become mixed up as apparent necessities of thought with the logical processes, so long as Euclid's method of constructive intuition is exclusively followed in geometry. It is in particular extremely difficult, on this method, to be quite sure that in the steps pre- scribed for the demonstration we have not involun- tarily and unconsciously drawn in some most general results of experience, which the power of executing certain parts of the operation has already taught us practically. In drawing any subsidiary line for the sake of his demonstration, the well-trained geometer always asks if it is possible to draw such a line. It is well known that problems of construction play an essen- GEOMETRICAL AXIOMS. 33 tial part in the system of geometry. At first sight, these appear to be practical operations, introduced for the training of learners; but in reality they estab- lish the existence of definite figures. They show that points, straight lines, or circles such as the problem re- quires to be constructed are possible under all con- ditions, or they determine any exceptions that there may be. The point on which the investigations turn, that we are about to consider, is essentially of this nature. The foundation of all proof by Euclid's method consists in establishing the congruence of lines, angles, plane figures, solids, &c. To make the congruence evident, the geometrical figures are sup- posed to be applied to one another, of course without changing their form and dimensions. That this is in fact possible we have all experienced from our earliest youth. But, if we proceed to build necessities of thought upon this assumption of the free trans- lation of fixed figures, with unchanged form, to every part of space, we must see whether the assumption does not involve some presupposition of which no logical proof is given. We shall see later on that it does indeed contain one of the most serious import. But if so, every proof by congruence rests upon a fact which is obtained from experience only. % I offer these remarks, at first only to show what difficulties attend the complete analysis of the pre- ii. p 34 ORIGIN AND SIGNIFICANCE OF suppositions we make, in employing the common con- structive method. We evade them when we apply, to the investigation of principles, the analytical method of modern algebraical geometry. The whole process of algebraical calculation is a purely logical operation ; it can yield no relation between the quantities sub- mitted to it that is not already contained in the equa- tions which give occasion for its being applied. The recent investigations in question have accordingly been conducted almost exclusively by means of the purely abstract methods of analytical geometry. However, after discovering by the abstract method what are the points in question, we shall best get a distinct view of them by taking a region of narrower limits than our own world of space. Let us, as we logically may, suppose reasoning beings of only two dimensions to live and move on the surface of some solid body. We will assume that they have not the power of perceiving anything outside this surface, but that upon it they have perceptions similar to ours. If such beings worked out a geometry, they would of course assign only two dimensions to their space. They would ascertain that a point in moving describes a, line, and that a line in moving describes a surface. But they could as little represent to themselves what further spatial construction would be generated by a surface moving out of itself, as we can represent what GEOMETRICAL AXIOMS. 35 would be generated by a solid moving out of the space we know. By the much-abused expression ' to re- present 'or ' to be able to think how something happens ' I understand — and I do not see how any- thing else can be understood by it without loss of all meaning — the power of imagining the whole series of sensible impressions that would be had in such a case. Now as no sensible impression is known relating to such an unheard-of event, as the movement to a fourth dimension would be to us, or as a movement to our third dimension would be to the inhabitants of a surface, such a ' representation ' is as impossible as the ' representation ' of colours would be to one born blind, if a description of them in general terms could be given to him. Our surface-beings would also be able to draw shortest lines in their superficial space. These would not necessarily be straight lines in our sense, but what are technically called geodetic lines of the surface on which they live ; lines such as are described by a tense thread laid along the surface, and which can slide upon it freely. I will henceforth speak of such lines as the straightest lines of any particular surface or given space, so as to bring out their analogy with the straight line in a plane. I hope by this expression to make the conception more easy for the apprehension D 2 36 OKIGIN AND SIGNIFICANCE OF of my non-mathematical hearers without giving rise to misconception. Now if beings of this kind lived on an infinite plane, their geometry would be exactly the same as our planimetry. They would affirm that only one straight line is possible between two points ; that through a third point lying without this line only one line can be drawn parallel to it ; that the ends of a straight line never meet though it is produced to infinity, and so on. Their space might be infinitely ex- tended, but even if there were limits to their move- ment and perception, they would be able to represent to themselves a continuation beyond these limits ; and thus their space would appear to them infinitely ex- tended, just as ours does to us, although our bodies cannot leave the earth, and our sight only reaches as far as the visible fixed stars. But intelligent beings of the kind supposed might also live on the surface of a sphere. Their shortest or straightest line between two points would then be an arc of the great circle passing through them. Every great circle, passing through two points, is by these divided into two parts ; and if they are unequal, the shorter is certainly the shortest line on the sphere be- tween the two points, but also the other or larger arc of the same great circle is a geodetic or straightest line, i.e. every small or part of it is the shortest line GEOMETRICAL AXIOMS. 37 between its ends. Thus the notion of the geodetic or straightest line is not quite identical with that of the shortest line. If the two given points are the ends of a diameter of the sphere, every plane passing through this diameter cuts semicircles, on the surface of the sphere, all of which are shortest lines between the ends ; in which case there is an equal number of equal shortest lines between the given points. Ac- cordingly, the axiom of there being only one shortest line between two points would not hold without a certain exception for the dwellers on a sphere. Of parallel lines the sphere -dwellers would know nothing. They would maintain that any two straightest lines, sufficiently produced, must finally cut not in one only but in two points. The sum of the angles of a triangle would be always greater than two right angles, increasing as the surface of the triangle grew greater. They could thus have no conception of geometrical similarity between greater and smaller figures of the same kind, for with them a greater triangle must have different angles from a smaller one. Their space would be unlimited, but would be found to be finite or at least represented as such. It is clear, then, that such beings must set up a very different system of geometrical axioms from that of the inhabitants of a plane, or from ours with our space of three dimensions, though the logical power* 38 ORIGIN AND SIGNIFICANCE OF of all were the same; nor are more examples neces- sary to show that geometrical axioms must vary ac- cording to the kind of space inhabited by beings whose powers of reason are quite in conformity with ours. But let us proceed still farther. Let us think of reasoning beings existing on the surface of an egg-shaped body. Shortest lines could be drawn between three points of such a surface and a triangle constructed. But if the attempt were made to construct congruent triangles at different parts of the surface, it would be found that two triangles, with three pairs of equal sides, would not have their angles equal. The sum of the angles of a triangle drawn at the sharper pole of the body would depart farther from two right angles than if the triangle were drawn at the blunter pole or at the equator. Hence it appears that not even such a simple figure as a triangle can be moved on such a surface without change of form. It would also be found that if circles of equal radii were constructed at different parts of such a surface (the length of the radii being always measured by shortest lines along the surface) the periphery would be greater at the blunter than at the sharper end. We see accordingly that, if a surface admits of the figures lying on it being freely moved without change of any of their lines and angles as measured along it, the property is a special one and does not belong to GEOMETRICAL AXIOMS. 39 every kind of surface. The condition under which a surface possesses this important property was pointed out by Gauss in his celebrated treatise on the cur- vature of surfaces.1 The * measure of curvature,' as he called it, i.e. the reciprocal of the product of the greatest and least radii of curvature, must be every- where equal over the whole extent of the surface. Gauss showed at the same time that this measure of curvature is not changed if the surface is bent with- out distension or contraction of any part of it. Thus we can roll up a flat sheet of paper into the form of a cylinder, or of a cone, without any change in the dimensions of the figures taken along the surface of the sheet. Or the hemispherical fundus of a bladder may be rolled into a spindle-shape without altering the dimensions on the surface. Geometry on a plane will therefore be the same as on a cylindrical surface ; only in the latter case we must imagine that any number of layers of this surface, like the layers of a rolled sheet of paper, lie one upon another, and that after each entire revolution round the cylinder a new layer is reached different from the previous ones. These observations are necessary to give the reader a notion of a kind of surface the geometry of which is on the whole similar to that of the plane, but in which 1 Gauss, Werke, Bd. IV. p. 215, first published in Commcntationes Sec, Ileg. Scientt. Gottengensis recetit'ivrcs, vol. vi., 1828. 40 OftlGIN AND SIGNIFICANCE OF the axiom of parallels does not hold good. This is a kind of curved surface which is, as it were, geometri- cally the counterpart of a sphere, and which has there- fore been called the pseudospherical surface by the distinguished Italian mathematician E. Beltrami, who has investigated its properties.1 It is a saddle-shaped surface of which only limited pieces or strips can be connectedly represented in our space, but which may yet be thought of as infinitely continued in all direc- tions, since each piece lying at the limit of the part constructed can be conceived as drawn back to the middle of it and then continued. The piece displaced must in the process change its flexure but not its dimensions, just as happens with a sheet of paper moved about a cone formed out of a plane rolled up. Such a sheet fits the conical surface in every part, but must be more bent near the vertex and cannot be so moved over the vertex as to be at the same time adapted to the existing cone and to its imaginary continuation beyond. Like the plane and the sphere, pseudospherical sur- faces have their measure of curvature constant, so that every piece of them can be exactly applied to every 1 Saggio di Interpretazione della Geometria Non-Euclidea, N apoli, 1868. — Teoria Jondamentale degli Spazii di Curvatura costante, An* nali di Matematica, Ser. II. Tom. II. pp. 232-55. Both have been translated into French by J. Houel, AnnaLs Scienti/iqua de Xorniale, Tom V., 1860. GECttlETEICAL AXIOMS. 41 other piece, and therefore all figures constructed at one place on the surface can be transferred to any other place with perfect congruity of form, and perfect equality of all dimensions lying in the surface itself. The measure of curvature as laid down by Gauss, which is positive for the sphere and zero for the plane, would have a constant negative value for pseudo- spherical surfaces, because the two principal curvatures of a saddle-shaped surface have their concavity turned opposite ways. A strip of a pseudospherical surface may, for exam- ple, be represented by the inner surface (turned towards the axis) of a solid anchor-ring. If the plane figure aabb (Fig. 1) is made to revolve on its axis of symme- try AB, the two arcs ab will describe a pseudospherical concave-convex surface like that of the ring. Above and below, towards aa and 66, the surface will turn outwards with ever-increasing flexure, till it becomes perpendicular to the axis, and ends at the edge with one curvature infinite. Or, again, half of a pseudospheri- cal surface may be rolled up into the shape of a cham- pagne-glass (Fig. 2), with tapering stem infinitely prolonged. But the surface is always necessarily bounded by a sharp edge beyond which it cannot be directly continued. Only by supposing each single piece of the edge cut loose and drawn along the surface of the ring or glass, can it be brought to places of 42 ORIGIN AND SIGNIFICANCE OF different flexure, at which farther continuation of the piece is possible. In this way too the straight est lines of the pseudo- spherical surface may be infinitely produced. They do not, like those on a sphere, return upon themselves, but, as on a plane, only one shortest line is possible between the two given points. The axiom of parallels does not, however, hold good. If a straightest line is Fia. 1. given on the surface and a point without it, a whole pencil of straightest lines may pass through the point, no one of which, though infinitely produced, cuts the first line; the pencil itself being limited by two straightest lines, one of which intersects one of the ends of the given line at an infinite distance, the other the other end. Such a system of geometry, which excluded the axiom of parallels, was devised on Euclid's synthetic method, as far back as the year 1829, by N. J. Lo- GEOMETEICAL AXIOMS. 43 batchewsky, professor of mathematics at Kasan,1 and it was proved that this system could be carried out as consistently as Euclid's. It agrees exactly with the geometry of the pseudospherical surfaces worked out recently by Beltrami. Thus we see that in the geometry of two dimen- sions a surface is marked out as a plane, or a sphere, or a pseudospherical surface, by the assumption that any figure may be moved about in all directions without change of dimensions. The axiom, that there is only one shortest line between any two points, distinguishes the plane and the pseudospherical surface from the sphere, and the axiom of parallels marks off the plane from the pseudosphere. These three axioms are in fact necessary and sufficient, to define as a plane the surface to which Euclid's planimetry has reference, as distinguished from all other modes of space in two dimensions. The difference between plane and spherical geome- try has been long evident, but the meaning of the axiom of parallels could not be understood till Gauss had developed the notion of surfaces flexible without dilatation, and consequently that of the possibly in- finite continuation of pseudospherical surfaces. In- habiting, as we do, a space of three dimensions and endowed with organs of sense for their perception, we 1 Principien der Geometric, Kasan, 1829-30. 44 ORIGIN AND SIGNIFICANCE OF can represent to ourselves the various cases in which beings on a surface might have to develop their per- ception of space ; for we have only to limit our own perceptions to a narrower field. It is easy to think away perceptions that we have ; but it is very difficult to imagine perceptions to which there is nothing ana- logous in our experience. When, therefore, we pass to space of three dimensions, we are stopped in our power of representation, by the structure of our organs and the experiences got through them which correspond only to the space in which we live. There is however another way of treating geometry scientifically. All known space-relations are measur- able, that is, they may be brought to determination of magnitudes (lines, angles, surfaces, volumes). Problems in geometry can therefore be solved, by finding methods of calculation for arriving at unknown magnitudes from known ones. This is done in analytical geometry, where all forms of space are treated only as quantities and determined by means of other quantities. Even the axioms themselves make reference to magnitudes. The straight line is defined as the shortest between two points, which is a determination of quantity. The axiom of parallels declares that if two straight lines in a plane do not intersect (are parallel), the alternate angles, or the corresponding angles, made by a third line intersecting them, are equal; or it may be laid GEOMETRICAL AXTOm 45 down instead that the sum of the angles of any triangle is equal to two right angles. These, also, are determinations of quantity. Now we may start with this view of space, accord- ing to which the position of a point may be deter- mined by measurements in relation to any given figure (system of co-ordinates), taken as fixed, and then inquire what are the special characteristics of our space as manifested in the measurements that have to be made, and how it differs from other extended quantities of like variety. This path was first entered by one too early lost to science, B. Eiemann of Grott- ingen.1 It has the peculiar advantage that all its operations consist in pure calculation of quantities, which quite obviates the danger of habitual percep- tions being taken for necessities of thought. The number of measurements necessary to give the position of a point, is equal to the number of dimensions of the space in question. In a line the distance from one fixed point is sufficient, that is to say, one quantity ; in a surface the distances from two fixed points must be given ; in space, the distances from three ; or we require, as on the earth, longitude, latitude, and height above the sea, or, as is usual in analytical geometry, the distances from three co-ordinate planes. Eiemann 1 Ueber die Hypothesen welche der Geometrie zu Grunde liegen, Habilitationsschrift vom 10 Juni 1854. (AbJuindl. der koidgl, Gesellsch. zu Gottinqen, Bd. XIII.) 4f» OEIGIX AND SIGNIFICANCE 051 calls a system of differences in which one thing can be determined by n measurements an 'Tifold extended aggregate ' or an * aggregate of n dimensions/ Thus the space in which we live is a threefold, a surface is a twofold, and a line is a simple extended aggregate of points. Time also is an aggregate of one dimension. The system of colours is an aggregate of three dimen- sions, inasmuch as each colour, according to the inves- tigations of Thomas Young and of Clerk Maxwell,1 may be represented as a mixture of three primary colours, taken in definite quantities. The particular mixtures can be actually made with the colour-top. In the same way we may consider the system of simple tones2 as an aggregate of two dimensions, if we distinguish only pitch and intensity, and leave out of account differences of timbre. This generalisation of the idea is well suited to bring out the distinction be- tween space of three dimensions and other aggregates. We can, as we know from daily experience, compare the vertical distance of two points with the horizontal distance of two others, because we can apply a measure first to the one pair and then to the other. But we cannot compare the difference between two tones of equal pitch and different intensity, with that between two tones of equal intensity and different pitch. Eiemann showed, by considerations of this kind, that the essential foun- 1 Jlelmlioltz's Popular Lectures, Series I. p. 243. « Ibid, p. 86. GEOMETRICAL AXIOMS. 