Conversations on Natural Philosophy, in which the Elements of that Science are Familiarly Explained
Part 22
_Mrs. B._ Do not forget that the direct rays of light which pass from the sun to the earth, do not meet our eyes, excepting when we are looking at that luminary, and thus intercept them; in which case, you know, that the sun appears white. The atmosphere is a transparent medium, through which the sun's rays pass freely to the earth; but the particles of which it is composed, also reflect the rays of light, and it appears that they possess the property of reflecting the blue rays, the most copiously: the light, therefore, which is reflected back into the atmosphere, from the surface of the earth, falls upon these particles of air, and the blue rays are returned by reflection: this reflection is performed in every possible direction; so that whenever we look at the atmosphere, some of these rays fall upon our eyes; hence we see the air of a blue colour. If the atmosphere did not reflect any rays, though the objects, on the surface of the earth, would be illuminated, the sky would appear perfectly black.
_Caroline._ Oh, how melancholy would that be; and how pernicious to the sight, to be constantly viewing bright objects against a black sky. But what is the reason that bodies often change their colour; as leaves, which wither in autumn, or a spot of ink, which produces an iron-mould on linen?
_Mrs. B._ It arises from some chemical change, which takes place in the arrangement of the component parts; by which they lose their tendency to reflect certain colours, and acquire the power of reflecting others. A withered leaf thus no linger reflects the blue rays; it appears, therefore, yellow, or has a slight tendency to reflect several rays, which produce a dingy brown colour.
An ink spot on linen, at first absorbs all the rays; but, from the action of soap, or of some other agent, it undergoes a chemical change, and the spot partially regains its tendency to reflect colours, but with a preference to reflect the yellow rays, and such is the colour of the iron-mould.
_Emily._ Bodies, then, far from being of the colour which they appear to possess, are of that colour to which they have the greatest aversion, with which they will not incorporate, but reject, and drive from them.
_Mrs. B._ It certainly is so; though I scarcely dare venture to advance such an opinion, whilst Caroline is contemplating her beautiful rose.
_Caroline._ My poor rose! you are not satisfied with depriving it of colour, but even make it have an aversion to it; and I am unable to contradict you.
_Emily._ Since dark bodies, absorb more solar rays than light ones, the former should sooner be heated if exposed to the sun?
_Mrs. B._ And they are found, by experience, to be so. Have you never observed a black dress, to be warmer than a white one?
_Emily._ Yes, and a white one more dazzling: the black is heated by absorbing the rays, the white is dazzling, by reflecting them.
_Caroline._ And this was the reason that the brown paper was burnt in the focus of the lens, whilst the white paper exhibited the most luminous spot, but did not take fire.
_Mrs. B._ It was so. It is now full time to conclude our lesson. At our next meeting, I shall give you a description of the eye.
Questions
1. (Pg. 179) What is meant by the refraction of light?
2. (Pg. 179) What is believed to be the cause of refraction?
3. (Pg. 180) How is a ray refracted in passing obliquely from air into water?
4. (Pg. 180) How is this refraction explained in fig. 1, plate 19?
5. (Pg. 180) What is fig. 2 intended to explain?
6. (Pg. 180) What is the rule respecting refraction, by different mediums?
7. (Pg. 181) What is meant by the perpendicular?
8. (Pg. 181) How does fig. 3, plate 19, elucidate the law of refraction?
9. (Pg. 181) What will be the effect on the apparent situation of the flower?
10. (Pg. 181) What effect has refraction upon the apparent depth of a stream of water?
11. (Pg. 182) How does the atmosphere refract the rays of the sun, as represented, fig. 4?
12. (Pg. 182) Why have we the rays of the sun always refracted?
13. (Pg. 182) What length of time is required for light to travel from the sun, to the earth?
14. (Pg. 182) What effect has this upon his apparent place?
15. (Pg. 182) How is the length of the day affected by refraction?
16. (Pg. 183) How are rays refracted, which fall obliquely upon a flat pane of glass, (fig. 5, plate 19?)
17. (Pg. 183) What is the reason that objects are distorted, when seen through common window glass?
18. (Pg. 184) What is meant by a lens?
