i. Purulent Otitis Media, caused by the Nasal Douche, and accompanied by Double Hearing. ii. The Influence of Spectacles on the Optical Constants and Visual Acuteness of the Eye. Large Cyst of tlie Iris, cured by Operation. ii IV. A case of Extirpation of a Cancroid Growth of the Inner Canthus and Upper Eyelid. Blepharoplasty by Sliding Flaps; By Prof. II. KNAPP, M.B., Surgeon in Chief to the JVeiv York Ophthalmic and Aural Institute. Reprinted from the Archives of Ophthalmology and Otology, I., 2, 1870. ’■ JIew York : WILLIAM WOOD & COMPANY, 61 Walk: k . i k"et. 187c. PURULENT OTITIS MEDIA, CAUSED BY THE NASAL DOUCHE, AND ACCOMPANIED BY DOUBLE HEAIRNG. H. KNAPP. The use of Weber’s nasal douche for diseases of the naso-pharyngeal region has of late become very exten- sive. Some recent publications, however, show that it is not without serious danger. Dr. D. B. St. John Boosa describes in the first number of these Archives (p. 259, etc.) a case in which the origin of a purulent inflamma- tion of the middle ear, of the very severest kind, could be traced to the use of the nasal douche. He adds that he had observed other cases in which the nasal douche was followed by bad symptoms, and that it hardly ever could be tolerated for any length of time. S. Moos, in a note to the German translation of Roosa’s communica- tion, confirms these views by stating that he saw the fluid which had been injected into the nostril by Weber’s douche, flow out of the ears in two cases of perforation of the drum-head. Although the application of the douche is not hurtful in such cases, they prove that 2 water thus introduced into the posterior nasal space may penetrate through the Eustachian tubes into the tym- panic cavity. Moos, too, saw a case in which an acute aural catarrh was brought about by the nasal douche. The practical importance of these observations induces me to communicate a case of a similar kind :— A merchant of New York, 32 years of age, was in the habit of in- jecting, by Weber’s douche, warm water into his nose for chronic catarrh. He once took cold water, and felt, immediately after the in- jection, considerable pain in both ears, disappearing, however, very soon. Since that time he used warm water for six months without any unpleasant symptoms. Then he employed cold water once again, and experienced instantly in his left ear a severe pain, which soon abated, but nevertheless continued dull and annoying for a fortnight. Then suddenly it increased very much, was combined with headache, throbbing in the ear, loss of appetite, and deafness. Three days later an abundant purulent discharge from the left ear set in. He came to my office presenting all the symptoms of a very severe otitis media, with perforation of the membrana tympani. He remained under my treatment from March 6th to April 11th. Three weeks after his first call a great improvement had been obtained, the discharge was stopped, and the perforation in the drum-head closed for four days. Then an exacerbation and a new perforation occurred. The discharge kept flowing for a fortnight, when again an improvement was obtained, and the patient left New York to complete his recovery under the care of his father, a physician in the neighborhood of Philadelphia. There is no doubt that the purulent inflammation of the middle ear was caused by the flowing of cold water into the tympanic cavity. Whether warm water some- times or usually passed into the drum during the use of Weber’s douche cannot be ascertained, since the patient 3 never felt it. I am satisfied that water can penetrate into the drum only when the patient accidentally swallows during the time the current is running over the orifices of the Eustachian tubes. It is easily explainable that cold water is more apt to provoke involuntary swallow- ing than warm. Moreover, the latter, when passing into the tympanum, would probably not cause much reaction or bad consequences. It therefore is certainly less ob- jectionable than the use of cold water in cleansing the na- sal and upper pharyngeal region. Since the observation above related, and the communications of Poosa and Moos, I have not recommended any more the use of the na- sal douche, but applied injections of astringent remedies by the posterior nares syringe. They are disagreeable for a great many patients, producing very unpleasant fits of sneezing and coughing, but their action is efficient, and, as it seems, devoid of danger. If we inject only small quantities of fluid, which is mostly sufficient, there is commonly no unpleasant reaction. Besides its origin, the above case was very remarkable for a symptom not much noticed yet, viz., double hearing with loth ears. Troltsch and Politzer mention its occur- rence only with two lines; Moos records in his “ Klinik der Olirenkrankheiten,” p. 319, etc., what is known on it. There are three incomplete observations in older litera- ture, to which are added two of Moos himself, and one of Von Wittich. The first of Moos’ patients, suffering from acute aural