47 dation of any system of geometry, is the expression that it gives for the distance between two points lying in any direction towards one another, beginning with the infinitesimal interval. He took from analytical geometry the most general form for this expression, that, namely, which leaves altogether open the kind of measurements by which the position of any point is given.1 Then he showed that the kind of free mobi- lity without change of form which belongs to bodies in our space can only exist when certain quantities yielded by the calculation 2 — quantities that coincide with Gauss's measure of surface-curvature when they are expressed for surfaces — have everywhere an equal value. For this reason Eiemann calls these quantities, when they have the same value in all directions for a particular spot, the measure of curvature of the space at this spot. To prevent misunderstanding,3 I will once more observe that this so-called measure of space-curvature is a quantity obtained by purely ana- lytical calculation, and that its introduction involves no suggestion of relations that would have a meaning only for sense-perception. The name is merely taken, 1 For the square of the distance of two infinitely near points the expression is a homogeneous quadric function of the differentials of their co-ordinates. 2 They are algebraical expressions compounded from the co- efficients of the various terms in the expression for the square of the distance of two contiguous points and from their differential quotients. * As occurs, for instance, in the above-mentioned work of Tobias, pp. 70, etc. 48 ORIGIN AND SIGNIFICANCE OP as a short expression for a complex relation, from the one case in which the quantity designated admits, of sensible representation. Now whenever the value of this measure of curva- ture in any space is everywhere zero, that space every- where conforms to the axioms of Euclid ; and it may be called a flat (homaloid) space in contradistinction to other spaces, analytically constructible, that may be c ailed curved, because their measure of curvature has a value other than zero. Analytical geometry may be as completely and consistently worked out for such spaces as ordinary geometry can for our actually existing homaloid space. If the measure of curvature is positive we have spherical space, in which straightest lines return upon themselves and there are no parallels. Such a space would, like the surface of a sphere, be unlimited but not infinitely great. A constant negative measure of curvature on the other hand gives pseudo-spherical space, in which straightest lines run out to infinity, and a pencil of straightest lines may be drawn, in any flattest surface, through any point which does not inter- sect another given straightest line in that surface. Beltrami * has rendered these last relations imagin- able by showing that the points, lines, and surfaces of a pseudospherical space of three dimensions, can be so 1 Teoria fondamentale, $ GEOMETRICAL AXIOMS. 49 portrayed in the interior of a sphere in Euclid's homa- loid space, that every straightest line or flattest surface of the pseudospherical space is represented by a straight line or a plane, respectively, in the sphere. The surface itself of the sphere corresponds to the infinitely distant points of the pseudospherical space ; and the different parts of this space, as represented in the sphere, become smaller, the nearer they lie to the spherical surface, diminishing more rapidly in the direc- tion of the radii than in that perpendicular to them. Straight lines in the sphere, which only intersect beyond its surface, correspond to straightest lines of the pseudospherical space which never intersect. Thus it appeared that space, considered as a region of measurable quantities, does not at all correspond with the most general conception of an aggregate of three dimensions, but involves also special conditions, depending on the perfectly free mobility of solid bodies without change of form to all parts of it and with all possible changes of direction ; and, further, on the special value of the measure of curvature which for our actual space equals, or at least is not distin- guishable from, zero. This latter definition is given in the axioms of straight lines and parallels. Whilst Eiemann entered upon this new field from the side of the most general and fundamental questions of analytical geometry, I myself arrived at similar II. I 50 ORIGIN AND SIGNIFICANCE OS conclusions,1 partly from seeking to represent in space the system of colours, involving the comparison of one threefold extended aggregate with another, and partly from inquiries on the origin of our ocular measure for distances in the field of vision. Kiemann starts by assuming the above-mentioned algebraical expression which represents in the most general form the distance between two infinitely near points, and deduces there- from, the conditions of mobility of rigid figures. I, on the other hand, starting from the observed fact that the movement of rigid figures is possible in our space, with the degree of freedom that we know, deduce the necessity of the algebraic expression taken by Biemann as an axiom. The assumptions that I had to make as the basis of the calculation were the following. First, to make algebraical treatment at all possible, it must be assumed that the position of any point A can be determined, in relation to certain given figures taken as fixed bases, by measurement of some kind of magnitudes, as lines, angles between lines, angles between surfaces, and so forth. The measurements necessary for determining the position of A are known as its co-ordinates. In general, the number of co- ordinates necessary for the complete determination of the position of a point, marks the number of the dimen- 1 Ueber die Thatsachen die der Geometric ziirn Grande liegen {Nachrickten, yonder k'dnigl. Ges. d. Wiss.zu Gottingen, Juni 3, 1868). GEOMETRICAL AXIOMS. 51 sions of the space in question. It is further assumed that with the movement of the point A, the magnitudes used as co-ordinates vary continuously. Secondly, the definition of a solid body, or rigid system of points, must be made in such a way as to admit of magnitudes being compared by congruence. As we must not, at this stage, assume any special methods for the measurement of magnitudes, our defi- nition can, in the first instance, run only as follows » Between the co-ordinates of any two points belonging to a solid body, there must be an equation which, how- ever the body is moved, expresses a constant spatial relation (proving at last to be the distance) between the two points, and which is the same for congruent pairs of points, that is to say, such pairs as can be made successively to coincide in space with the same fixed pair of points. However indeterminate in appearance, this defini- tion involves most important consequences, because with increase in the number of points, the number of equations increases much more quickly than the number of co-ordinates which they determine. Five points, A, B, C, D, E, give ten different pairs of points AB, AC, AD, AE, EC, BD, BE, CD, CE, DE, 52 ORIGIN AND SIGNIFICANCE 0£ and therefore ten equations, involving in space of three dimensions fifteen variable co-ordinates. But of these fifteen, six must remain arbitrary, if the system of five points is to admit of free movement and rotation, and thus the ten equations can determine only nine co-ordi- nates as functions of the six variables. With six points we obtain fifteen equations for twelve quantities, with seven points twenty-one equations for fifteen, and so on. Now from n independent equations we can determine n contained quantities, and if we have more than n equations, the superfluous ones must be deducible from the first n. Hence it follows that the equations which subsist between the co-ordinates of each pair of points of a solid body must have a special character, seeing that, when in space of three dimen- sions they are satisfied for nine pairs of points as formed out of any five points, the equation for the tenth pair follows by logical consequence. Thus our assump- tion for the definition of solidity, becomes quite suffi- cient to determine the kind of equations holding be- tween the co-ordinates of two points rigidly connected. Thirdly, the calculation must further be based on the fact of a peculiar circumstance in the movement of solid bodies, a fact so familiar to us that but for this inquiry it might never have been thought of as some- thing that need not be. When in our space of three dimensions two points of a solid body are kept fixed, GEOMETRICAL AXIOMS. 53 its movements are limited to rotations round the straight line connecting them. If we turn it com- pletely round once, it again occupies exactly the po- sition it had at first. This fact, that rotation in one direction always brings a solid body back into its ori- ginal position, needs special mention. A system of geometry is possible without it. This is most easily seen in the geometry of a plane. Suppose that with every rotation of a plane figure its linear dimensions in- creased in proportion to the angle of rotation, the figure after one whole rotation through 360 degrees would no longer coincide with itself as it was originally. But any second figure that was congruent with the first in its original position might be made to coincide with it in its second position by being also turned through 360 degrees. A consistent system of geometry would be possible upon this supposition, which does not come under Eiemann's formula. On the other hand I have shown that the three assumptions taken together form a sufficient basis for the starting-point of Eiemann's investigation, and thence for all his further results relating to the dis- tinction of different spaces according to their measure of curvature. It still remained to be seen whether the laws of motion, as dependent on moving forces, could also be consistently transferred to spherical or pseudospherical 54 ORIGIN AND SIGNIFICANCE OF space. This investigation has been carried out by Professor Lipschitz of Bonn.1 It is found that the comprehensive expression for all the laws of dynamics, Hamilton's principle, may be directly transferred to spaces of which the measure of curvature is other than zero. Accordingly, in this respect also, the disparate systems of geometry lead to no contradiction. We have now to seek an explanation of the special characteristics of our own flat space, since it appears that they are not implied in the general notion of an extended quantity of three dimensions and of the free mobility of bounded figures therein. Necessities of thought, such as are involved in the conception of such a variety, and its measurability, or from the most general of all ideas of a solid figure contained in it, and of its free mobility, they undoubtedly are not. Let us then examine the opposite assumption as to their origin being empirical, and see if they can be inferred from facts of experience and so established, or if, when tested by experience, they are perhaps to be rejected. If they are of empirical origin, we must be able to represent to ourselves connected series of facts, indicating a different value for the measure of curva- ture from that of Euclid's flat space. But if we can • 'Untersuclmngen iiber die ganzen homogenen Functionen von n Differentialen' (Borchardt's Journal filr MatJiematik, Bd. Ixx. 3, 71 ; Ixxiii. 3, 1) ; « Untersuchung eines Problems der Variationsrechnung' ( Ibid. Bd. Ixxiv.). GEOMETEICAL AXIOMS. 55 imagine such spaces of other sorts, it cannot be main- tained that the axioms of geometry are necessary con- sequences of an a priori transcendental form of intui- tion, as Kant thought. The distinction between spherical, pseudospherical, and Euclid's geometry depends, as was above observed, on the value of a certain constant called, by Eiemann, the measure of curvature of the space in question. The value must be zero for Euclid's axioms to hold good. If it were not zero, the sum of the angles of a large triangle would differ from that of the angles of a small one, being larger in spherical, smaller in pseu- dospherical, space. Again, the geometrical similarity of large and small solids or figures is possible only in Euclid's space. All systems of practical mensuration that have been used for the angles of large rectilinear triangles, and especially all systems of astronomical measurement which make the parallax of the im- measurably distant fixed stars equal to zero (in pseudo- spherical space the parallax even of infinitely distant points would be positive), confirm empirically the axiom of parallels, and show the measure of curvature of our space thus far to be indistinguishable from zero It remains, however, a question, as Biemann observed, whether the result might not be different if we could use other than our limited base-lines, the greatest oi which is the major axis of the earth's orbit. 56 ORIGIN AND SIGNIFICANCE OF Meanwhile, we must not forget that all geometrical measurements rest ultimately upon the principle of congruence. We measure the distance between points by applying to them the compass, rule, or chain. We measure angles by bringing the divided circle or theo- dolite to the vertex of the angle. We also determine straight lines by the path of rays of light which in our experience is rectilinear ; but that light travels in shortest lines as long as it continues in a medium of constant refraction would be equally true in space of a different measure of curvature. Thus all our geo- metrical measurements depend on our instruments being really, as we consider them, invariable in form, or at least on their undergoing no other than the small changes we know of, as arising from variation of tem- perature, or from gravity acting differently at different places. In measuring, we only employ the best and surest means we know of to determine, what we otherwise are in the habit of making out by sight and touch or by pacing. Here our own body with its organs is the instrument we carry about in space. Now it is the hand, now the leg, that serves for a compass, or the eye turning in all directions is our theodolite for measur- ing arcs and angles in the visual field. Every comparative estimate of magnitudes or mea- surement of their spatial relations proceeds therefore GEOMETRICAL AXIOMS. 57 upon a supposition as to the behaviour of certain phy- sical things, either the human body or other instru- ments employed. The supposition may be in the highest degree probable and in closest harmony with all other physical relations known to us, but yet it passes beyond the scope of pure space-intuition. It is in fact possible to imagine conditions for bodies apparently solid such that the measurements in Euclid's space become what they would be in spherical or pseudospherical space. Let me first remind the reader that if all the linear dimensions of other bodies, and our own, at the same time were diminished or in- creased in like proportion, as for instance to half or double their size, we should with our means of space- perception be utterly unaware of the change. This would also be the case if the distension or contraction were different in different directions, provided that our own body changed in the same manner, and further that a body in rotating assumed at every moment, without suffering or exerting mechanical resistance, the amount of dilatation in its different dimensions corresponding to its position at the time. Think of the image of the world in a convex mirror. The common silvered globes set up in gardens give the essential features, only distorted by some optical ir- regularities. A well-made convex mirror of moderate aperture represents the objects in front of it as ap- 58 OKiaiN AND SIGNIFICANCE 0? parently solid and in fixed positions behind its surface. But the images of the distant horizon and of the sun in the sky lie behind the mirror at a limited distance, equal to its focal length. Between these and the sur- face of the mirror are found the images of all the other objects before it, but the images are diminished and flattened in proportion to the distance of their objects from the mirror. The flattening, or decrease in the third dimension, is relatively greater than the decrease of the surface-dimensions. Yet every straight line or every plane in the outer world is represented by a straight. line or a plane in the image. The image of a man measuring with a rule a straight line from the mirror would contract more and more the farther he went, but with his shrunken rule the man in the image would count out exactly the same number of centimetres as the real man. And, in general, all geometrical measurements of lines or angles made with regularly varying images of real instruments would yield exactly the same results as in the outer world, all congruent bodies would coincide on being applied to one another in the mirror as in the outer world, all lines of sight in the outer world would be represented by straight lines of sight in the mirror. In short I do not see how men in the mirror are to discover that their bodies are not rigid solids and their experiences good examples of the correctness of Euclid's axioms. But if they could look out upon our GEOMETKICAL AXIOMS. 