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Lenses and Waves

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130 CHAPTER 4<br />

Therefore the distance between lines FE <strong>and</strong> HB must be twice a large as that<br />

between AC <strong>and</strong> HB. As a result, the ball reaches point I on the circle. The<br />

same is the case when instead of a cloth the ball hits the surface of a body of<br />

water. For the water does not alter the motion of the ball any further after it<br />

has passed the surface, according to Descartes. When the ball passes a<br />

boundary where in some way or another its quantity of motion is augmented,<br />

it reaches the circumference of the circle earlier <strong>and</strong> is deflected towards the<br />

normal of the surface. Note that Descartes did not specify the change of the<br />

perpendicular component, a point that is often overlooked. He did not know<br />

that amount <strong>and</strong> he did not need to, for the two assumptions he used suffice<br />

for the derivation of the sine law. 81<br />

As Descartes took the motions of the ball to reflect the deflections of<br />

light, he could now draw his main conclusion. Rays of light are deflected in<br />

exact proportion to the ease with which a transparent medium receives them<br />

compared to the medium from which they come. The only remaining<br />

difference between the motion of a ball <strong>and</strong> the action of light is that a<br />

denser medium like water allows rays of light to pass more easily. The<br />

deflection caused by the passage from one medium into another ought to be<br />

measured, not by the angles made with the refracting surface, but by the lines<br />

CB <strong>and</strong> BE. Unlike the proportion between the angles of incidence <strong>and</strong><br />

refraction, the proportion between these sines remains the same for any<br />

refraction caused by a pair of mediums, irrespective of the angle of<br />

incidence. Et voilà, the law of sines.<br />

Epistemic aspects of Descartes’ account in historical context<br />

Both historically <strong>and</strong> intrinsically, Descartes’ account of refraction is a key<br />

text in the transition from medieval perspectiva to seventeenth-century<br />

optics. Yet, the line of inference is subtle <strong>and</strong>, at many points, implicitly<br />

pursued. I will have to enlarge in some detail on its epistemic aspects in their<br />

historical context.<br />

At least three levels of inference can be distinguished in Descartes’<br />

account. In the first place the level of mathematics. This holds the derivation<br />

of the sine law from the two assumptions conveyed in the diagrams<br />

accompanying his discourse. First, the passage to another medium alters in a<br />

fixed ratio the quantity of motion. This ratio is represented by the radius of<br />

the circle. Second, the parallel component of the direction of motion is<br />

unaffected. This is represented by drawing horizontal lines in proportion to<br />

the successive times to travel to <strong>and</strong> from the center of the circle. The<br />

mathematical inference of Descartes’ account constituted a successful<br />

culmination of perspectivist optics, in that Descartes was the first to derive a<br />

law of refraction on the analytical groundwork laid by Kepler <strong>and</strong> his<br />

forebears. He brought consistency to the analysis of reflection <strong>and</strong> refraction<br />

by having the parallel component constant in all cases. More important, in<br />

81 When both aspects of the motion are interpreted as speeds the assumptions can be written as: vr = nvi<br />

<strong>and</strong> vi sini = vr sinr, which directly yield sini = n sinr. See Sabra, Theories of Light, 111.

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