19. (Pg. 184) What are the five kinds called, represented at fig. 1, plate 20?
20. (Pg. 184) What is meant by the axis of a lens?
21. (Pg. 184) How are parallel rays, refracted by the double convex lens, fig. 6, plate 19?
22. (Pg. 184) What is meant by the focus of a lens?
23. (Pg. 184) What is the focal distance of parallel rays, from a double convex lens?
24. (Pg. 184) How are the rays refracted by a concave lens, fig. 7, plate 19?
25. (Pg. 185) What is the effect of one plane side in a lens?
26. (Pg. 185) How is the focus of the plano-convex lens situated, fig. 2, plate 20?
27. (Pg. 185) How does a convex lens magnify objects, fig. 6, plate 19?
28. (Pg. 185) What is the article denominated which is represented at fig. 3, plate 20?
29. (Pg. 185) How will a ray be refracted, which enters on one side of the prism, in the direction A B?
30. (Pg. 185) What effect is produced by this refraction, as represented in fig. 4, plate 20?
31. (Pg. 186) Of what are the rays of white light said to be composed?
32. (Pg. 186) What colours are produced?
33. (Pg. 186) By what property, in light, does refraction enable us to separate these different rays?
34. (Pg. 187) What experiment may be performed with a piece of card, so as to exemplify the compound nature of light?
35. (Pg. 187) How can the same be shown by a lens, fig. 5. plate 20?
36. (Pg. 187) Is it certain that there are seven primitive colours in the spectrum?
37. (Pg. 188) How is the rainbow produced, and what is necessary to its production?
38. (Pg. 188) How are the solar rays affected by a convex lens?
39. (Pg. 188) Why is such a lens, called a burning glass?
40. (Pg. 188) Why are bodies of a dark colour, more readily inflamed, than those which are white?
41. (Pg. 189) What is believed to be the reason, why some bodies absorb more rays than others?
42. (Pg. 189) What determines the colour of any particular body?
43. (Pg. 189) What exemplifications are given?
44. (Pg. 189) By what reasoning is it proved, that bodies do not retain their colours in the dark?
45. (Pg. 190) What proof of the truth of this theory of colours, may be afforded by the prism?
46. (Pg. 191) Why will green leaves, when exposed to the red ray, appear of a dingy brown?
47. (Pg. 191) Bodies, in general, when placed in a ray differing in colour from their own, appear of a mixed hue, what causes this?
48. (Pg. 191) Why will bodies of a pale, or light hue, most perfectly, assume the different colours of the spectrum?
49. (Pg. 192) Upon what property in a body, does the darkness of its colour depend?
50. (Pg. 192) Why do some bodies appear white, others black, and others of different colours?
51. (Pg. 192) From what cause do blue articles appear green, by candle-light?
52. (Pg. 193) What is believed to be the cause, of the red appearance of the sun, through a fog, or misty atmosphere?
53. (Pg. 193) From what is the blue colour of the sky, thought to arise?
54. (Pg. 193) What would be the colour of the sky, did not the atmosphere reflect light?
55. (Pg. 193) From what cause do some bodies change their colour, as leaves formerly green, become brown, and ink, yellow?
56. (Pg. 194) Why is a black dress, warmer in the sunshine, than a white one of the same texture?
CONVERSATION XVII.
ON THE STRUCTURE OF THE EYE, AND OPTICAL INSTRUMENTS.
DESCRIPTION OF THE EYE. OF THE IMAGE ON THE RETINA. REFRACTION BY THE HUMOURS OF THE EYE. OF THE USE OF SPECTACLES. OF THE SINGLE MICROSCOPE. OF THE DOUBLE MICROSCOPE. OF THE SOLAR MICROSCOPE. MAGIC LANTHORN. REFRACTING TELESCOPE. REFLECTING TELESCOPE.
MRS. B.
The body of the eye, is of a spherical form: (fig. 1. plate 21.) it has two membranous coats, or coverings; the external one, _a a a_, is called the sclerotica, this is commonly known under the name of the white of the eye; it has a projection in that part of the eye which is exposed to view, _b b_, which is called the transparent cornea, because, when dried, it has nearly the consistence of very fine horn, and is sufficiently transparent for the light to obtain free passage through it.