59 world as we can look into theirs, without overstepping the boundary, they must declare it to be a picture in a spherical mirror, and would speak of us just as we speak of them ; and if two inhabitants of the different worlds could communicate with one another, neither, so far as I can see, would be able to convince the other that he had the true, the other the distorted, relations. Indeed I cannot see that such a question would have any meaning at all, so long as mechanical considerations are not mixed up with it. Now Beltrami's representation of pseudospherical space in a sphere of Euclid's space, is quite similar, ex- cept that the background is not a plane as in the convex mirror, but the surface of a sphere, and that the proportion in which the images as they approach the spherical surface contract, has a different mathe- matical expression.1 If we imagine then, conversely, that in the sphere, for the interior of which Euclid's axioms hold good, moving bodies contract as they depart from the centre like the images in a convex mirror, and in such a way that their representatives in pseudospherical space retain their dimensions unchanged, — observers whose bodies were regularly subjected to the same change would obtain the same results from the geometrical measurements they could make as if they lived in pseudospherical space. 1 Compare the Appendix at the end of this Lecture-. 60 ORIGIN AND SIGNIFICANCE OF We can even go a step further, and infer how the objects in a pseudospherical world, were it possible to enter one, would appear to an observer, whose eye- measure and experiences of space had been gained like ours in Euclid's space. Such an observer would con- tinue to look upon rays of light or the lines of vision as straight lines, such as are met with in flat space, and as they really are in the spherical representation of pseudospherical space. The visual image of the objects in pseudospherical space would thus make the same impression upon him as if he were at the centre of Beltrami's sphere. He would think he saw the most remote objects round about him at a finite distance,1 let us suppose a hundred feet off. But as he approached these distant objects, they would dilate before him, though more in the third dimension than superficially, while behind him they would contract. He would know that his eye judged wrongly. If he saw two straight lines which in his estimate ran parallel for the hundred feet to his world's end, he would find on following them that the farther he advanced the more they diverged, because of the dilatation of all the objects to which he approached. On the other hand, behind him, their distance would seem to diminish, so that as he advanced they would 1 The reciprocal of the square of this distance, expressed in negative quantity, would be the measure of curvature of the pseudo- spherical space. GEOMETRICAL AXIOMS. 61 appear always to diverge more and more. But two straight lines which from his first position seemed to converge to one and the same point of the background a hundred feet distant, would continue to do this however far he went, and he would never reach their point of intersection. Now we can obtain exactly similar images of our real world, if we look through a large convex lens of corresponding negative focal length, or even through a pair of convex spectacles if ground somewhat prisma- tically to resemble pieces of one continuous larger lens. With these, like the convex mirror, we see remote ob- jects as if near to us, the most remote appearing no farther distant than the focus of the lens. . In going about with this lens before the eyes, we find that the objects we approach dilate exactly in the manner I have described for pseudospherical space. Now any one using a lens, were it even so strong as to have a focal length of only sixty inches, to say nothing of a hun- dred feet, would perhaps observe for the first moment that he saw objects brought nearer. But after going about a little the illusion would vanish, and in spite of the false images he would judge of the distances rightly. We have every reason to suppose that what happens in a few hours to any one beginning to wear spectacles would soon enough be experienced in pseu- dospherical space. In short, pseudospherical space 62 OEIGIN AND SIGNIFICANCE OF would not seem to us very strange, comparatively speaking; we should only at first be subject to illu- sions in measuring by eye the size and distance of the more remote objects. There would be illusions of an opposite description, if, with eyes practised to measure in Euclid's space, we entered a spherical space of three dimensions. We should suppose the more distant objects to be more remote and larger than they are, and should find on approaching them that we reached them more quickly than we expected from their appearance. But we should also see before us objects that we can fixate only with diverging lines of sight, namely, all those at a greater distance from us than the quadrant of a great circle. Such an aspect of things would hardly strike us as very extraordinary, for we can have it even as things are if we place before the eye a slightly pris- matic glass with the thicker side towards the nose : the eyes must then become divergent to take in distant objects. This excites a certain feeling of unwonted strain in the eyes, but does not perceptibly change the appearance of the objects thus seen. The strangest sight, however, in the spherical world would be the back of our own head, in which all visual lines not stopped by other objects would meet again, and which must fill the extreme background of the whole per- spective picture. GEOMETRICAL AXIOMS. f>3 At the same time it must be noted that as a small elastic flat disk, say of india-rubber, can only be fitted to a slightly curved spherical surface with relative con- traction of its border and distension of its centre, so our bodies, developed in Euclid's flat space, could not pass into curved space without undergoing similar distensions and contractions of their parts, their co- herence being of course maintained only in as far as their elasticity permitted their bending without break- ing. The kind of distension must be the same as in passing from a small body imagined at the centre of Beltrami's sphere to its pseudospherical or spherical representation. For such passage to appear possible, it will always have to be assumed that the body is sufficiently elastic and small in comparison with the real or imaginary radius of curvature of the curved space into which it is to pass. These remarks will suffice to show the way in which we can infer from the known laws of our sen- sible perceptions the series of sensible impressions which a spherical or pseudospherical world would give us, if it existed. In doing so, we nowhere meet with inconsistency or impossibility any more than in the calculation of its metrical proportions. "We can re- present to ourselves the look of a pseudospherical world in all directions just as we can develop the con* ception of it. Therefore it cannot be allowed that the 64 OBiaiN AND SIGNIFICANCE 0? axioms of our geometry depend on the native form of our perceptive faculty, or are in any way connected with it. It is different with the three dimensions of space. As all our means of sense-perception extend only to space of three dimensions, and a fourth is not merely a modification of what we have, but something per- fectly new, we find ourselves by reason of our bodily organisation quite unable to represent a fourth di- mension. In conclusion, I would again urge that the axioms of geometry are not propositions pertaining only to the pure doctrine of space. As I said before, they are concerned with quantity. We can speak of quantities only when we know of some way by which we can com- pare, divide, and measure them. All space-measure- ments, and therefore in general all ideas of quantities applied to space, assume the possibility of figures mov- ing without change of form or size. It is true we are accustomed in geometry to call such figures purely geometrical solids, surfaces, angles, and lines, because we abstract from all the other distinctions, physical and chemical, of natural bodies ; but yet one physical quality, rigidity, is retained. Now we have no other mark of rigidity of bodies or figures but congruence, whenever they are applied to one another at any time or place, and after any revolution. We cannot, hovv- GEOMETKICAL AXIOMS. 65 ever, decide by pure geometry, and without mechanical considerations, whether the coinciding bodies may not both have varied in the same sense. If it were useful for any purpose, we might with perfect consistency look upon the space in which we live as the apparent space behind a convex mirror with its shortened and contracted background ; or we might consider a bounded sphere of our space, beyond the limits 'of which we perceive nothing further, as infinite pseudospherical space. Only then we should have to ascribe to the bodies which appear to us to be solid, and to our own body at the same time, corresponding disten- sions and contractions, and we should have to change our system of mechanical principles entirely ; for even the proposition that every point in motion, if acted upon by no force, continues to move with unchanged velo- city in a straight line, is not adapted to the image of the world in the convex-mirror. The path would in- deed be straight, but the velocity would depend upon the place. Thus the axioms of geometry are not concerned with space-relations only but also at the same time with the mechanical deportment of solidest bodies in motion. The notion of rigid geometrical figure might indeed be conceived as transcendental in Kant's sense, namely, as formed independently of actual experience, which need not exactly correspond therewith, any more II. F 60 ORIGIN AND SIGNIFICANCE OP than natural bodies do ever in fact correspond exactly to the abstract notion we have obtained of them by in- duction. Taking the notion of rigidity thus as a mere ideal, a strict Kantian might certainly look upon the geometrical axioms as propositions given, a priori, by transcendental intuition, which no experience could either confirm or refute, because it must first be decided by them whether any natural bodies can be considered as rigid. But then we should have to maintain that the axioms of geometry are not synthetic propositions, as Kant held them ; they would merely define what quali- ties and deportment a body must have to be recognised as rigid. But if to the geometrical axioms we add proposi- tions relating to the mechanical properties of natural bodies, were it only the axiom of inertia, or the single proposition, that the mechanical and physical proper- ties of bodies and their mutual reactions are, other circumstances remaining the same, independent of place, such a system of propositions has a real import which can be confirmed or refuted by experience, but just for the same reason can also be gained by expe- rience. The mechanical axiom, just cited, is in fact of the utmost importance for the whole system of our mechanical and physical conceptions. That rigid solids, as we call them, which are really nothing else than elas- tic solids of great resistance, retain the same form in GEOMETRJCAL AXIOMS. 67 every part of space if no external force affects them, is a single case falling under the general principle. In conclusion, I do not, of course, maintain that man- kind first arrived at space-intuitions, in agreement with the axioms of Euclid, by any carefully executed systems of exact measurement. It was rather a succession of everyday experiences, especially the perception of the geometrical similarity of great and small bodies, only possible in flat space, that led to the rejection, as im- possible, of every geometrical representation at variance with this fact. For this no knowledge of the neces- sary logical connection between the observed fact of geometrical similarity and the axioms was needed ; but only an intuitive apprehension of the typical relations between lines, planes, angles, &c., obtained by nume- rous and attentive observations — an intuition of the kind the artist possesses of the objects he is to repre- sent, and by means of which he decides with certainty and accuracy whether a new combination, which he tries, will correspond or not with their nature. It is true that we have no word but intuition to mark this ; but it is knowledge empirically gained by the aggregation and reinforcement of similar recurrent impressions in memory, and not a transcendental form given before experience. That other such empirical intuitions of fixed typical relations, when not clearly comprehended, have frequently enough been taken by metaphysicians 72 68 ORIGIN AND SIGNIFICANCE OF for a priori principles, is a point on which I need not insist. To sum up, the final outcome of the whole inquiry may be thus expressed : — (1.) The axioms of geometry, taken by themselves out of all connection with mechanical propositions, re- present no relations of real things. When thus iso- lated, if we regard them with Kant as forms of intuition transcendentally given, they constitute a form into which any empirical content whatever will fit, and which therefore does not in any way limit or determine beforehand the nature of the content. This is true, however, not only of Euclid's axioms, but also of the axioms of spherical and pseudospherical geo- metry. (2.) As soon as certain principles of mechanics are conjoined with the axioms of geometry, we obtain a system of propositions which has real import, and which can be verified or overturned by empirical obser- vations, just as it can be inferred from experience. If such a system were to be taken as a transcendental form of intuition and thought, there must be assumed fc pre-established harmony between form and reality. GEOMETRICAL AXIOMS. 60 APPENDIX. THE elements of the geometry of spherical space are most easily obtained by putting for space of four dimensions the equation for the sphere and for the distance ds between the points (x, y, z, t) and [(x+dx) (y+dy) (z+dz) (t + dt)] the value ...... (2.) It is easily found by means of the methods used for three dimensions that the shortest lines are given by equations of the form ,3 . in which a, b, c,f, as well as a, f3, y, , are constants. The length of the shortest arc, s, between the points (a;, y, z, t), and (£, 17, £, r) follows, as in the sphere, from the equation cos J*±£!*l± ......... (4.) One of the co-ordinates may be eliminated from the values given in 2 to 4, by means of equation 1, and the expressions then apply to space of three dimensions. If we take the distances from the points £=,,=£=0 70 ORIGIN AND SIGNIFICANCE OF GEOMETRICAL AXIOMS from which equation 1 gives r=7?, then, sin in which J RTT. Tha extension in the direction of r is then APPENDIX. 71 In order to obtain corresponding expressions for pseudo- Bpherical space, let R and t be imaginary; that is, ^=Ii, and t=tl Equation 6 gives then from which, eliminating the imaginary form, we get ,0=l f log. nat. |±5 Here SQ has real values only as long as r=R; for r=1J, the distance SQ in pseudospherical space is infinite. The image in plane space is, on the contrary, contained in the sphere of radius JR, and every point of this sphere forms only one point of the infinite pseudospherical space. The extension in the direction of r is dsQ= W dc $2-i» For linear elements, on the contrary, whose direction is at right angles to r, and for which t is unchanged, we have in both cases ON THE EELATION OP OPTICS TO PAINTING. Being the substance of a aeries of Lectures delivered in Cologne, Berlin, and Bonn. I FEAR that the announcement of my intention to ad- dress you on the subject of plastic art may have created no little surprise among some of my hearers. For I cannot doubt that many of you have had more fre- quent opportunities of viewing works of art, and have more thoroughly studied its historical aspects, than I can lay claim to have done ; or indeed have had personal experience in the actual practice of art, in which I am entirely wanting. I have arrived at my artistic studies by a path which is but little trod, that is, by the phy- siology of the senses ; and in reference to those who have a long acquaintance with, and who are quite at home in the beautiful fields of art, I may compare 74 ON THE KELATION OF OPTICS TO PAINTING. myself to a traveller who has entered upon them by a steep and stony mountain path, but who, in doing so, has passed many a stage from which a good point of view is obtained. If therefore I relate to you what I consider I have observed, it is with the understand- ing that I wish to regard myself as open to instruction by those more experienced than myself. The physiological study of the manner in which the perceptions of our senses originate, how impressions from without pass into our nerves, and how the condi- tion of the latter is thereby altered, presents many points of contact with the theory of the fine arts. On a former occasion T endeavoured to establish such a relation between the physiology of the sense of hearing, and the theory of music. Those relations in that case are particularly clear and distinct, because the elemen- tary forms of music depend more closely on the nature and on the peculiarities of our perceptions than is the case in other arts, in which the nature of the material to be used and of the objects to be represented has a far greater influence. Yet even in those other branches of art, the especial mode of perception of that organ of sense by which the impression is taken up is not without importance ; and a theoretical in- sight into its action, and into the principle of its methods, cannot be complete if this physiological ele- ment is not taken into account. Next to music this ON THE RELATION OF OPTICS TO PAINTING. 