catarrh, heard simultaneously the third of each tone he was singing. The catarrh and double 4 hearing disappeared both together very soon. The second patient had impairment of hearing from chronic aural catarrh for ten years. One evening, to shorten a fit of his habitual asthma, he anaesthetized himself by chloroform. On awaking his deafness was very much worse, and he heard all the sounds of the upper three octaves of a piano double. During the course of some months his hearing power diminished still further, the double hearing continued for some time, and ultimately all musical sounds appeared to him so perverse that music in general, which he had been very fond of before, became a perfect horror to him. In none of these two cases mention is made which ear perceived rightly the natural tone, nor whether the pseudo-tone was higher or lower in pitch. The only well-analyzed case of the few cases of double hearing which are on record up to this day, is the observation made by Prof. Von Wittich on himself. The excellent physiologist of Koenigsberg no- ticed, four weeks after an acute purulent otitis media, that he heard all the tones of the middle octave of a jpiano half a note higher with the diseased ear than with the healthy one. His explanation is, that an exudation into the tympanic cavity, by altering the pressure of the fluid in the labyrinth, had changed the tuning of the terminal fibres of the auditory nerve. When I examined the patient whose history I have sketched above, three days after the discharge had set in, I found in the diseased ear the hearing power for noises very much diminished (a watch of 6' hearing 5 distance was heard from £"), whilst musical sounds were nearly as sharply perceived as in the normal state. A large tuning-fork, placed on the glabella, was heard double, and in the affected ear more strongly and about tivo tones higher than in the sound ear. On trial with a piano I found out that the same anomaly existed for the tones of the middle and next higher octaves, but not for the deeper ones. It was not distinctly marked at which note of the musical scale the double hearing be- gan, nor where it terminated. This anomaly existed unchanged during the first week, as long as the perfora- tion of the membrana tympani was large and the dis- charge abundant. Then the double sounds gradually came nearer to each other in pitch, until, at the end of three weeks, they hardly differed by half a tone, and sometimes were heard separately only by strained attention. After the relapse the double hearing was again a little better perceived, but the two tones never differed so much as in the beginning; moreover, their difference in pitch was changing from day to day. I have not heard of the patient since he left New York. This observation has many features in common with that of Von Wittich, above all, the origin of the anomaly in an acute purulent otitis media. The principal dif- ferences of both cases are the following: 1st. The pseudo-tone (that of the diseased ear) was higher in Wittich’s, lower in mine, than the right tone. 2d. The difference of pitch between real and pseudo-tone was greater in my case than in Wittich’s. 3d. The differ- 6 ence of pitch between both tones was changing in my case, but constant in that of Von Wittich. I shall try to account for these differences, together with giving an explanation of the whole anomaly. The latter is most appropriately termed diplacusis binauri- cularis, in analogy with a similar anomaly of the organ of sight, viz., diplopia binocularis. Helmholtz1 s theory is perfectly adapted to explain binauricular diplacusis. In conformity with this theory we may compare the cochlear portion of the inner ear with a stringed instru- ment. Corti’s arcs or fibres—the strings—are so tuned as to yield all the sounds of the musical scale. Both cochleae represent two instruments in perfect accord. If a sound is produced in the air, the vibrations of the latter will be transmitted through both membranae tympani and the chain of the ossicles to those strings of Corti’s organ which are tuned for this sound, and thus sympa- thetic vibrations are occasioned in Corti’s fibres, and con- veyed to the brain by the filaments of the auditory nerve connected with the vibrating fibres of Corti’s organ. The same external sound will excite in either cochlea corresponding (identical) acoustic nerve fibres by producing sympathetic vibrations in corresponding (identical) arcs of Corti’s organ. In analogy with simi- lar conditions of both retinae, those fibres of both cochleae may be called corresponding or identical, the simultane- ous and equivalent excitement of ivhich generates but one sensation of sound. This constitutes the anatomical and physiological foundation of single hearing with both 7 ears, in a similar manner as we see single with both eyes. Now, suppose the strings of one instrument (Corti’s organ) are tighter drawn, then this instrument will be differently, that is, higher tuned, so that a string which formerly made f. i. 