The second membrane which lines the cornea, and envelops the eye, is called the choroid, _c c c_; this has an opening in front, just beneath the cornea, which forms the pupil, or sight of the eye, _d d_, through which the rays of light pass into the eye. The pupil is surrounded by a coloured border called the iris, _e e_, which, by its muscular motion, always preserves the pupil of a circular form, whether it is expanded in the dark, or contracted by a strong light. This you will understand better by examining fig. 2.
_Emily._ I did not know that the pupil was susceptible of varying its dimensions.
_Mrs. B._ The construction of the eye is so admirable, that it is capable of adapting itself, more or less, to the circumstances in which it is placed. In a faint light, the pupil dilates so as to receive an additional quantity of rays, and in a strong light, it contracts, in order to prevent the intensity of the light from injuring the optic nerve. Observe Emily's eyes, as she sits looking towards the windows: the pupils appear very small, and the iris, large. Now, Emily, turn from the light, and cover your eyes with your hand, so as entirely to exclude it, for a few moments.
_Caroline._ How very much the pupils of her eyes are now enlarged, and the iris diminished! This is, no doubt, the reason why the eyes suffer pain, when from darkness, they suddenly come into a strong light; for the pupil being dilated, a quantity of rays must rush in, before it has time to contract.
_Emily._ And when we go from a strong light, into obscurity, we at first imagine ourselves in total darkness; for a sufficient number of rays cannot gain admittance into the contracted pupil, to enable us to distinguish objects: but in a few minutes it dilates, and we clearly perceive objects which were before invisible.
_Mrs. B._ It is just so. The choroid _c c_, is embued with a black liquor, which serves to absorb all the rays that are irregularly reflected, and to convert the body of the eye, into a more perfect camera obscura. When the pupil is expanded to its utmost extent, it is capable of admitting ten times the quantity of light, that it does when most contracted. In cats, and animals which are said to see in the dark, the power of dilatation and contraction of the pupil, is still greater; it is computed that the pupils of their eyes may admit one hundred times more light at one time than at another.
Within these coverings of the eye-ball, are contained, three transparent substances, called humours. The first occupies the space immediately behind the cornea, and is called the aqueous humour, _f f_, from its liquidity and its resemblance to water. Beyond this, is situated the crystalline humour, _g g_, so called from its clearness and transparency: it has the form of a lens, and refracts the rays of light in a greater degree of perfection, than any that have been constructed by art: it is attached by two muscles, _m m_, to each side of the choroid. The back part of the eye, between the crystalline humour and the retina, is filled by the vitreous humour, _h h_, which derives its name from a resemblance it is supposed to bear, to glass, or vitrified substances.
The membranous coverings of the eye are intended chiefly for the preservation of the retina, _i i_, which is by far the most important part of the eye, as it is that which receives the impression of the objects of sight, and conveys it to the mind. The retina is formed by the expansion of the optic nerve, and is of a most perfect whiteness: this nerve proceeds from the brain, enters the eye, at _n_, on the side next the nose, and is finely spread over the interior surface of the choroid.
The rays of light which enter the eye, by the pupil, are refracted by the several humours in their passage through them, and unite in a focus on the retina.
_Caroline._ I do not understand the use of these refracting humours: the image of objects was represented in the camera obscura, without any such assistance.
_Mrs. B._ That is true; but the representation became much more strong and distinct, when we enlarged the opening of the camera obscura, and received the rays into it, through a lens.
I have told you, that rays proceed from bodies in all possible directions. We must, therefore, consider every part of an object which sends rays to our eyes, as points from which the rays diverge, as from a centre.
_Emily._ These divergent rays, issuing from a single point, I believe you told us, were called a pencil of rays?