75 seems to predominate more particularly in painting, and this is the reason why I have chosen painting as the subject of my present lecture. The more immediate object of the painter is to produce in us by his palette a lively visual impression of the objects which he has endeavoured to represent. The aim, in a certain sense, is to produce a kind of optical illusion ; not indeed that, like the birds who pecked at the painted grapes of Apelles, we are to sup- pose we have present the real objects themselves, and not a picture ; but in so far that the artistic represen- tation produces in us a conception of their objects as vivid and as powerful as if we had them actually before us. The study of what are called illusions of the senses is however a very prominent and important part of the physiology of the senses ; for just those cases in which external impressions evoke conceptions which are not in accordance with reality are particularly in- structive, for discovering the laws of those means and processes by which normal perceptions originate. We must look upon artists as persons whose observation of sensuous impressions is particularly vivid and accu- rate, and whose memory for these images is particu- larly true. That which long tradition has handed down to the men most gifted in this respect, and that which they have found by innumerable experi- ments in the most varied directions, as regards means 76 ON THE RELATION OF OPTICS TO PAINTING. and methods of representation, forms a series of import- ant and significant facts, which the physiologist, who has here to learn from the artist, cannot afford to ne- glect. The study of works of art will throw great light on the question as to which elements and relations of our visual impressions are most predominant in deter- mining our conception of what is seen, and what others are of less importance. As far as lies within his power, the artist will seek to foster the former at the cost of the latter. In this sense then a careful observation of the works of the great masters will be serviceable, not only to physiological optics, but also because the investigation of the laws of the perceptions and of the observations of the senses will promote the theory of art, that is, the comprehension of its mode of action. We have not here to do with a discussion of the ultimate objects and aims of art, but only with an ex- amination of the action of the elementary means with which it works. The knowledge of the latter must, however, form an indispensable basis for the solution of the deeper questions, if we are to understand the problems which the artist has to solve, and the mode in which he attempts to attain his object. I need scarcely lay stress on the fact, following as it does from what I have already said, that it is not my intention to furnish instructions according to which ON THE EELATION OF OPTICS TO PAINTING. 77 the artist is to work. I consider it a mistake to sup- pose that any kind of aesthetic lectures such as these can ever do so ; but it is a mistake which those very frequently make who have only practical objects in view. 78 OS THE RELATION OF OPTICS TO PAINTIN&. I. FORM. The painter seeks to produce in his picture an image of external objects. The first aim of our investigation must be to ascertain what degree and what kind of similarity he can expect to attain, and what limits are assigned to him by the nature of his method. The uneducated observer usually requires nothing more than an illusive resemblance to nature : the more this is obtained, the more does he delight in the picture. An observer, on the contrary, whose taste in works of art has been more finely educated, will, consciously or unconsciously, require something more, and something different. A faithful copy of crude Nature he will at most regard as an artistic feat. To satisfy him, he will need artistic selection, grouping, and even idealisa- tion of the objects represented. The human figures in a work of art must not be the everyday figures, such as we see in photographs ; they must have ex- pression, and a characteristic development, and if possible beautiful forms, which have perhaps be- longed to no living individuals or indeed any indi- viduals which ever have existed, but only to such a one as might exist, and as must exist, to produce a ON THE RELATION OF OPTICS TO PAINTING. 79 vivid perception of any particular aspect of human existence in its complete and unhindered development. If however the artist is to produce an artistic arrangement of only idealised types, whether of man or of natural objects, must not the picture be an actual, complete, and directly true delineation of that which would appear if it anywhere came into being ? Since the picture is on a plane surface, this faith- ful representation can of course only give a faithful perspective view of the objects. Yet our eye, which in its optical properties 'is equivalent to a camera obscura, the well-known apparatus of the photo- grapher, gives on the retina, which is its sensitive plate, only perspective views of the external world ; these are stationary, like the drawing on a picture, as long as the standpoint of the eye is not altered. And, in fact, if we restrict ourselves in the first place to the form of the object viewed, and disregard for the present any consideration of colour, by a correct perspective drawing we can present to the eye of an observer, who views it from a correctly chosen point of view, the same forms of the visual image as the inspection of the objects themselves would present to the same eye, when viewed from the corresponding point of view. But apart from the fact that any movement of the observer, whereby his eye changes its position, will 80 ON THE EELATION OF OPTICS TO PAINTING. produce displacements of the visual image, different when he stands before objects from those when he stands before the image, I could speak of only one eye for which equality of impression is to be estab- lished. We however see the world with two eyes, which occupy somewhat different positions in space, and which therefore show two different perspective views of objects before us. This difference of the images of the two eyes forms one of the most im- portant means of estimating the distance of objects from our eye, and of estimating depth, and this is what is wanting to the painter, or even turns against him; since in binocular vision the picture distinctly forces itself on our perception as a plane surface. You must all have observed the wonderful vividness which the solid form of objects acquires when good stereoscopic images are viewed in the stereoscope, a kind of vividness in which either of the pictures is wanting when viewed without the stereoscope. The illusion is most striking and instructive with figures in simple line ; models of crystals and the like, in which there is no other element of illusion. The reason of this deception is, that looking with two eyes we view the world simultaneously from somewhat different points of view, and thereby acquire two dif- ferent perspective images. With the right eye we see somewhat more of the right side of objects before us,, ON THE KELATION OF OPTICS TO PAINTING. 81 and also somewhat more of those behind it, than we do with the left eye ; and conversely we see with the left, more of the left side of an object, and of the back- ground behind its left edges, and partially concealed by the edge. But a flat picture shows to the right eye absolutely the same picture, and all objects represented upon it, as to the left eye. If then we make for each eye such a picture as that eye would perceive if itself looked at the object, and if both pictures are combined in the stereoscope, so that each eye sees its correspond- ing picture, then as far as form is concerned the same impression is produced in the two eyes as the object itself produces. But if we look at a drawing or a picture with both eyes, we just as easily recognise that it is a representation on a plane surface, which is different from that which the actual object would show simultaneously to both eyes. Hence is due the well- known increase in the vividness of a picture if it is looked at with only one eye, and while quite stationary, through a dark tube ; we thus exclude any comparison of its distance with that of adjacent objects in the room. For it must be observed that as we use differ- ent pictures seen with the two eyes for the perception of depth, in like manner as the body moves from one place to another, the pictures seen by the same eye serve for the same purpose. In moving, whether on foot or riding, the nearer objects are apparently dis- ii. O 82 ON THE RELATION OF OPTICS TO PAINTING. placed in comparison with the more distant ones ; the former appear to recede, the latter appear to move with us. Hence arises a far stricter distinction between what is near and what is distant, than seeing with one eye from one and the same spot would ever afford us. If we move towards the picture, the sensuous impression that it is a flat picture hanging against the wall forces itself more strongly upon us than if we look at it while we are stationary. Compared with a large picture at a greater distance, all those elements which depend on bin- ocular vision and on the movement of the body are less operative, because in very distant objects the differ- ences between the images of the two eyes, or be- tween the aspect from adjacent points of view, seem less. Hence large pictures furnish a less distorted aspect of their object than small ones, while the impression on a stationary eye, of a small picture close at hand, might be just the same as that of a large distant one. In a painting close at hand, the fact that it is a flat picture continually forces itself more power- fully and more distinctly on our perception. The fact that perspective drawings, which are taken from too near a point of view, may easily produce a distorted impression, is, I think, connected with this. For here the want of the second representation for the other eye, which would be very different, is too marked. On the other hand, what are called geometrical pro- ON THE RELATION OF OPTICS TO PAINTING. 83 jections, that is, perspective drawings which represent a view taken from an infinite distance, give in many cases a particularly favourable view of the object, although they correspond to a point of sight which does not in reality occur. Here the pictures of both eyes for such an object are the same. You will notice that in these respects there is a primary incongruity, and one which cannot be got over, between the aspect of a picture and the aspect of reality. This incongruity may be lessened, but never entirely overcome. Owing to the imperfect action of binocular vision, the most important natural means is lost of enabling the observer to estimate the depth of objects represented in the picture. The painter possesses a series of subordinate means, partly of limited applicability, and partly of slight effect, of expressing various distances by depth. It is not unimportant to become acquainted with these elements, as arising out of theoretical considerations ; for in the practice of the art of painting' they have manifestly exercised great influence on the arrangement, selec- tion, and mode of illumination of the objects repre- sented. The distinctness of what is represented is indeed of subordinate importance when considered in reference to the ideal aims of art ; it must not however be depreciated, for it is the first condition by which the observer attains an intelligibility of expres- e 2 84. ON THE RELATION OF OPTICS TO PAINTING. sion, which impresses itself without fatigue on the observer. This direct intelligibility is again the preliminary condition for an undisturbed, and vivid action of the picture on the feelings and mood of the observer. The subordinate methods of expressing depth which have been referred to, depend in the first place on per- spective. Nearer objects partially conceal more distant ones, but can never themselves be concealed by the latter. If therefore the painter skilfully groups his ob- jects, so that the feature in question comes into play, this gives at once a very certain gradation of far and near. This mutual concealment may even preponderate over the binocular perception of depth, if stereoscopic pictures are intentionally produced in which each coun- teracts the other. Moreover, in bodies of regular or of known form, the forms of perspective projection are for the most part characteristic for the depth of the object. If we look at houses, or other results of man's artistic activity, we know at the outset that the forms are for the most part plane surfaces at right angles to each other, with occasional circular or even spheroidal surfaces. And in fact, when we know so much, a correct perspective drawing is sufficient to produce the whole shape of the body. This is also the case with the figures of men and animals which are familiar to us, and whose forms moreover show two symmetrical halves. The best per- ON THE RELATION OF OPTICS TO PAINTING. 85 spective drawing is however of but little avail in the case of irregular shapes, rough blocks of rock and ice, masses of foliage, and the like ; that this is so, is best seen in photographs, where the perspective and shading may be absolutely correct, and yet the total impression is indistinct and confused. When human habitations are seen in a picture, they represent to the observer the direction of the hori- zontal surfaces at the place at which they stand ; and in comparison therewith the inclination of the ground, which without them would often be difficult to repre- sent. The apparent magnitude which objects, whose actual magnitude is known, present in different parts of the picture must also be taken into account. Men and animals, as well as familiar trees, are useful to the painter in this respect. In the more distant centre of the landscape they appear smaller than in the fore- ground, and thus their apparent magnitude furnishes a measure of the distance at which they are placed. Shadows, and more especially double ones, are of great importance. You all know how much more distinct is the impression which a well-shaded drawing gives as distinguished from an outline ; the shading is hence one of the most difficult, but at the same time most effective, elements in the productions of the draughtsman and painter. It is his task to imitate 86 ON THE RELATION OP OPTICS TO PAIXTINQ. the fi.ae gradation and transitions of light and shade on rounded surfaces, which are his chief means of ex- pressing their modelling, with all their fine changes of curvature ; he must take into account the extension or restriction of the sources of light, and the mutual reflection of the surfaces on each other. While the modifications of the lighting on the surface of bodies themselves is often dubious — for instance, an intaglio of a medal may, with a particular illumination, pro- duce the impression of reliefs which are only illumi- nated from the other side — double shadows, on the contrary, are undoubted indications that the body which throws the shadow is nearer the source of light than that which receives the shadow. This rule is so com- pletely without exception, that even in stereoscopic views a falsely placed double shadow may destroy or confuse the entire illusion. The various kinds of illumination are not all equally favourable for obtaining the full effect of shadows. When the observer looks at the objects in the same direction as that in which light falls upon them, he sees only their illuminated sides and nothing of the shadow; the whole relief which the shadows could give then disappears. If the object is between the source of light and the observer he only sees the shadows. Hence we need lateral illumination for a picturesque shading ; and over surfaces which like those of plane ON THE RELATION OF OPTICS TO PAINTING. 