300 vibrations per second now makes 350 per second. Say 300 vibrations per second cor- respond to the tone c, 350 to the tone e. If, now, the latter tone, e, is sounded at any musical instrument, it will excite sympathetic movements in all strings so tuned as to perform 350 vibrations per second. (I may disregard entirely the harmonics.) In the healthy ear this will be Corti’s fibre corresponding to the sound e, but in the diseased ear 350 vibrations are now performed by a fibre which formerly performed only 300 per second, and which, of course, is still connected with that auditory nerve-fibre Avhich always committed the impression of 300 vibrations, that is, the tone c, to the brain. There- fore this ear will engender the perception of the lower sound c, whilst at the same time the other one will en- gender the perception of the higher sound e. Such were about the conditions in the case of double hearing observed by me. The opposite state must have been present in Von Wittich’s case. He heard with the diseased ear the tone higher than with the healthy one. Suppose he heard with the latter the sound c (300 vibrations per second), and with the diseased the sound d (say 325 vibrations per second), then Corti’s fibre, tuned in the healthy state 8 to 325 vibrations, must have been so much relaxed that it now made only 300 per second. An external sound, c, of 300 vibrations per second, will induce sympathetic vibrations in that of Corti’s arc of either ear which is tuned to 300 vibrations. In the healthy ear the right sound o is perceived, but in the diseased ear the relaxed arc will continue to excite the auditory fibre which always conducted the impression of 325 vibrations per second, that is, of the sound d, to the brain. Von Wit- tich made a very ingenious experiment to confirm this theory. If two tuning-forks, differing in pitch by half a tone, were so put before the ears that the lower one was before the diseased, the higher before the healthy ear, only one sound was perceived. The tuning-fork which yielded a lower sound produced sympathetic undulations in the relaxed Corti’s arc which formerly was tuned half a tone higher, and now the nerve connected with it is excited with its corresponding nerve in the other cochlea. Thus it is evident that diplacusis binauricularis may be of two kinds, by false higher tuning, tightening, and by false lower tuning, relaxing, of Corti’s organ. In the latter the pseudo-tone will be higher, in the former it will be lower, than the right tone. Ihe greater the difference in pitch, the greater will be the degree of false tuning, either by increased tension or by relaxation of Cortis organ. This principle explains the second and third points of difference between my case and that of Von Wittich.. There was, at the begin- ning of my observation, a morbid action on the cochlea 9 about four times as intense as in Yon Wittich’s case. This morbid action, however, was not constant during the course of my observation, but decreased in propor- tion with the decreasing intensity of the inflammation. It was scarcely yet perceptible when the discharge had stopped and the perforation of the drum-head was closed. In a case of Dr. Gumpert (see Moos, 1. c., p. 319) the difference of pitch of both sounds varied between a third, fourth, and octave during one week, and then disappeared entirely. Of what nature the changes are which produce false tuning of Corti’s organ, I am not at all prepared to answer. Yon Wittich assumes that exudation into the tympanic cavity changes the pressure of the fluid in the labyrinth. In his case the membrana tympani seems to have been entire at the time when diplacusis was noticed, for he adds that neither filling of the auditory canal with water, nor inflation of the tympanum with air, pro- duced any alteration in the double hearing. In my case diplacusis of opposite kind existed, with perforation of the membrana tympani. Is the integrity of the mem- brana tympani essential in relaxing Corti’s organ ? Does its perforation produce tightening of it ? I am unable to answer these questions. The first of Moos’ cases, acute aural catarrh, seems to be analogous with Wittich’s observation. “The patient heard simultaneously the third of every tone.” If here, what is not stated, but seems to be understood, the third was the pseudo-tone, then there existed, like in Wittich’s observation, dipla- 10 cusis by relaxation of Corti’s organ. The drum-head was not ruptured. The other observation of Moos, where diplacusis was occasioned by anaesthetizing with chloroform in a case of chronic aural catarrh, seems to be an example of idio- pathic false tuning of Corti’s organ, that is, not dependent on inflammatory changes in the middle ear. I think that, for the present, it is of greater importance to collect more facts relative to this anomaly than to seek for a theory. The symptom of double hearing, when further studied, may be not only of physiological significance, but assume practical importance. It may guide our prognosis and treatment, by demonstrating that in the respective cases the labyrinth is either primarily affected or participates in some other disease. I suppose also that diplacusis binauricularis will be more frequently noticed than has been the case hitherto, if our attention be directed to it. With regard to future investigations, I propose that our inquiries should try to solve the following questions :— 1. How great is the difference of pitch between the two sounds ? 