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a history of science-2-第51章
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to an oblong form; was by the second reduced into an orbicular one with as much regularity as when it did not all pass through them。 So that; whatever was the cause of that length; 'twas not any contingent irregularity。 〃I then proceeded to examine more critically what might be effected by the difference of the incidence of rays coming from divers parts of the sun; and to that end measured the several lines and angles belonging to the image。 Its distance from the hole or prism was 22 feet; its utmost length 13 1/4 inches; its breadth 2 5/8; the diameter of the hole 1/4 of an inch; the angle which the rays; tending towards the middle of the image; made with those lines; in which they would have proceeded without refraction; was 44 degrees 56'; and the vertical angle of the prism; 63 degrees 12'。 Also the refractions on both sides of the prismthat is; of the incident and emergent rayswere; as near as I could make them; equal; and consequently about 54 degrees 4'; and the rays fell perpendicularly upon the wall。 Now; subducting the diameter of the hole from the length and breadth of the image; there remains 13 inches the length; and 2 3/8 the breadth; comprehended by those rays; which; passing through the centre of the said hole; which that breadth subtended; was about 31'; answerable to the sun's diameter; but the angle which its length subtended was more than five such diameters; namely 2 degrees 49'。 〃Having made these observations; I first computed from them the refractive power of the glass; and found it measured by the ratio of the sines 20 to 31。 And then; by that ratio; I computed the refractions of two rays flowing from opposite parts of the sun's discus; so as to differ 31' in their obliquity of incidence; and found that the emergent rays should have comprehended an angle of 31'; as they did; before they were incident。 〃But because this computation was founded on the hypothesis of the proportionality of the sines of incidence and refraction; which though by my own experience I could not imagine to be so erroneous as to make that angle but 31'; which in reality was 2 degrees 49'; yet my curiosity caused me again to make my prism。 And having placed it at my window; as before; I observed that by turning it a little about its axis to and fro; so as to vary its obliquity to the light more than an angle of 4 degrees or 5 degrees; the colors were not thereby sensibly translated from their place on the wall; and consequently by that variation of incidence the quantity of refraction was not sensibly varied。 By this experiment; therefore; as well as by the former computation; it was evident that the difference of the incidence of rays flowing from divers parts of the sun could not make them after decussation diverge at a sensibly greater angle than that at which they before converged; which being; at most; but about 31' or 32'; there still remained some other cause to be found out; from whence it could be 2 degrees 49'。〃 All this caused Newton to suspect that the rays; after their trajection through the prism; moved in curved rather than in straight lines; thus tending to be cast upon the wall at different places according to the amount of this curve。 His suspicions were increased; also; by happening to recall that a tennis…ball sometimes describes such a curve when 〃cut〃 by a tennis…racket striking the ball obliquely。 〃For a circular as well as a progressive motion being communicated to it by the stroke;〃 he says; 〃its parts on that side where the motions conspire must press and beat the contiguous air more violently than on the other; and there excite a reluctancy and reaction of the air proportionately greater。 And for the same reason; if the rays of light should possibly be globular bodies; and by their oblique passage out of one medium into another acquire a circulating motion; they ought to feel the greater resistance from the ambient ether on that side where the motions conspire; and thence be continually bowed to the other。 But notwithstanding this plausible ground of suspicion; when I came to examine it I could observe no such curvity in them。 And; besides (which was enough for my purpose); I observed that the difference 'twixt the length of the image and diameter of the hole through which the light was transmitted was proportionable to their distance。 〃The gradual removal of these suspicions at length led me to the experimentum crucis; which was this: I took two boards; and; placing one of them close behind the prism at the window; so that the light must pass through a small hole; made in it for the purpose; and fall on the other board; which I placed at about twelve feet distance; having first made a small hole in it also; for some of the incident light to pass through。 Then I placed another prism behind this second board; so that the light trajected through both the boards might pass through that also; and be again refracted before it arrived at the wall。 This done; I took the first prism in my hands and turned it to and fro slowly about its axis; so much as to make the several parts of the image; cast on the second board; successively pass through the hole in it; that I might observe to what places on the wall the second prism would refract them。 And I saw by the variation of these places that the light; tending to that end of the image towards which the refraction of the first prism was made; did in the second prism suffer a refraction considerably greater than the light tending to the other end。 And so the true cause of the length of that image was detected to be no other than that LIGHT consists of RAYS DIFFERENTLY REFRANGIBLE; which; without any respect to a difference in their incidence; were; according to their degrees of refrangibility; transmitted towards divers parts of the wall。〃'1'
THE NATURE OF COLOR Having thus proved the composition of light; Newton took up an exhaustive discussion as to colors; which cannot be entered into at length here。 Some of his remarks on the subject of compound colors; however; may be stated in part。 Newton's views are of particular interest in this connection; since; as we have already pointed out; the question as to what constituted color could not be agreed upon by the philosophers。 Some held that color was an integral part of the substance; others maintained that it was simply a reflection from the surface; and no scientific explanation had been generally accepted。 Newton concludes his paper as follows: 〃I might add more instances of this nature; but I shall conclude with the general one that the colors of all natural bodies have no other origin than this; that they are variously qualified to reflect one sort of light in greater plenty than another。 And this I have experimented in a dark room by illuminating those bodies with uncompounded light of divers colors。 For by that means any body may be made to appear of any color。 They have there no appropriate color; but ever appear of the color of the light cast upon them; but yet with this difference; that they are most brisk and vivid in the light of their own daylight color。 Minium appeareth there of any color indifferently with which 'tis illustrated; but yet most luminous in red; and so Bise appeareth indifferently of any col
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