87 + or hilly land only present slightly moving figures, we require light which is almost in the direction of the surface itself, for only such a one gives shadows. This is one of the reasons which makes illumination by the rising or the setting sun so effective. The forms of the landscape become more distinct. To this must also be added the influence of colour, and of aerial light, which we shall subsequently discuss. Direct illumination from the sun, or from a flame, makes the shadows sharply defined, and hard. Illu- mination from a very wide luminous surface, such as a cloudy sky, makes them confused, or destroys them altogether. Between these two extremes there are transitions; illumination by a portion of the sky, defined by a window, or by trees, &c., allows the shadows to be more or less prominent according to the nature of the object. You must have seen of what importance this is to photographers, who have to modify their light by all manner of screens and curtains in order to obtain well-modelled portraits. Of more importance for the representation of depth than the elements hitherto enumerated, and which are more or less of local and accidental signific- ance, is what is called aerial perspective. By this we understand the optical action of the light, which the illuminated masses of air, between the observer and distant objects, give. This arises from a fine opacity 88 ON THE RELATION OF OPTICS TO PAINTING. in the atmosphere, which never entirely disappears* If, in a transparent medium, there are fine transparent particles of varying density and varying refrangibility, in so far as they are struck by it, they deflect the light passing through such a medium, partly by reflec- tion and partly by refraction ; to use an optical expres- sion, they scatter it in all directions. If the opaque particles are sparsely distributed, so that a great part of the light can pass through them without being deflected, distant objects are seen in sharp, well-defined outlines through such a medium, while at the same time a portion of the light which is deflected is dis- tributed in the transparent medium as an opaque halo. Water rendered turbid by a few drops of milk shows this dispersion of the light and cloudiness very distinctly. The light in this case is deflected by the microscopic globules of butter which are suspended in the milk. In the ordinary air of our rooms, this turbidity is very apparent when the room is closed, and a ray of sunlight is admitted through a narrow aperture. We see then some of these solar particles, large enough to be distinguished by the naked eye, while others form a fine homogeneous turbidity. But even the latter must consist mainly of suspended particles of organic substances, for, according to an observation of Tyndall, they can be burnt. If the flame of a spirit lamp is placed directly below the path of these rays, the air ON THE .RELATION OF OPTICS TO PAINTING. 89 rising from the flame stands out quite dark in the surrounding bright turbidity; that is to say, the air rising from the flame has been quite freed from dust. In the open air, besides dust and occasional smoke, we must often also take into account the turbidity arising from incipient aqueous deposits, where the tempera- ture of moist air sinks so far that the water retained in it can no longer exist as invisible vapour. Part of the water settles then in the form of fine drops, as a kind of the very finest aqueous dust, and forms a finer or denser fog; that is to say, cloud. The turbidity which forms in hot sunshine and dry air may arise, partly from dust which the ascending currents of warm air whirl about; and partly from the irregular mixture of cold and warm layers of air of different density, as is seen in the tremulous motion of the lower layers of air over surfaces irradiated by the sun. But science can as yet give no explanation of the turbidity in the higher regions of the atmosphere which produces the blue of the sky ; we do not know whether it arises from suspended particles of foreign substances, or whether the molecules of air themselves may not act as turbid particles in the luminous ether. The colour of the light reflected by the opaque particles mainly depends on their magnitude. When a block of wood floats on water, and by a succession of falling drops we produce small wave-rings near it, 90 ON THE RELATION OF OPTICS TO FAIN'TING these are repelled by the floating wood as if it. were a solid wall. But in the long waves of the sea, a block of wood would be rocked about without the waves being thereby materially disturbed in their progress. Now light is well known to be an undulatory motion of the ether which fills all space. The red and yellow rays have the longest waves, the blue and violet the shortest. Very fine particles, therefore, which disturb the uniformity of the ether, will accordingly reflect the latter rays more markedly than the red and yellow rays. The light of turbid media is bluer, the finer are the opaque particles ; while the larger particles of uniform light reflect all colours, and therefore give a whitish turbidity. Of this kind is the celestial blue, that is, the colour of the turbid atmosphere as seen against dark cosmical space. The purer and the more transparent the air, the bluer is the sky. In like man ner it is bluer and darker when we ascend high moun- tains, partly because the air at great heights is freer from turbidity, and partly because there is less air above us. But the same blue, which is seen against the dark celestial space, also occurs against dark terrestrial objects ; for instance, when a thick layer of illuminated air is between us and masses of deeply shaded or wooded hills. The same aerial light makes the sky blue, as well as the mountains ; excepting that in the former case it is pure, while in the latter it is mixed ON THE RELATION OF OPTICS TO PAINTING. 91 with the light from objects behind; and moreover it belongs to the coarser turbidity of the lower regions of the atmosphere, so that it is whiter. In hot coun- tries, and with dry air, the aerial turbidity is also finer m the lower regions of the air, and therefore the blue in front of distant terrestrial objects is more like that of the sky. The clearness and the pure colours of Italian landscapes depend mainly on this fact. On high mountains, particularly in the morning, the aerial turbidity is often so slight that the colours of the most distant objects can scarcely be distinguished from those of the nearest. The sky may then appear almost bluish-black. Conversely, the denser turbidity consists mainly of coarser particles, and is therefore whitish. As a rule, this is the case in the lower layers of air, and in states of weather in which the aqueous vapour in the air is near its point of condensation. On the other hand, the light which reaches the eye of the observer after having passed through a long layer of air, has been robbed of part of its violet and blue by scattered reflections ; it therefore appears yel- lowish to reddish-yellow or red, the former when the turbidity is fine, the latter when it is coarse. Thus the sun and the moon at their rising and setting, and also distant brightly illuminated mountain-tops, espe- cially siiow-mountains, appear coloured. 92 ON THE RELATION OF OPTICS TO PAINTING. These colourations are moreover not peculiar to the air, but occur in all cases in which a transparent substance is made turbid by the admixture of another transparent substance. We see it, as we have ob- served, in diluted milk, and in water to which a few drops of eau de Cologne have been added, whereby the ethereal oils and resins dissolved by the latter, sepa- rate out and produce the turbidity. Excessively fine blue clouds, bluer even than the air, may be produced, as Tyndall has observed, when the sun's light is allowed to exert its decomposing action on the vapours of certain carbon compounds. Groethe called attention to the universality of this phenomenon, and ende*- voured to base upon it his theory of colour. By aerial perspective we understand the artistic representation of aerial turbidity; for the greater or less predominance of the aerial colour above the colour of the objects, shows their varying distance very definitely ; and landscapes more especially acquire the appearance of depth. According to the weather, the turbidity of the air may be greater or less, more white or more blue. Very clear air, as sometimes met with after continued rain, makes the distant mountains appear small and near ; whereas, when the air contains more vapour, they appear large and distant. This latter is decidedly better for the landscape painter, and the high transparent landscapes of moun- ON THE RELATION OF OPTICS TO PAINTING. 93 tainous regions, which so often lead the Alpine climber to under-estimate the distance and the magnitude of the mountain-tops before him, are also difficult to turn to account in a picturesque manner. Views from the valleys, and from seas and plains in which the aerial light is faintly but markedly developed, are far better ; not only do they allow the various distances and mag- nitudes of what is seen to stand out, but they are on the other hand favourable to the artistic unity of colouration. Although aerial colour is most distinct in the greater depths of landscape, it is not entirely wanting in front of the near objects of a room. What is seen to be isolated and well denned, when sunlight passes into a dark room through a hole in the shutter, is also not quite wanting when the whole room is lighted. Here, also, the aerial lighting must stand out against the background, and must somewhat deaden the colours in comparison with those of nearer objects; and these differences, also, although far more delicate than against the background of a landscape, are important for the historical, genre, or portrait painter ; and when they are carefully observed and imitated, they greatly heighten the distinctness of his representation. 94 ON THE RELATION OF OPTICS TO PAINTING. II. SHADE. The circumstances which we have hitherto dis- cussed indicate a profound difference, and one which is exceedingly important for the perception of solid form, between the visual image which our eyes give, when we stand before objects, and that which the picture gives. The choice of the objects to be represented in pictures is thereby at once much restricted. Artists are well aware that there is much which cannot be represented by the means at their disposal. Part of their artistic skill consists in the fact that by a suitable grouping, position, and turn of the objects, by a suitable choice of the point of view, and by the mode of lighting, they learn to overcome the unfavourable conditions which are imposed on them in this respect. It might at first sight appear that of the requisite truth to nature of a picture, so much would remain that, seen from the proper point of view, it would at least produce the same distribution of light, colour, and shadow in its field of view, and would produce in the interior of the eye exactly the same image on the retina as the object represented would do if we had it actually before us, and looked at it from a definite, ON THE EELATION OF OPTICS TO PAINTING. 95 fixed point of- view. It might seem to be an object of pictorial skill to aim at producing, under the given limitations, the same effect as is produced by the object itself. / If we proceed to examine whether, and how far, painting can satisfy such a condition, we come upon difficulties before which we should perhaps shrink, if we did not know that they had been already over- come. Let us begin with the simplest case ; with the quan- titative relations between luminous intensities. If the artist is to imitate exactly the impression which the object produces on our eye, he ought to be able to dispose of brightness and darkness equal to that which nature offers. But of this there can be no idea. Let me give a case in point. Let there be, in a pic- ture-gallery, a desert-scene, in which a procession of Bedouins, shrouded in white, and of dark negroes, marches under the burning sunshine; close to it a bluish moonlight scene, where the moon is reflected in the water, and groups of trees, and human forms, are seen to be faintly indicated in the darkness. You know from experience that both pictures, if they are well done, can produce with surprising vividness the representation of their objects; and yet, in both pictures, the brightest parts are produced with the same white-lead, which is but slightly altered by ad- 96 ON THE KELATION OF OPTICS TO PAINTING. mixtures ; while the darkest parts are produced with the same black. Both, being hung on the same wall, share the same light, and the brightest as well as the darkest parts of the two scarcely differ as concerns the degree of their brightness. How is it, however, with the actual degrees of brightness represented? The relation between the brightness of the sun's light, and that of the moon, was measured by Wollaston, who compared their in- tensities with that of the light of candles of the same material. He thus found that the luminosity of the sun is 800,000 times that of the brightest light of a full moon. An opaque body, which is lighted from any source whatever, can, even in the most favourable case, only emit as much light as falls upon it. Yet, from Lam- bert's observations, even the whitest bodies only reflect about two fifths of the incident light. The sun's rays, which proceed parallel from the sun, whose diameter is 85,000 miles, when they reach us, are distributed uniformly over a sphere 195 millions of miles in dia- meter. Its density and illuminating power is here only the one forty-thousandth of that with which it left the sun's surface ; and Lambert's number leads to the conclusion that even the brightest white surface on which the sun's rays fall vertically, has only the one hundred- thousandth part of the brightness of the ON THE KELAT10N OF OPTICS TO PAINTING. 97 sun's disk. The moon however is a gray body, whose mean brightness is only about one fifth of that of the purest white. And when the moon irradiates a body of the purest white on the earth, its brightness is only the hundred- thousandth part of the brightness of the moon itself ; hence the sun's disk is 80,000 million times brighter than a white which is irradiated by the full moon. Now pictures which hang in a room are not lighted by the direct light of the sun, but by that which is re- flected from the sky and clouds. I do not know of ^iny direct measurements of the ordinary brightness of the light in a picture gallery, but estimates may be made from known data. With strong upper light and bright light from the clouds, the brightest white on a picture has probably l-20th of the brightness of white directly lighted by the sun ; it will generally be only l-40th, or even less. Hence the painter of the desert, even if he gives up the representation of the sun's disk, which is always very imperfect, will have to represent the glaringly lighted garments of his Bedouins with a white which, in the most favourable case, shows only the 1-2 Oth part of the brightness which corresponds to actual fact. If he could bring it, with its lighting unchanged, into the desert near the white there, it would seem like a dark grey. 1 found in fact, by an experiment, tha.t lamp- H. ii 98 ON THE RELATION OF OPTICS TO PAIXTINIK black, lighted by the sun, is not less than balf as bright, as shaded white in the brighter part of a room. On the picture of the moon, the same white which has been used for depicting the Bedouins' garments must be used for representing the moon's disk, and its reflection in the water ; although the real moon ha a only one fifth of this brightness, and its reflection in water still less. Hence white garments in moonlight, or marble surfaces, even when the artist gives them a grey shade, will always be ten to twenty times as bright in his picture as they are in reality. On the other hand, the darkest black which the artist could apply would be scarcely sufficient to repre- sent the real illumination of a white object on which the moon shone. For even the deadest black coatings of lamp-black, black velvet, when powerfully lighted appear grey, as we often enough know to our cost, when we wish to shut off superfluous light. I investigated a coating of lamp-black, and found its brightness to be about ^fa that of white paper. The brightest colours of a painter are only about one hundred times as bright as his darkest shades. The statements I have made may perhaps appear exaggerated. But they depend upon measurements, and you can control them by well-known observations. According to Wollaston, the light of the full moon is ON THE EELATION OF OPTICS TO PAINTING. 99 equal to that % of a candle burning at a distance of 12 feet. You know that we cannot read by the light of the full moon, though we can read at a distance of three or four feet from a candle. Now assume that you suddenly passed from a room in daylight to a vault perfectly dark, with the exception of the light of a single candle. You would at first think you were in absolute darkness, and at most you would only recognise the candle itself. In any case, you would not recognise the slightest trace of any objects at a distance of 12 feet from the candle. These however are the objects whose illumination is the same as that which the moonlight gives. You would only become accustomed to the darkness after some time, and you would then find your way about without difficulty. If, now, you return to the daylight, which before was perfectly comfortable, it will appear so dazzling that you will perhaps have to close the eyes, and only be able to gaze round with a painful glare. You see thus that we are concerned here not with minute, but with colossal, differences. How now is it possible that, under such circumstances, we can imagine there is any similarity between the picture and reality ? Our discussion of what we did not see at first, but could afterwards see in the vault, points to the most important element in the solution ; it is the varying extent to which our senses are deadened by light ; a E 2 100 ON THE RELATION OF OPTICS TO PAINTING. process to which we can attach the same name, fatigue, as that for the corresponding one in the muscle. Any activity of our nervous system diminishes its power for the time being. The muscle is tired by work, the brain is tired by thinking, and by mental operations ; the eye is tired by light, and the more so the more powerful the light. Fatigue makes it dull and in- sensitive to new impressions, so that it appreciates strong ones only moderately, and weak ones not at all. But now you see how different is the aim of the artist when these circumstances are taken into account. The eye of the traveller in the desert, who is looking at the caravan, has been dulled to the last degree by the dazzling sunshine ; while that of the wanderer by moon- light has been raised to the extreme of sensitiveness. The condition of one who is looking at a picture differs from both the above cases by possessing a cer- tain mean degree of sensitiveness. Accordingly, the painter must endeavour to produce by his colours, on the moderately sensitive eye of the spectator, the same impression as that which the desert, on the one hand, produces on the deadened, and the moonlight, on the other hand, creates on the untired eye of its observer. Hence, along with the actual luminous phenomena of the outer world, the different physiological conditions of the eye play a most important part in the work of the artist. What he has to give is not a mere tran- ON THE RELATION OF OPTICS TO PAINTING. 