2. Has the pseudo-tone the same intensity and clang- tint (timbre) as the right tone (that of the healthy ear) \ 3. Are these differences constant or varying during the duration of the anomaly ? 4. Is the pseudo-tone higher or lower than the right tone (diplacusis by relaxation or tension of Corti’s fibres) ? 11 5. Is it possible to obtain single bearing by producing tones of different pitch before either ear ? The tuning- fork placed before the diseased ear ought to differ so much in pitch from the tuning-fork placed before the healthy ear as the pseudo-tone differs from the right tone, but the difference in pitch must be of opposite direction, f. i., if the pseudo-tone is half a tone higher than the right tone, then the tuning-fork placed before the diseased ear must be half a tone lower than that be- fore the healthy ear. If the pseudo-tone is lower than the right tone, then the tuning-fork before the diseased ear must be so much lower. 6. At which heights of the musical scale does double hearing begin and terminate, that is, how great is the range of double hearing t 7. Are the limits, on the musical scale, between single and double hearing distinct or fading away gradually f 8. If the entire Corti’s organ of one ear be differently tuned from that of the other ear, compound tones and pure chords must appear dissonant in binauricular, but consonant in monauricular hearing, also when in the latter case the healthy ear is excluded from the act of hearing. But if only a part of Corti’s organ of one ear be differ- ently tuned from the corresponding part of the other ear, all compound tones and the purest chords must ap- pear dissonant in monauricular as well as in binauricular audition. All music must be a horrible dissonance, as in the one of Mood cases. The examination has to de- termine of what hind these dissonances in monauricular 12 and binauricular audition are, which will he possible by analyzing the anomaly according to Helmholtz’s theory. 9. What is the cause of diplacusis t Is the latter de- pendent on a primary lesion of the labyrinth, or conse- quent to morbid processes in the middle ear ? In what state is the membrana tympani ? Is there any change in intra-auricular pressure ? A complete investigation of this kind may, at first, be fraught with difficulties, and perhaps deemed result- less ; but let me remind the reader that diplopia, not long ago, was an abstruse subject too, which has now become most valuable with regard to diagnosis, prognosis, and treatment of a large group of eye-diseases. 13 THE INFLUENCE OF SPECTACLES ON THE OPTICAL CON- STANTS AND VISUAL ACUTENESS OF THE EYE. H. KNAPP. (a.) influence of spectacles on the ordinary eye. Every oculist at the present day is fully convinced that an accurate determination of the acuteness of vision (S) is of the greatest importance in the practice of ophthal- mology. The older methods are now all given up in favor of ascertaining S by a rational system of test-types. In cases of anomalous refraction, S is found out by means of convex or concave glasses neutralizing the anomaly of refraction. That, in doing so, a certain de- gree of inaccuracy is introduced by disregarding the magnifying and diminishing influence of these glasses is evident, but the amount of this inaccuracy has not yet been calculated. Even Donders, in his very ex- haustive treatise on the Anomalies of Accommodation and Refraction, does not touch this question. He says (p. 152) that, without further determination, a com- parison of tiie visual axgles can only be made if the 14 visual object can be accurately seen with or without auxiliary glasses. I purpose now to examine what influence on the visual acuteness these auxiliary glasses exert in ametropic eyes. It is known that ametropia is caused not by any nota- ble changes in the refracting media and their surfaces of separation, but by changes of position of the retina. Therefore we may assume that the optical constants of ametropic eyes are equal to those of emmetropic ones. I shall take as a basis for the calculation the values of listing's diagranmiatic eye given in most text-books, for instance, Helmholtz1 s Physiological Optics, p. Ill, and IJonders' Accom. and Refraction, p. 67. (In the latter there is a misprint: line 7 from the bottom of the page, anterior focal distance of the eye ought to be 14,858 instead of 19,875.) To solve the problem in a general way, I shall calcu- late the optical constants of a compound dioptrical system, consisting of the normal (or diagrammatical) eye combined with the series of our