_Mrs. B._ Yes. Now, divergent rays, on entering the pupil, do not cross each other; the pupil, however, is sufficiently large to admit a small pencil of them; and these, if not refracted to a focus, by the humours, would continue diverging after they had passed the pupil, would fall dispersed upon the retina, and thus the image of a single point, would be expanded over a large portion of the retina. The divergent rays from every other point of the object, would be spread over a similar extent of space, and would interfere and be confounded with the first; so that no distinct image could be formed, and the representation on the retina would be confused, both in figure and colour. Fig. 3. represents two pencils of rays, issuing from two points of the tree, A B, and entering the pupil C, refracted by the crystalline humour D, and forming on the retina, at _a b_, distinct images of the spot they proceed from. Fig. 4. differs from the preceding, merely from not being supplied with a lens; in consequence of which, the pencils of rays are not refracted to a focus, and no distinct image is formed on the retina. I have delineated only the rays issuing from two points of an object, and distinguished the two pencils in fig. 4. by describing one of them with dotted lines: the interference of these two pencils of rays on the retina, will enable you to form an idea of the confusion which would arise, from thousands and millions of points, at the same instant pouring their divergent rays upon the retina.
_Emily._ True; but I do not yet well understand, how the refracting humours, remedy this imperfection.
_Mrs. B._ The refraction of these several humours, unites the whole of a pencil of rays, proceeding from any one point of an object, to a corresponding point on the retina, and the image is thus rendered distinct and strong. If you conceive, in fig. 3., every point of the tree to send forth a pencil of rays, similar to those from A B, every part of the tree will be as accurately represented on the retina, as the points _a b_.
_Emily._ How admirably, how wonderfully, is this contrived!
_Caroline._ But since the eye absolutely requires refracting humours, in order to have a distinct representation formed on the retina, why is not the same refraction equally necessary, for the images formed in the camera obscura?
_Mrs. B._ It is; excepting the aperture through which we receive the rays into the camera obscura, is extremely small; so that but very few of the rays diverging from a point, gain admittance; but when we enlarged the aperture, and furnished it with a lens, you found the landscape more perfectly represented.
_Caroline._ I remember how obscure and confused the image was, when you enlarged the opening, without putting in the lens.
_Mrs. B._ Such, or very similar, would be the representation on the retina, unassisted by the refracting humours.
You will now be able to understand the nature of that imperfection of sight, which arises from the eyes being too prominent. In such cases, the crystalline humour, D, (fig. 5.) being extremely convex, refracts the rays too much, and collects a pencil, proceeding from the object A B, into a focus, F, before they reach the retina. From this focus, the rays proceed, diverging, and consequently form a very confused image on the retina, at _a b_. This is the defect in short-sighted people.
_Emily._ I understand it perfectly. But why is this defect remedied by bringing the object nearer to the eye, as we find to be the case with short-sighted people?
_Mrs. B._ The nearer you bring an object to your eye, the more divergent the rays fall upon the crystalline humour, and consequently they are not so soon converged to a focus: this focus, therefore, either falls upon the retina, or at least approaches nearer to it, and the object is proportionally distinct, as in fig. 6.
_Emily._ The nearer, then, you bring an object to a lens, the further the image recedes behind it.
_Mrs. B._ Certainly. But short-sighted persons have another resource, for objects which they can not bring near to their eyes; this is, to place a concave lens, C D, (fig. 1, plate 22.) before the eye, in order to increase the divergence of the rays. The effect of a concave lens, is, you know, exactly the reverse of a convex one: it renders parallel rays divergent, and those which are already divergent, still more so. By the assistance of such glasses, therefore, the rays from a distant object, fall on the pupil, as divergent as those from a less distant object; and, with short-sighted people, they throw the image of a distant object, back, as far as the retina.
_Caroline._ This is an excellent contrivance, indeed.
_Mrs. B._ And tell me, what remedy would you devise for such persons as have a contrary defect in their sight; that is to say, who are long-sighted, in whom the crystalline humour, being too flat, does not refract the rays sufficiently, so that they reach the retina before they are converged to a point?
_Caroline._ I suppose that a contrary remedy must be applied to this defect; that is to say, a convex lens, L M, fig. 2, to make up for the deficiency of convexity of the crystalline humour, O P. For the convex lens would bring the rays nearer together, so that they would fall, either less divergent, or parallel, on the crystalline humour; and, by being sooner converged to a focus, would fall on the retina.