101 script of the object, but a translation of his impression into another scale of sensitiveness, which belongs to a different degree of impressibility of the observing eye, in which the organ speaks a very different dialect in responding to the impressions of the outer world. In order to understand to what conclusions this leads, I must first of all explain the law which Fechner discovered for the scale of sensitiveness of the eye, which is a particular case of the more general psycho- physical law of the relations of the various sensuous impressions to the irritations which produce them. This law may be expressed as follows: Within very wide limits of brightness, differences in the strength of light are equally distinct or appear equal in sensation, if they form an equal fraction of the total quantity of light compared. Thus, for instance, differences in in- tensity of one hundredth of the total amount can be recognised without great trouble with very different strengths of light, without exhibiting material dif- ferences in the certainty and facility of the estimate, whether the brightest daylight or the light of a good candle be used. The easiest method of producing accurately mea- surable differences in the brightness of two white surfaces, depends on the use of rapidly rotating disks. If a disk, like the adjacent one in Fig. 3, is made to rotate very rapidly (that is, 20 to 30 times in a second), 102 ON THE RELATION OF OPTICS TO PAINTING. it appears to the eye to be covered with three grey rings as in Fig. 4. The reader must, however, figure to himself the grey of these rings, as it appears on FIG. 3. FIG. 4. the rotating disk of Fig. 3, as a scarcely perceptible shade of the ground. When the rotation is rapid each ring of the disk appears illuminated, as if all the light which fell upon it had been uniformly distributed over its entire surface. Those rings, in which are the black bands, have somewhat less light than the quite white ones, and if the breadth of the marks is com- pared with the length of half the circumference of the corresponding ring, we get the fraction by which the intensity of the light in the white ground of the disk is diminished in the ring in question. If the bands are all equally broad, as in Fig. 3, the inner rings appear darker than the outer ones, for in this latter case the same loss of light is distributed over a larger area than in the former. In this way extremely delicate shades of ON THE KELATION 0*F OPTICS TO PAINTING. 103 brightness may be obtained, and by this method, when the strength of the illumination varies, the brightness always diminishes by the same proportion of its total value. Now it is found, in accordance with Fechners law, that the distinctness of the rings is nearly con- stant for very different strengths of light. We ex- clude, of course, the cases of too dazzling or of too dim a light. In both cases the finer distinctions can no longer be perceived by the eye. The case is quite different when for different strengths of illumination we produce differences which always correspond to the same quantity of light. If, for instance, we close the shutter of a room at daytime, so that it is quite dark, and now light it by a candle, we can discriminate without difficulty the shadows, such as that of the hand, thrown by the candle on a sheet of white paper. If, however, the shutters are again opened, so that daylight enters the room, for the same position of the hand we can no longer recognise the sha- dow, although there falls on that part of the white sheet, which is not struck by this shadow, . the same excess of candle-light as upon the parts shaded by the hand. But this small quantity of light disappears in compari- son with the newly added daylight, provided that this strikes all parts of the white sheet uniformly. You see then that, while the difference between candle-light and darkness can be easily perceived, the equally great J04 ON THE EELATiON OF OPTICS TO PAINTING. difference between daylight, on the one hand, and day light plus candle-light on the other, can be no longei recognised. This law is of great importance in discriminating between various degrees of brightness of natural objects. A white body appears white because it reflects a large fraction, and a grey body appears grey because it re- flects a small fraction, of incident light. For different intensities of illumination, the difference of brightness between the two will always correspond to the same frac- tion of their total brightness, and hence will be equally perceptible to our eyes, provided we do not approach too near to the upper or the lower limit of the brightness, for which Fechner's law no longer holds. Hence, on the whole, the painter can produce what appears an equal difference for the spectator of his picture, notwithstand- ing the varying strength of light in the gallery, provided he gives to his colours the same ratio of brightness as that which actually exists. For, in fact, in looking at natural objects, the abso- lute brightness in which they appear to the eye varies within very wide limits, according to the intensity of the light, and the sensitiveness of the eye. That which is constant is only the ratio of the brightness in which surfaces of various depth of colour appear to us when lighted to the same amount. But this ratio of bright- ness is for us the perception, from which we form our ON THE RELATION OF OPTICS TO TAINTING. 100 judgment as Ho the lighter or darker colour of the bodies we see. Now this ratio can be imitated by the painter without restraint, and in conformity with na- ture, to evoke in us the same conception as to the nature of the bodies seen. A truthful imitation in this respect would be attained within the limits in which Fechner's law holds, if the artist reproduced the fully lighted parts of the objects which he has to represent with pigments, which, with the same light, were equal to the colours to be represented. This is approximately the case. On the whole, the painter chooses coloured pigments which almost exactly reproduce the colours of the bodies represented, especially for objects of no great depth, such as portraits, and which are only darker in the shaded parts. Children begin to paint on this principle; they imitate one colour by another; and, in like manner also, nations in which painting has remained in a childish stage. Perfect artistic painting is only reached when we have succeeded in imitating the action of light upon the eye, and not merely the pigments; and only when we look at the object of pictorial representation from this point of view, will it be possible to understand the variations from nature which artists have to make in the choice of their scale of colour and of shade. These are, in the first case, due to the circumstance that Fechner's law only holds for mean degrees of 106 ON THE RELATION OF OPTICS TO PAINTING. brightness ; while, for a brightness which is too high or too low, appreciable divergences are met with. At both extremes of luminous intensity the eye is less sensitive for differences in light than is required by that law. With a very strong light it is dazzled ; that is, its internal activity cannot keep pace with the ex- ternal excitations ; the nerves are too soon tired. Very bright objects appear almost always to be equally bright, even when there are, in fact, material differ- ences in their luminous intensity. The light at the edge of the sun is only about half as bright as that at the centre, yet none of you will have noticed that, if you have not looked through coloured glasses, which reduce the brightness to a convenient extent. With a weak light the eye is also less sensitive, but from the opposite reason. If a body is so feebly illuminated that we scarcely perceive it, we shall not be able to perceive that its brightness is lessened by a shadow by the one hundredth or even by a tenth. It follows from this, that, with moderate illumina- tion, darker objects become more like the darkest objects, while with greater illumination brighter ob- jects become more like the brightest than should be the case in accordance with Fechner's law, which holds for mean degrees of illumination. From this results, what, for painting, is an extremely characteristic ON THE RELATION OF OPTICS TO PAINTING. 107 V difference between the impression of very powerful and very feeble illumination. When painters wish to represent glowing sunshine, they make all objects almost equally bright, and thus produce with their moderately bright colours the im- pression which the sun's glow makes upon the dazzled eye of the observer. If, on the contrary, they wish to represent moonshine, they only indicate the very brightest objects, particularly the reflection of moon- light on shining surfaces, and keep everything so dark as to be almost unrecognisable ; that is to say, they make all dark objects more like the deepest dark which they can produce with their colours, than should be the case in accordance with the true ratio of the luminosities. In both cases they express, by their gradation of the lights, the insensitiveness of the eye for differences of tco bright or too feeble lights. If they could employ the colour of the dazzling bright- ness of full sunshine, or of the actual dimness of moonlight, they would not need to represent the gradation of light in their picture other than it is in nature; the picture would then make the same im- pression on the eye as is produced by equal degrees of brightness of actual objects. The alteration in the scale of shade which has been described is necessary because the colours of the picture are seen in the mean brightness of a moderately lighted room, for 108 ON THE RELATION OF OPTICS TO PAINTING. which Fechners law holds ; and therewith objects are to be represented whose brightness is beyond the limits of this law. We find that the older masters, and pre-eminently Rembrandt, employ the same deviation, which corre- sponds to that actually seen in moonlight landscapes ; and this in cases in which it is by no means wished to produce the impression of moonshine, or of a similar feeble light. The brightest parts of the objects are given in these pictures in bright, luminous yellowish colours ; but the shades towards the black are made very marked, so that the darker objects are almost lost in an impermeable darkness. But this darkness is covered with the yellowish haze of powerfully lighted aerial masses, so that, notwithstanding their darkness, these pictures give the impression of sunlight, and the very marked gradation of the shadows, the contours of the faces and figures, are made extremely prominent. The deviation from strict truth to nature is very re- markable in this shading, and yet these pictures give particularly bright and vivid aspects of the objects. Hence they are of particular interest for understand- ing the principles of pictorial illumination. In order to explain these actions we must, I think, consider that while Fechner's law is approximately cor- rect for those mean lights which are agreeable to the eye, the deviations which are so marked, for too high or toe ON THE EELATIOX OF OPTICS TO PAINTING. 109 low lights, are not without some influence in the region of the middle lights. We have to observe more closely in order to perceive this influence. It is found, in fact, that when the very finest differences of shade are pro- duced on a rotating disk, they are only visible by a light which about corresponds to the illumination of a white paper on a bright day, which is lighted by the light of the sky, but is not directly struck by the sun. With such a light, shades of y^- or y^- of the total intensity can be recognised. The light in which pictures are looked at is, on the contrary, much feebler ; and if we are to retain the same distinctness of the finest shadows and of the modelling of the contours which it produces, the gradations of shade in the picture must be somewhat stronger than cor- responds to the exact luminous intensities. The darkest objects of the picture thereby become un- naturally dark, which is however not detrimental to the object of the artist if the attention of the observer is to be directed to the brighter parts. The great artistic effectiveness of this manner shows us that the chief emphasis is to be laid on imitating difference of brightness and not on absolute brightness ; and that the greatest differences in this latter respect can be borne without perceptible incongruity, if only their grada- tions are imitated with expression. 110 ON THE KELATION OF OPTICS TO PAINTING. III. COLOUR. With these divergences in brightness are connected certain divergences in colour, which, physiologically, are caused by the fact that the scale of sensitiveness is different for different colours. The strength of the sensation produced by light of a particular colour, and for a given intensity of light, depends altogether on the special reaction of that complex of nerves which are set in operation by the action of the light in question. Now all our sensations of colour are ad- mixtures of three simple sensations ; namely, of red, green, and violet,1 which, by a not improbable suppo- sition of Thomas Young, can be apprehended quite independently of each other by three different systems of nerve-fibres. To this independence of the different sensations of colour corresponds their independence in the gradation of intensity. Recent measurements 2 have shown that the sensitiveness of our eye for feeble shadows is greatest in the blue and least in the red. A difference of -^-^g- to -^-Q of the intensity can be observed in the blue, and with an untired eye 1 Helmholtz's Popular Scientific Lectures, pp. 232-52. * Dobrowolsky in Gracfe's Arckiv fur Oj)htlialmologie, vol. xviii. part i. pp. 24-92, ON THE RELATION OF OPTICS TO PAINTING. Ill of ^ in the red ; or when the colour is dimmed by being looked at for a long time, a difference of sVto^V- Ked therefore acts as a colour towards whose shades the eye i? relatively less sensitive than towards that of blue. In agreement with this, the impression of glare, as the intensity increases, is feebler in red than in blue. According to an observation of Dove, if a blue and a red paper be chosen which appear of equal brightness under a mean degree of white light, as the light is made much dimmer the blue appears brighter, and as the light is much strengthened, the red. I myself have found that the same differences are seen, and even in a more striking manner, in the red and violet spectral colours, and, when their intensity is increased only moderately, by the same fraction for both. Now the impression of white is made up of the impressions which the individual spectral colours make on our eye. If we increase the brightness of white, the strength of the sensation for the red and yellow rays will relatively be more increased than that for the blue and violet. In bright white, therefore, the former will produce a relatively stronger impression than the latter; in dull white the blue and bluish colours will have this effect. Very bright white appears therefore yellowish, and dull white appears bluish. In 112 ON THE RELATION OF OPTICS TO PAINTING. our ordinary way of looking at the objects about us, we are not so readily conscious of this ; for the direct comparison of colours of very different shade is diffi- cult, and we are accustomed to see in this alteration in the white the result of different illumination of one and the same white object, so that in judging pigment- colours we have learnt to eliminate the influence of brightness. If however to the painter is put the problem of imi- tating, with faint colours, white irradiated by the sun, he can attain a high degree of resemblance ; for by an admixture of yellow in his white he makes this colour preponderate just as it would preponderate in actual bright light, owing to the impression on the nerves. It is the same impression as that produced if we look at a clouded landscape through a yellow glass, and thereby give it the appearance of a sunny light. The artist will, on the contrary, give a bluish tint to moon- light, that is, a faint white ; for the colours on the picture must, as we have seen, be far brighter than the colour to be represented. In moonshine scarcely any other colour can be recognised than blue ; the blue starry sky or blue colours may still appear distinctly coloured, while yellow and red can only be seen as obscurations of the general bluish white or I wiil again remind you that these changes of ON TIIE RELATION OF OPTICS TO PAINTING. 