common spectacle- glasses. This work has not yet been done, and may also prove useful in solving other questions relating to vision through lenses. In the calculations I shall avail myself of the conveni- ent formulas given in Helmholtz's “Physiologische Optih." The usual distance at which spectacles are worn before the eye is about half a Paris inch. We may, therefore, place the auxiliary lens 14,858 mm. in front of the first principal plane of the eye. It is sufficiently accurate for 15 oui' present purpose to disregard the thickness of the glass lens, its two principal and focal points falling together and coinciding with the so-called optical centre. By placing the glass 14,858 mm. before the first princi- pal plane of the eye, the optical centre of the first system coincides with the first focal point of the second system, the anterior focal length of the latter being 14,858 mm. These suppositions made, we can proceed to determine the position of the cardinal points of the compound sys- tem. f and f denote the first and second focal lengths* of the first system, which, being equal, may indiscriminately be represented byf 2, the second focal length of the eye. If we place a negative lens (—10") before the eye, the second principal point is likewise obtained by formula lie, with the difference only that f2 being negative in this case, renders the value of h2 positive, namely— d (po = a - $>, + f, = i.0909™™- This shows that with negative glasses of the same focal length the second principal point recedes by the same quantity as it advances with positive glasses. The second focal length of the compound system is, 19 therefore, obtained for concave glasses by subtracting this quantity from the value above found for a2 r2, which expresses the distance between the second focal point of the compound system from the second principal point of the eye. Therefore, F2 = 20,966 - 1,0909. F2 = 19,875 mm. = $2. Thus we have found that the second focal length, F.z, of the compound system proves equal to the second focal length of the naked eye, whether for convex or for concave glasses. The position of the nodal points is now easily ascer- tained, as, in every system, the distance of the first nodal from the first focal point is equal to the second focal length. All these quantities of the compound system having been found identical with the corresponding quan- tities of the naked eye, the first nodal point of the com- pound system must also coincide with the first nodal point of the eye. The equality of the posterior focal length of the com- pound system with that of the eye, has been obtained only by numerical calculation of one example, and from it the position of the first nodal point has been deduced. As this may not be considered sufficient evidence, I shall demonstrate it in a general way. Formula 11<^, i - d fi ‘“d-fc-tf determines the position of the first principal point by the 20 distance (d) of tlie glass lens from tlie anterior principal point, moreover by the anterior focal length of the eye, and the focal length of the glass (b = f2). The position of the focal points of a compound dioptrical sys- tem may be determined independently from the principal points, by proceeding from the nodal points of the single systems in a similar way as by making use of the princi- pal points. If d! signifies the distance between the second nodal point of the first system and the first nodal point of the second system, <£>2 the second focal length of the second system, and b and f2 the anterior and posterior focal lengths of the first system, the formula is trans- formed into the following: f X — —il 1 - d'-ft-fi in which Kj represents the situation of the anterior nodal point of the compound system in front of the an- terior nodal point of the first system, d' = 1. It is, therefore, evident that by wearing convex glasses the optical power of the eye increases, even if we leave out 27 of consideration tlie correction of tlie impurity of the retinal images. o • Suppose somebody is able to see at distance distinctly without and with convex glasses (facultative hyperopia, Bonders), then his eye, when unaided, would form the perfectly pure image luf, and, when armed with a con- vex glass, the image hi quite as distinctly, but larger, of the same object. Therefore the eye, when armed with convex glasses, would be able to read smaller type than Sn. xx. at 20' distance, that is, his visual acuteness would be greater than normal, according to our usual method of testing. Both nodal points advance in every eye by accommoda- tion. By A = d this advancement amounts to 0,4 to 0,5 mm., causing an adequate aggrandizement of the retinal images equivalent to that produced by convex spec- tacles No. 24, as the table further below demonstrates. In this way we are able to compare the aggrandizement of the image caused by accommodation in the unarmed hyperopic eye, with the aggrandizement of the image caused by convex glasses in the hyperopic eye. To de- termine how much the magnifying effect