_Mrs. B._ Very well, Caroline. This is the reason why elderly people, the humours of whose eyes are decayed by age, are under the necessity of using convex spectacles. And when deprived of that resource, they hold the object at a distance from their eyes, as in fig. 3, in order to bring the focus more forward.
_Caroline._ I have often been surprised, when my grandfather reads without his spectacles, to see him hold the book at a considerable distance from his eyes. But I now understand the cause; the more distant the object is from the crystalline lens, the nearer to it, will the image be formed.
_Emily._ I comprehend the nature of these two opposite defects very well; but I cannot now conceive, how any sight can be perfect: for, if the crystalline humour is of a proper degree of convexity, to bring the image of distant objects to a focus on the retina, it will not represent near objects distinctly; and if, on the contrary, it is adapted to give a clear image of near objects, it will produce a very imperfect one, of distant objects.
_Mrs. B._ Your observation is very good, Emily; and it is true, that every person would be subject to one of these two defects, if we had it not in our power to adapt the eye, to the distance of the object; it is believed that this is accomplished, by our having a command over the crystalline lens, so as to project it towards, or draw it back from the object, as circumstances require, by means of the two muscles, to which the crystalline humour is attached; so that the focus of the rays, constantly falls on the retina, and an image is formed equally distinct, either of distant objects, or of those which are near.
_Caroline._ In the eyes of fishes, which are the only eyes I have ever seen separate from the head, the cornea does not protrude, in that part of the eye which is exposed to view.
_Mrs. B._ The cornea of the eye of a fish is not more convex than the rest of the ball of the eye; but to supply this deficiency, their crystalline humour is spherical, and refracts the rays so much, that it does not require the assistance of the cornea to bring them to a focus on the retina.
_Emily._ Pray, what is the reason that we cannot see an object distinctly, if we place it very near to the eye?
_Mrs. B._ Because the rays fall on the crystalline humour, too divergent to be refracted to a focus on the retina; the confusion, therefore, arising from viewing an object too near the eye, is similar to that which proceeds from a flattened crystalline humour; the rays reach the retina before they are collected to a focus, (fig. 4.) If it were not for this imperfection, we should be able to see and distinguish the parts of objects, which, from their minuteness, are now invisible to us; for, could we place them very near the eye, the image on the retina would be so much magnified, as to render them visible.
_Emily._ And could there be no contrivance, to convey the rays of objects viewed, close to the eye, so that they should be refracted to a focus on the retina?
_Mrs. B._ The microscope is constructed for this purpose. The single microscope (fig. 5.) consists simply of a convex lens, commonly called a magnifying glass; in the focus of which the object is placed, and through which it is viewed: by this means, you are enabled to place your eye very near to the object, for the lens A B, by diminishing the divergence of the rays, before they enter the pupil C, makes them fall parallel on the crystalline humour D, by which they are refracted to a focus on the retina, at R R.
_Emily._ This is a most admirable invention, and nothing can be more simple; for the lens magnifies the object, merely by allowing us to bring it nearer to the eye.
_Mrs. B._ Those lenses, therefore, which have the shortest focus will magnify the object most, because they enable us to place it nearest to the eye.
_Emily._ But a lens, that has the shortest focus, is most bulging or convex; and the protuberance of the lens will prevent the eye from approaching very near to the object.
_Mrs. B._ This is remedied by making the lens extremely small: it may then be spherical without occupying much space, and thus unite the advantages of a short focus, and of allowing the eye to approach the object.
There is a mode of magnifying objects, without the use of a lens: if you look through a hole, not larger than a small pin, you may place a minute object near to the eye, and it will be distinct, and greatly enlarged. This piece of tin has been perforated for the purpose; place it close to your eye, and this small print before it.
_Caroline._ Astonishing! the letters appear ten times as large as they do without it: I cannot conceive how this effect is produced.
_Mrs. B._ The smallness of the hole, prevents the entrance into the eye, of those parts of every pencil of rays which diverge much; so that, notwithstanding the nearness of the object, those rays from it, which enter the eye, are nearly parallel, and are, therefore, brought to a focus by the humours of the eye.
_Caroline._ We have a microscope at home, which is a much more complicated instrument than that you have described.