113 colour TV o aid not be necessary if the artist 'had at his disposal colours of the same brightness, or the same faintness, as are actually shown by the bodies irradiated by the sun or by the moon. The change of colour, like the scale of shade, pre- viously discussed, is a subjective action which the artist must represent objectively on his canvas, since moderately bright colours cannot produce them. We observe something quite similar in regard to the phenomena of Contrast. By this term we under- stand cases in which the colour or brightness of a surface appears changed by the proximity of a mass of another colour or shade, and, in such a manner, that the original colour appears darker by the proximity of a brighter shade, and brighter by that of a darker shade ; while by a colour of a different kind it tends towards the complementary tint. The phenomena of contrast are very various, and depend on different causes. One class, ChevreuUs simul- taneous Contrast, is independent of the motions of the eyes, and occurs with surfaces where there are very slight differences in colour and shade. This contrast appears both on the picture and in actual objects, and is well known to painters. Their mixtures of colours on the palette often appear quite different to what they are on the picture. The changes of colour which are here met with are often very striking ; I will not, II. 1 114 ON THE EELATION OF OPTICS TO PAINTING. however, enter upon them, for they produce no diver- gence between the picture and reality. The second class of phenomena of contrast, and one which, for us, is more important, is met with in \x changes of direction of the glance, and more especially between surfaces in which there are great differences of shade and of colour. As the eye glides over bright and dark, or coloured objects and surfaces, the impres- sion of each colour changes, for it is depicted on por- tions of the retina which directly before were struck by other colours and lights, and were therefore changed in their sensitiveness to an impression. This kind of contrast is therefore essentially dependent on move- ments of the eye, and has been called by Chevreul, 'successive Contrast.9 We have already seen that the retina is more sen- sitive in the dark to feeble light than it was before. By strong light, on the contrary, it is dulled, and is less sensitive to feeble lights which it had before per- ceived. This latter process is designated as < Fatigue ' of the retina ; an exhaustion of the capability of the retina by its own activity, just as the muscles by their activity become tired. I must here remark that the fatigue of the retina by light does not necessarily extend to the whole surface ; but when only a small portion of this membrane is struck by a minute, defined picture it also be locally developed in this part only. ON THE RELATION OF OPTICS TO PAINTING. 115 You must all have observed the dark spots which move about in the field of vision, when we have been looking for only a short time towards the setting sun, and which physiologists call negative after-images of the sun. They are due to the fact that only those parts of the retina which are actually struck by the image of the sun in the eye, have become insensitive to a new impression of light. If, with an eye which is thus locally tired, we look towards a uniformly bright sur- face, such as the sky, the tired parts of the retina are more feebly and more darkly affected than the other portions, so that the observer thinks he sees dark spots in the sky, which move about with his sight. We have then in juxtaposition, in the bright parts of the sky, the impression which these make upon the untired parts of the retina, and in the dark spots their action on the tired portions. Objects, bright like the sun, produce negative after-images In the most striking manner; but with a little attention they may be seen even after much more moderate impres- sions of light. A longer time is required in order to de- velop such an impression, so that it may be distinctly recognised, and a definite point of the bright object must be fixed, without moving the eye, so that its image may be distinctly formed on the retina, and only a limited portion of the retina be excited and tired, just as in producing sharp photographic portraits, the i 2 116 ON TEE EELATION OF OPTICS TO PAINTING. object must be stationary during the time of exposure in order that its image may not be displaced on the sensitive plate. The after-image in the eye is, as it were, a photograph on the retina, which becomes visible owing to the altered sensitiveness towards fresh light, but only remains stationary for a short time ; it is longer, the more powerful and durable was the action of light. If the object viewed was coloured, for instance red paper, the after-image is of the complementary colour on a grey ground ; in this case of a bluish green.1 Kose-red paper, on the contrary, gives a pure green after-image, green a rose-red, blue a yellow, and yellow a blue. These phenomena show that in the retina partial fatigue is possible for the several colours. According to Thomas Young's hypothesis of the existence of three systems of fibres in the visual nerves,2 of which one set perceives red whatever the kind of irritation, the second green, and the third violet, with green light, only those fibres of the retina which are sensitive to green are powerfully excited and tired. 1 In order to see this kind of image as distinctly as possible, it is desirable to avoid all movements of the eye. On a large sheet of dark grey paper a small black cross is drawn, the centre of which is steadily viewed, and a quadrangular sheet of paper of that colour whose after-image is to be observed is slid from the side, so that one of its corners touches the cross. The sheet is allowed to remain for a mmute or two, the cross being steadily viewed, and it is then drawn snddenly away, without relaxing the view. In place of the sheet removed the after-image appears then on the dark ground. 2 See Helmholtz's Popular Lectures, first series, p. 250. ON THE RELATION OF OPTICS TO PAINTING. 117 If this same part of the, retina is afterwards illuminated with white light, the sensation of green is enfeebled, while that of red and violet is vivid and predominant ; their sum gives the sensation of purple, which mixed with the unchanged white ground forms rose-red. In the ordinary way of looking at light and coloured objects, we are not accustomed to fix continuously one and the same point ; for following with the gaze the play of our attentiveness, we are always turning it to new parts of the object as they happen to interest us. This way of looking, in which the eye is continually moving, and therefore the retinal image is also shift- ing about on the retina, has moreover the advantage of avoiding disturbances of sight, which powerful and continuous after-images would bring with them. Yet here also, after-images are not wanting ; only they are shadowy in their contours, and of very short duration. If a red surface be laid upon a grey ground, and if we look from the red over the edge towards the grey, the edges of the grey will seem as if struck by such an after-image of red, and will seem to be of a faint bluish green. But as the after-image rapidly disappears, it is mostly only those parts of the grey, which are nearest the red, which show the change in a marked degree. This also is a phenomenon which is produced more strongly by bright light and brilliant saturated colours than by fainter light and duller colours. The artist 118 ON THE RELATION OF OPTICS TO PAINTING. However, works for the most part with the latter. He produces most of his tints by mixture; each mixed pigment is, however, greyer and duller than the pure colour of which it is mixed, and even the few pig- ments of a highly saturated shade, which oil-painting can employ, are comparatively dark. The pigments employed in water-colours and coloured chalks are again comparatively white. Hence such bright con- trasts, as are observed in strongly coloured and strongly lighted objects in nature, cannot be expected from their representation in the picture. If, therefore, with the pigments at his command, the artist wishes to reproduce the impression which objects give, as strikingly as possible, he must paint the contrasts which they produce. If the colours on the picture are as brilliant and luminous as in the actual objects, the contrasts in the former case would produce them- selves as spontaneously as in the latter. Here, also, subjective phenomena of the eye must be objectively introduced into the picture, because the scale of colour and of brightness is different upon the latter. With a little attention you will see that painters and draughtsmen generally make a plain uniformly lighted surface brighter, where it is close to a dark object, and darker, where it is near a light object. You will find that uniform grey surfaces are given a yellowish tint at the edge where there is a back- ON THE KELAIION OF OPTICS TO PAINTING. 119 ground of blue, and a rose-red tint where they im- piiige on green, provided that none of the light collected from the blue or green can fall upon the grey. Where the sun's rays passing through the green leafy shade of trees strike against the ground, they appear to the eye, tired with looking at the predomi- nant green, of a rose-red tint; the whole daylight, entering through a slit, appears blue, compared with reddish yellow candle-light. In this way they are re- presented by the painter, since the colours of his pic- tures are not bright enough to produce the contrast without such help. To the series of subjective phenomena, which artists are compelled to represent objectively in their pictures, must be associated certain phenomena of irradiation. By this is understood cases in which any brig at object in the field spreads its light or colour over the neighbourhood. The phenomena are the more marked the brighter is the radiating object, and the halo is brightest in the immediate neighbour- hood of the bright object, but diminishes at a greater distance. These phenomena of irradiation are most striking around a very bright light on a dark ground. If the view of the flame itself is closed by a narrow dark object such as the finger, a bright misty halo dis- appears, which covers the whole neighbourhood, and, at the same time, any objects there may be in the dark J20 ON THE KELATION OF OPTICS TO PAINTING. part of the field of view are seen more distinctly . If the flame is partly screened by a ruler, this appears jagged where the flame projects beyond it. The lu-> minosity in the neighbourhood of the flame is so in- tense, that its brightness can scarcely be distinguished from that of the flame itself; as is the case with all bright objects, the flame appears magnified, and as if spreading over towards the adjacent dark objects. The cause of this phenomenon is quite similar to that of aerial perspective. It is due to a diffusion of light which arises from the passage of light through dull media, excepting that for the phenomena of aerial perspective the turbidity is to be sought in the air in front of the eye, while for true phenomena of irradiation it is to be sought in the transparent media of the eye. \Vhen even the healthiest human eye is examined by powerful light, the best being a pencil of sunlight concentrated on the side by a condensing lens, it is seen that the sclerotica and crystalline lens ar« not per- fectly clear. If strongly illuminated, they both appear whitish and as if rendered turbid by a fine mist. Both are, in fact, tissues of fibrous structure, and are not therefore so homogeneous as a pure liquid or a pure crys- tal. Every inequality, however small, in the structure of a transparent body can, however, reflect some of the incident light— that is, can diffuse it in all directions.' 1 I disregard here the view that irradiation in the eye depends on ON THE RELATION OF OPTICS TO TAINTING. 121 The phenomena of irradiation also occur with moderate degrees of brightness. A dark aperture in a sheet of paper illuminated by the sun, or .a small dark object on a coloured glass plate which is held against the clear sky, appear as if the colour of the adjacent surface were diffused over them. Hence the phenomena of irradiation are very similar to those which produce the opacity of the air. The only essential difference lies in this, that the opacity by luminous air is stronger before distant objects which have a greater mass of air in front of them than before near ones ; while irradiation in the eye sheds its halo uniformly over near and over distant objects. Irradiation also belongs to the subjective pheno- mena, of the eye which the artist represents objectively, because painted lights and painted sunlight are not bright enough to produce a distinct irradiation in the eye of the observer. The representation which the painter has to give of the lights and colours of his object I have described as a translation, and I have urged that, as a general rule, it cannot give a copy true in all its details. The altered scale of brightness which the artist must apply in many cases is opposed to this. It is not the colours of the objects, but the impression which they a, diffusion of the excitation in the substance of the nerves, as this appears to me too hj-pothetical. Moreover, we are here concerned jvith the phenomena and not with their cause. 122 ON THE RELATION OF OPTICS TO PAIXTINO. have given, or would give, which is to be imitated, so as to produce as distinct and vivid a conception as pos- sible of those objects. As the painter must change the scale of light and colour in which he executes his picture, he only alters something which is subject to manifold change according to the lighting, and the degree of fatigue of the eye. He retains the more essential, that is, the gradations of brightness and tint. Here present themselves a series of phenomena which are occasioned by the manner in which the eye replies to an external irritation ; and since they depend upon the intensity of this irritation they are not directly produced by the varied luminous intensity and colours of the picture. These objective phenomena, which occur on looking at the object, would be wanting if the painter did not represent them objectively on his can- vas. The fact that they are represented is particu- larly significant for the kind of problem which is to be solved by a pictorial representation. Now, in all translations, the individuality of the translator plays a part. In artistic productions many important points are left to the choice of the artist, which he can decide according to his individual taste, or according to the requirements of his subject. Within certain limits he can freely select the absolute brightness of his colours, as well as the strength of the shadows. Like Kembrandt, he may exaggerate them ON THE RELATION OF OPTICS TO PAINTING. 123 in order to obtain strong relief ; or he may dimmish them, with Fra Angelico and his modern imitators, in order to soften earthly shadows in the representation of sacred objects. Like the Dutch school, he may represent the varying light of the atmosphere, now bright and sunny, and now pale, or warm and cold, and thereby evoke in the observer moods which depend on the illumination and on the state of the weather; or by means of undisturbed air he may cause his figures to stand out objectively clear as it were, and uninfluenced by subjective impressions. By this means, great variety is attained in what artists call 8 style ' or ' treatment,' and indeed in their purely pic- torial elements. 1 24 ON THE RELATION OF OPTICS TO PAINTING. IV. HARMONY OF COLOUR. We here naturally raise the question : If, owing to the small quantity of light and saturation of his colours, the artist seeks, in all kinds of indirect ways, by imi- tating subjective impressions to attain resemblance to nature, as close as possible, but still imperfect, would it not be more convenient to seek for means of obvi- ating these evils ? Such there are indeed. Frescoes are sometimes viewed in direct sunlight ; transparen- cies and paintings on glass cau utilise far higher degrees of brightness, and far more saturated colours ; in dioramas and in theatrical decorations we may employ powerful artificial light, and, if need be, the electric light. But when I enumerate these branches of art, it will at once strike you that those works which we admire as the greatest masterpieces of painting, do not belong to this class ; but by far the larger number of the great works of art are executed with the comparatively dull water or oil-colours, or at any rate for rooms with softened light. If higher ariistic effects could be attained with colours lighted by the sun, we should undoubtedly have pic- tures which took advantage of this. Fresco painting ON THE KELATION OF OPTICS TO PAINTING. 125 frould have led to this ; or the experiments of Munich's celebrated optician Steinheil, which he made as a matter of science, that is, to produce oil paintings which should be looked at in bright sunshine, would not be isolated. Experiment seems therefore to teach, that modera- tion of light and of colours in pictures is ever advan- tageous, and we need only look at frescoes in direct sunlight, such as those of the new Pinakothek in Miinich, to learn in what this advantage consists. Their brightness is so great that we cannot look at them steadily for any length of time. And what in this case is so painful and so tiring to the eye, would also operate in a smaller degree if, in a picture, bril- liant colours were used, even locally and to a moderate extent, which were intended to represent bright sun- light, and a mass of light shed over the picture. It is much easier to produce an accurate imitation of the feeble light of moonshine with artificial light in dioramas and theatre decorations. We may therefore designate truth to Nature of a beautiful picture as an ennobled fidelity to Nature. Such a picture reproduces all that is essential in the impression, and attains full vividness of conception, but without injury or tiring the eye by the nude lights of reality. The differences between Art and Nature are chiefly confined, as we have already seen, to those 126 ON THE RELATION OF OPTICS TO PAINTING. matters which we can in reality only estimate in an un- certain manner, such as the absolute intensities of light. That which is pleasant to the senses, the beneficial bat not exhausting fatigue of our nerves, the feeling of comfort, corresponds in this case, as in others, to those conditions which are most favourable for per- ceiving the outer world, and which admit of the finest discrimination and observation. It has been mentioned above that the discrimina- tion of the finest shadows, and of the modelling which they express, is the most delicate under a certain mean brightness. I should like to direct your atten- tion to another point which has great importance in painting: I refer to our natural delight in colours, which has undoubtedly a great influence upon our pleasure in the works of the painter. In its simplest expression, as pleasure in gaudy flowers, feathers, stones, in fireworks, and Bengal lights, this inclination has but little to do with man's sense of art ; it only ap- pears as the natural pleasure of the perceptive organism in the varying and multifarious excitation of its various nerves, which is necessary for its healthy continuance and productivity. But the thorough fitness in the con- struction of living organisms, whatever their origin, excludes the possibility that in the majority of healthy individuals an instinct should be developed or main- tain itself which did not serve some definite purpose. ON THE RELATION OF OPTICS TO PAINTING. 