of convex glasses exceeds that produced by accommodation, we take the former in the table further below, and deduct from it the aggrandizement produced by accommodation. If, f. i., a patient with hyperopia = wishes to see clearly at distance wdthout glasses, he must make an accommo- dative effort of A- But this is only the third part of A = b; the aggrandizement by accommodation, therefore, 28 is only one-third of that produced by a convex glass No. 24, or equivalent to that of + 72. We shall, here- after, see that the magnifying effect of glasses weaker than No. 10 may fairly be neglected for practical pur- poses ; so much the more may we disregard the influence of accommodation on the size of the retinal images. Apart from that, it is the object of the present investiga- tion to evaluate the changes of size brought about by spectacles in the retinal images, making abstraction of the optical purity of the latter. In that way only we obtain a correct measure to compare the visual acuteness of armed ametropic eyes with that of the unarmed emmetropic eye; for spectacles re-establish the purity of the retinal images, and render accommodation equal to that of the emmetropic eye ; but in doing so they more- over exert some influence on the size of the retinal image, and it is the amount and consequences of this accessory factor we are endeavoring here to ascertain. The fore- going lines, however, solve the problem raised by Don- ders, and quoted at the beginning of this paper, that a comparison of the visual angles can only be made, if the visual object can be accurately seen with or without auxiliary glasses. Instead of visual angles we would now say the size of the retinal images. The conditions of myopic eyes are easier to analyze. The retina, mgm, Figs. 1 and 2, being distended, displays a less density of its percipient elements. The line mgm may be supposed, as I have shown, to contain no more percipient elements than eg6 or hgh in the emmetropic 29 and hyperopic eyes. If, now, mgm (Fig. 2) is the small- est perceptible retinal image of an unaided myopic eye, the addition of a concave glass would reduce this image of the same object to the size of mn, by shifting the second nodal point from backward to h™. The di- mension mn being less than the distance of two adjoin- ing percipient elements, or less than the smallest per- ceptible retinal image, the addition of a concave glass has rendered visual acuteness less than normal. The amount of increase or diminution of visual acuteness brought about by spectacles is proportionate to the increase or diminution they produce in the retinal images. This amount may be estimated as follows: Calculation of the amount of increase of the reti- nal image, and, consequently, of visual acuteness by con- vex glasses. Let hf = i®i,Fig. 2, be the linear dimension of a smallest retinal image of an hyperopic eye, and hi — jS2, the retinal image of the same object in the same distance when looked at through a convex glass, then ft and 02 constitute cor- responding lines in two similar triangles, and are to each other as their distances from the corresponding nodal points. The quantity by which the second nodal point is shifted on the axes may be called 8 = h\ \\ — h\ 1%, then hk| = Fi — S, since the distance of the second nodal point of the compound system from the retina is equal to the first focal length of the eye, hk| = Ft. We there- fore obtain the following proportion:— 30 — = from wliicli is deduced 0i f i ~ o, a _ Fi ~ Fj— <5' If we give [3t the standard value 1, we obtain F 02 = as the amount of 02 with regard to 0t. hi— o Fi being 14,858 mm., and 5 = 1,0909 mm. (for + 10 as we saw above), we obtain 02 — 1,0793, as the co-efficient of any retinal image, when + 10 is xoorn half an inch before the eye. If we measure visual acuteness by the smallest percep- tible retinal image, and assume the hyperopic eye had S — 1, it will have S = 1,0793 when armed with + 10. Since the linear dimension of the retinal image is in simple inverse proportion to the distance of the object, that is, decreases as the object is removed, Sn. xx. must be 1,0793 x 20' = 21,580'removed from an eye armed with + 10 in order to produce the smallest perceptible retinal image. ( B.) Calculation of the amount of diminution of the reti- nal image, and, consequently, the visual acuteness, by con- cave glasses. In the unaided myopic eye the second nodal point lies in the same place as in the emmetropic eye, Fig. 2. Since the retina is distended proportionately to its retrocession, the retinal elements contained in the line eg6 of the emmetropic eye are distributed over the longer line mgm of the myopic eye. The retrocession of the second nodal point from ~k\ to h™, resulting from the ad- 31 dition of a concave glass before tlie eye, generates from the same object which in the unaided myopic eye produ- ced the image my”1, now the smaller image mn. The relation of magnitude of both these images is easy to as- certain. m k™ is equal to Jh\ — 14,858 mm., and k™ k\ — 8 is the retrocession of the second nodal point, amounting for a glass of 10" of negative focal distance to 1,0909 mm. If mn = z3'2 and mgm = fi1} the similarity of the respec- tive triangles shows — = d~'—r = 0,9316, fit F, + S which expresses the co-efficient of the diminishing power of concave 10". A myopic eye, armed with—10", therefore, must be con- sidered to possess normal acuteness of vision, if it is able to read Sn. xx. at 0,9316 x 20' = 18,632'. I have disregarded, in the foregoing investigations, the appearance of dispersion circles, and was certainly justi- fied to do so, because I founded the visual acuteness on the density of the percipient retinal elements and the dimen- sions —‘J—‘J—1 I—1 H‘H>1—1■ 1—11—‘ t—<; t—'Ml-‘1—l 'rfa.'oo CO Ox 4*-'oo'u>'fcO>'t-‘'>—> i—‘ t—1 ©'©'© ocoojtoooMkoatoMWMO^^ko StMOaOOitKO^t'OOMK-CDQOOi (Xm^OiOOCOOiCChOhmOIOO Co-efficient of magni- fying effect of con- vex glass. O o o o o © ©p o o o oi os ci —t oo*00*oo'bo'bo'co'c©'co'c©'c© go m o w s o io #—i o o h u a s WtOOSMWUO^tOMOiOih-ffiffi SSQOOOOCOHi-aOOOMOOtOtO Co-efficient of dimin- ishing effect of con- cave glass. JOJfrJOjt* J—1 00 pi OxjS-JW U> tCJ.O MOO O to Ox so Ox SOOxtOOtOOOMOi^O^tOCOOsO S being 1, No. xx. Sn. should be read with convex glass in Paris feet. J—1 Jo po S Jjfo JSs Js> J-l JM J» J» CD Jo Jo © 00 H1- o'*o'4i-'o'ox'co'Voo'H-‘'oo'o5'c-‘ Ox N OUO 00 M 00 S W O >MO O to W to to S — 1, No. xx Sn. should be read with concave glass in Paris feet .Remarks on the foregoing Table. Tlie displacement of tlie second cardinal points, that is, the second principal, nodal, and focal points, expresses at the same time the elongation or shortening of the ocular axis in degrees of ametropia corresponding to the number of the spectacle-glasses enumerated in the first column. The length of the ocular axis, that is, the dis- tance between the apex of the cornea and the fovea centralis retinae, in the normal eye, is 22,23 mm., ac- cording to Listing'1 s diagram. We may, therefore, avail ourselves of this table to determine, with the ophthalmo- scope or functional testing, the situation of any part of the fundus oculi with regard to the position of the posterior 34 focal plane. If, for instance, a tumor or a circumscribed exudation projects over tlie background of tlie eye, we have first to ascertain with which auxiliary glass, put behind the ophthalmoscope, we can see clearly, by relaxed accommodation and in the upright image, the background of the eye, and, secondly, with which other glass we can see the summit of the projection. The difference of both glasses will give the height of the elevation by referring to the first and second columns of our table. Since this evaluation is of importance in judging the existence and amount of any elevation or depression, as well as its aug- mentation or diminution during the course of the disease, I shall illustrate the manner of this ophthalmoscopic measurement by some examples. 1. In an emmetropic eye, the fundus of which an em- metropic observer sees distinctly without any auxiliary glass put behind the ophthalmoscope, and an ametropic observer with his neutralizing glass, there is a circum- scribed exudation or tumor, the summit of which is dis- tinctly seen in the erect image with all the convex glasses up to number 8, whilst with stronger glasses it appears indistinct. Then No. 8, the strongest convex glass with which the summit of the tumor appears distinct, indicates an elevation of the tumor by 1,36 mm. over the back- ground of the eye, as is seen by the number of the second column of the above table corresponding to No. 8.* * I have described this method of estimating the relief of the background of the eye at the meeting of the Societe Universelle d’Ophthalmologie, Aug., 1867, in Paris, and given a table relating to it in my book on “ Intraocular 35 2. The fundus oculi is seen with + 24 distinctly, the summit of a tumor with + 4. The height of the tumor is calculated as follows: J ~ or nearly ~. No. 5 in the first column of the above table indicates, as seen in the second column, an elevation of 2,18 mm. over the level of the retina. 3. The fundus is seen distinctly with — 20; the sum- mit of a tumor with + 10. ~o + 20 — =63 gives, with reference to columns the first and second, 1,66 mm. as the height of the tumor. 