127 We have not far to ""seek for the delight in light and in colours, and for the dread of darkness; this coincides with the endeavour to see and to recognise surrounding objects. Darkness owes the greater part of the terror which it inspires to the fright of what is unknown and cannot be recognised. A coloured picture gives a far more accurate, richer, and easier conception than a similarly executed drawing, which only retains the contrasts of light and shade. A picture retains the latter, but has in addition the material for discrimination which colours afford; by which surfaces which appear equally bright in the drawing, owing to their different colour, are now assigned to various objects, or again as alike in colour are seen to be parts of the same, or of similar objects. In utilising the relations thus naturally given, the artist, by means of prominent colours, can direct and enchain the attention of the observer upon the chief objects of the picture; and by the variety of the garments he can discriminate the figures from each other, but complete each individual one in itself. Even the natural pleasure in pure, strongly saturated colours, finds its justification in this direction. The case is analogous to that in music, with the full, pure, well-sounding tones of a beautiful voice. Such a one is more expressive ; that is, even the smallest change of its pitch, or its quality — any slight interruption, 158 ON THE KELATION OF OPTICS TO PAINTING. any tremulousness, any rising or falling in it — is at once more distinctly recognised by the hearer than could be the case with a less regular sound ; and it seems also that the powerful excitation which it pro- duces in the ear of the listener, arouses trains of ideas and passions more strongly than does a feebler excita- tion of the same kind. A pure, fundamental colour bears to small admixtures the same relation as a dark ground on which the slightest shade of light is visible. Any of the ladies present will have known how sensi- tive clothes of uniform saturated shades are to dirt, in comparison with grey or greyish-brown materials. This also corresponds to the conclusions from Young's theory of colours. According to this theory, the per- ception of each of the three fundamental colours arises from the excitation of only one kind of sensitive fibres, while the two others are at rest ; or at any rate are but feebly excited. A brilliant, pure colour pro- duces a powerful stimulus, and yet, at the same time, a great degree of sensitiveness to the admixture of other colours, in those systems of nerve-fibres which are at rest. The modelling of a coloured surface mainly depends upon the reflection of light of other colours which falls upon them from without. It is more particularly when the material glistens that the reflections of the bright places are preferably of the colour of the incident light. In the depth of the ON THE RELATION OF OPTICS TO PAINTING. 129 f3lds, on the contrary, 4he coloured surface reflects against itself, and thereby makes its own colour more saturated. A white surface, on the contrary, of great brightness, produces a dazzling effect, and is thereby insensitive to slight degrees of shade. Strong colours thus, by the powerful irritation which tt ?y produce, can enchain the eye of the observer, and yet be ex- pressive for the slightest change of modelling or of illumination ; that is, they are expressive in the artistic sense. If, on the other hand, we coat too large surfaces, they produce fatigue for the prominent colour, and a diminution in sensitiveness towards it. This colour then becomes more grey, and on all surfaces of a different colour the complementary tint appears, espe- cially on grey or black surfaces. Hence therefore clothes, and more particularly curtains, which are of too bright a single colour, produce an unsatisfactory and fatiguing effect ; the clothes have moreover the disadvantage for the wearer that they cover face and hands with the complementary colour. Blue produces yellow, violet gives greenish yellow, bright purple gives green, scarlet gives blue, and, conversely, yellow gives -blue, etc. There is another circumstance which the artist has to consider, that colour is for him an important means of attracting the attention of the observer. To be able to do this he must be sparing in U. K 130 ON THE RELATION OF OPTICS TO PAINTING. the use of the pure colours, otherwise they distract the attention, and the picture becomes glaring. It is necessary, on the other hand, to avoid a onesided fatigue of the eye by too prominent a colour. This is effected either by introducing the prominent colour to a moderate extent upon a dull, slightly coloured ground, or by the juxtaposition of variously saturated colours, which produce a certain equilibrium of irrita- tion in the eye, and, by the contrast in their after- images, strengthen and increase each other. A green surface on which the green after-image of a purple one falls, appears to be a far purer green than without such an after-image. By fatigue towards purple, that is towards red and violet, any admixture of these two colours in the green is enfeebled, while this itself pro- duces its full effect. In this way the sensation of A green is purified from any foreign admixture. Even the purest and most saturated green, which Nature shows in the prismatic spectrum, may thus acquire a higher degree of saturation. We find thus that the other pairs of complementary colours, which we have mentioned, make each other more brilliant by their contrast, while colours which are very similar aro detrimental to each other, and acquire a grey tint. These relations of the colours to each other have manifestly a great influence on the degree of pleasure which different combinations of colours afford. Two ON THE RELATION OF OPTICS TO PAINTING. 131 colours may, without injury, be juxtaposed, which indeed are so similar as to look like varieties of the same colour, produced by varying degrees of light and shade. Thus, upon scarlet the more shaded parts ap- pear of a carmine, or on a straw-colour they appear of a golden yellow. If we pass beyond these limits, we arrive at un- pleasant combinations, such as carmine and orange, or orange and straw-yellow. The distance of the colours must then be increased, so as to create pleasing com- binations once more. The complementary colours are those which are most distant from each other. When these are combined, such, for instance, as straw-colour and ultramarine, or verdigris and purple, they have something insipid but crude ; perhaps because we are prepared to expect the second colour to appear as an after-image of the first, and it does not sufficiently appear to be a new and independent element in the compound. Hence, on the whole, combinations of those pairs are most pleasing in which the second colour of the complementary tint is near the first, though with a distinct difference. Thus, scarlet and greenish blue are complementary. The combination produced when the greenish blue is allowed to glide either into ultramarine, or yellowish green (sap green), is still more pleasing. In the latter case, the com- bination tends towards yellow, and in the former, K 2 132 ON THE RELATION OF OPTICS TO PAINTING. towards rose-red. Still more satisfactory combinations are those of three tints which bring about equilibrium in the impression of colour, and, notwithstanding the great body of colour, avoid a onesided fatigue of the eye, without falling into the baldness of complemen- tary tints. To this belongs the combination which the Venetian masters used so much — red, green, and violet; as well as Paul Veronese's purple, greenish blue, and yellow. The former triad corresponds ap- proximately to the three fundamental colours, in so far as these can be produced by pigments ; the latter gives the mixtures of each pair of fundamental colours. It is however to be observed, that it has not yet been possible to establish rules for the harmony of colours with the same precision and certainty as for the con- sonance of tones. On the contrary, a consideration of the facts shows that a number of accessory influences come into play,1 when once the coloured surface is also to produce, either wholly or in part, a representa- tion of natural objects or of solid forms, or even if it only offers a resemblance with the representation of a relief, of shaded and of non-shaded surfaces. It is moreover often difficult to establish, as a matter of fact, what are the colours which produce the harmonic impression. This is pre-eminently the case with 1 Conf. E. Briicke, Die Physiologic der Farben fur die Zn-ecke dcr Kunstg 'ewerbe. Leipzig, 1866. W. v. Bezold, Die Farbenlehre, tin Hinblick auf Kunst und Kuiistgerverbe. Braunschweig, 1874. ON THE RELATION OF OPTICS TO PAINTING. 133 pictures in which the ^aerial colour, the coloured re- flection and shade, so variously alter the tint of each single coloured surface when it is not perfectly smooth, that it is hardly possible to give an indisputable de- termination of its tint. In such cases, moreover, the direct action of the colour upon the eye is only a subordinate means; for, on the other hand, the prominent colours and lights must also serve for directing the attention to the more important points of the representation. Compared with these more poetical and psychological elements of the representa- tion, considerations as to the pleasing effect of the colours are thrown into the background. Only in the pure ornamentation on carpets, draperies, ribbons, or architectonic surfaces is there free scope for pure pleasure in the colours, and only there can it develop itself according to its own laws. In pictures, too, there is not, as a general rule, perfect equilibrium between the various colours, but one of them preponderates to an extent which corre- sponds to the dominant light. This is occasioned, in the first case, by the truthful imitation of physical circumstances. If the illumination is rich in yellow light, yellow colours will appear brighter and more brilliant than blue ones ; for yellow bodies are those which preferably reflect yellow light ; while that of blue is only feebly reflected, and is mainly absorbed. 134 ON THE RELATION OF OPTICS TO PAINTING. Before the shaded parts of blue bodies, the yellow aerial light produces its effect, and imparts to the blue more or less of a grey tint. The same thing happens in front of red and green, though to a less extent, so that, in their shadows, these colours merge into yellow. This also is closely in accordance with the aesthetic requirements of artistic unity of compo- sition in colour. This is caused by the fact that the divergent colours show a relation to the predominant colour, and point to it most distinctly in their shades. Where this is wanting, the various colours are hard and crude ; and, since each one calls attention to itself, they make a motley and disturbing impression ; and, on the other hand, a cold one, for the appearance of a flood of light thrown over the objects is wanting. We have a natural type of the harmony which a well-executed illumination of masses of air can produce in a picture, in the light of the setting sun, which throws over the poorest regions a flood of light and colour, and harmoniously brightens them. The natural reason for this increase of aerial illumination lies in the fact, that the lower and more opaque layers of air are in the direction of the sun, and therefore reflect more powerfully; while at the same time the yellowish red colour of the light which has passed through the atmosphere becomes more dis- ON THE RELATION OF OPTICS TO PAINTING. 135 tinct as the length of path increases which it has to traverse, and that further, this coloration is more pronounced as the background falls into shadow. In summing up once more these considerations, we have first seen what limitations are imposed on truth to Nature in artistic representation ; how the painter links the principal means which nature furnishes of recognising depths in the field of view, namely binocu- lar vision, which indeed is even turned against him, as it shows unmistakably the flatness of the picture ; how therefore the painter must carefully select, partly the perspective arrangement of his subject, its posi- tion and its aspect, and partly the lighting and shading, in order to give us a directly intelligible image of its magnitude, its shape, and distance, and how a truthful representation of aerial light is one of the most important means of attaining the object. We then saw that even the scale of luminous intensity, as met with in the objects, must be trans- formed in the picture to one differing sometimes by a hundredfold; how here, the colour of the object cannot be simply represented by the pigment; that indeed it is necessary to introduce important changes in the distribution of light and dark, of yellowish and of bluish tints. The artist cannot transcribe Nature; he must 136 ON THE KELATION OF OPTICS TO PAIXTING. translate her; yet this translation may give us an impression in the highest degree distinct and forcible, not merely of the objects themselves, but even of the greatly altered intensities of light under which we view them. The altered scale is indeed in many cases advantageous, as it gets rid of everything which, in the actual objects, is too dazzling, and too fatiguing for the eye. Thus the imitation of Nature in the picture is at the same time an ennobling of the im- pression on the senses. In this respect we can often give ourselves up more calmly and continuously, to the consideration of a work of art, than to that of a real object. The work of art can produce those gradations of light, and those tints in which the modelling of the forms is most distinct and therefore most expressive. It can bring forward a fulness of vivid fervent colours, and by skilful contrast can retain the sensitiveness of the eye in advantageous equilibrium. It can fearlessly apply the entire energy of powerful sensuous impres- sions, and the feeling of delight associated therewith, to direct and enchain the attention ; it can use their variety to heighten the direct understanding of what is represented, and yet keep the eye in a condition of excitation most favourable and agreeable for delicate sensuous impressions. If, in these considerations, my having continually laid much weight on the lightest, finest, and most ON TEE RLLATION OF OPTICS TO PAINTING. 137 accurate sensuous intelligibility of artistic representa- tion, may seem to many of you as a very subordinate point — a point which, if mentioned at all by writers on aesthetics, is treated as quite accessory — I think this is unjustly so. The sensuous distinctness is by no means a low or subordinate element in the action of works of art ; its importance has forced itself the more strongly upon me the more I have sought to discover the physiological elements in their action. What effect is to be produced by a work of art, using this word in its highest sense ? It should excite and enchain our attention, arouse in us, in easy play, a host of slumbering conceptions and their cor- responding feelings, and direct them towards a common object, so as to give a vivid perception of all the fea- tures of an ideal type, whose separate fragments lie scattered in our imagination and overgrown by the wild chaos of accident. It seems as if we can only refer the frequent preponderance, in the mind, of art over reality, to the fact that the latter mixes some- thing foreign, disturbing, and even injurious ; while art can collect all the elements for the desired impression, and allow them to act without restraint. The power of this impression will no doubt be greater the deeper, the finer, and the truer to nature is the sensuous impression which is to arouse the series of images and the effects connected therewith. It must act cer- 138 ON THE KELATION OF OPTICS TO PAINTING. tainly, rapidly, unequivocably, and with accuracy if it is to produce a vivid and powerful impression. These essentially are the points which I have sought to com- prehend under the name of intelligibility of the work of art. Then the peculiarities of the painters' technique (Technik), to which physiological optical investigation have led us, are often closely connected with the highest problems of art. We may perhaps think that even the last secret of artistic beauty — that is, the wondrous pleasure which we feel in its presence — is essentially based on the feeling of an easy, harmonic, vivid stream of our conceptions, which, in spite of manifold changes, flow towards a common object, bring to light laws hitherto concealed, and allow us to gaze in the deepest depths of sensation of our own nrindg. 139 ON THE OEIGIN OF TIIB PLANETABY SYSTEM. Lecture delivered in Heidelberg and in Cologne, in 1871. IT is my intention to bring a subject before you to-day which has been much discussed — that is, the hypothesis of Kant and Laplace as to the formation of the celestial bodies, and more especially of our planetary system. The choice of the subject needs no apology. In popular lectures, like the present, the hearers may reasonably expect from the lecturer, that he shall bring before them well-ascertained facts, and the complete results of investigation, and not unripe suppositions, hypothe- ses, or dreams. Of all the subjects to which the thought and im- agination of man could turn, the question as to the origin of the world has, since remote antiquity, been the favourite arena of the wildest speculation. Bene- 140