4. A hyperopic eye, the retina of which appears dis- tinct with + 6, suffers from chronic glaucoma. The area of the optic disc appears plain with +18. How deep is the excavation? ~ Answer: 1,2 mm. This method of estimating elevations and depressions is especially valuable in the early stages of new growths and excavations, when the differential diagnosis and our judgment with regard to the progressiveness of the morbid action are apt to be difficult. The third and fourth columns of the above table do not require much explanation. Each glass of the first column, Tumors,” p. 106. The numbers there were obtained by another way of calcu- lation, and differ slightly from those given in this paper, because I took as basis of the former calculation the results of my own measurements on the living eye, whilst for the calculation of the present table the values of Listing's dia- grammatic eye are taken as basis. I have here preferred Listing's values, although they are perhaps not so generally correct as those obtained on the living eye, because they are at the reach of everybody, and the difference between the two is unimportant. Dr. Mauthner also describes the measurement of the depth of the background of the eye in his Treatise on Ophthalmoscopy, Vienna, 1868. He gives some examples, but no table to refer to. 36 by displacing tbe second nodal point, produces a certain alteration of tlie size of tlie retinal images. This alter- ation is found by multiplying tlie linear dimensions of tlie retinal images with the corresponding numbers of the third and fourth columns. Therefore I have called them co-efficients of the magnifying or diminishing effect of spectacles. The fifth and sixth columns need not much explication either. Snellen’s test-types being so chosen that the size of the letters or the intervals between them produce, at the distance indicated by their numbers, the smallest per- ceptible retinal images, then by looking with spectacles, on account of their magnifying or diminishing power, the distances of the types from the eye must be changed, if the images are to remain the smallest possible for distinct perception. We find the requi- site distance for each number of Snellen’s test-types, and for each spectacle-glass, by multiplying the number of the type with the co-efficient of magnifying or diminish- ing power of the glass. This having been done for No. xx with the series of test-glasses, the fifth and sixth columns give a comprehensive statement of the influence of spectacles on the acuteness of vision. We see that spectacles weaker than number ten have but a slight influence on the distance in which the different types should be read, so that we may fairly neglect it. Stron- ger glasses than No. 10 have a notable influence on the distance in which the type ought to be read. This influ- ence, however, is not so great as might perhaps be an- 37 ticipated, since of strongest convex glasses No. 2 requires only one and a half of the distance indicated by the number of type, No. 4 nearly 1 of it, etc., whilst con- cave glasses No. 2 require only f of the distance stated in the number of type, in order to let visual acuteness appear normal. I think it is not practical to change anything in our accustomed annotations of visual acuteness. But when it is of importance to judge exactly of the acuity of vision, we may refer to the above table which will in a moment give us the correction to be made in our anno- tations. Say, for instance, a myopic eye can read with number two Sn- xx at 15', then we would note it as follows: M|, S*|. A look at column the sixth of our table will show us immediately that S in this case is not f, but 1. The use of the table for reference appears to me so simple, that I think it unnecessary to give any further examples. (b.) ixfluehce of spectacles ox the aphakial eye. The optical system of the aphakial eye—which means an eye whose crystalline lens has been removed, or dis- located, or absorbed—is essentially different from that of the emmetropic eye. As clear vision in aphakial eyes can only be brought about by the help of strong convex glasses, I shall now proceed to investigate what influences such glasses exert on the optical system and visual acuteness of aphakial eyes. In noting, at the present day, the results of our cataract-operations, we do no longer content ourselves by tlie general expres- sions that good or useful vision was obtained, or even that sight was regained, but we test the acuteness of vision in quite as rigid a manner as we do in ordinary eyes. To know the alterations which spectacles produce in aphakial eyes, is, therefore, not merely of theoretical, but of practical interest. I shall determine the optical constants of armed apha- kial eyes in the same manner as I did those of armed emmetropic eyes. The optical constants of tlie unarmed aphakial eye which constitute the second system, are the following ). The cyst itself appeared as a transparent, homogene- ous, somewhat grayish bag, filled with clear water. The coloboma and iris could be seen through it. The whole anterior surface of the cyst appeared to be in immediate contact with the cornea, whilst its inferior border was round, and formed an angle in the pupil (a). Its upper and outer part lay upon the iris, which it pushed back- ward (b). The surface of this part of the iris, visible through the cyst, displayed a grayish discoloration, but was smooth, with quite a regular pupillary edge. On the upper corneal margin there existed a small, slit- shaped iridodialysis (0, Figs. 5 and 6). Entirely differ- ent was that portion of the iris bordering on the inner side of the coloboma. It was very much pushed back- ward, and showed two cup-like depressions (