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Lenses and Waves

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THE 'PROJET' OF 1672 133<br />

analogies, despite the fact that it hardly appears in La Dioptrique. 89 Drawing<br />

on the work of Mahoney, he says that the analogies provided a ‘heuristic<br />

model’ that legitimately compared the action of light with the motion of a<br />

ball. By leaving specific material factors in the motion of the ball aside,<br />

Descartes could single out the ball’s tendency to move rather than its<br />

motion. He then was ready to consider this tendency <strong>and</strong> distinguish<br />

between “… the power, …, which causes the movement of this ball to<br />

continue …” <strong>and</strong> “… that which determines it to move in one direction<br />

rather than in another, …” 90 According to Schuster this does not refer to a<br />

distinction between force of motion <strong>and</strong> direction of motion, but to a<br />

distinction between quantity of force of motion <strong>and</strong> directional magnitude of<br />

force of motion. The two assumptions of Descartes’ derivation are based on<br />

this distinction: the quantity depended on the medium <strong>and</strong> the parallel<br />

component of directional magnitude was constant. In La Dioptrique<br />

Descartes labeled the directional magnitude with the term ‘determination’ in<br />

order to analyze the components of the action without implicating the<br />

notion of velocity. 91<br />

With this interpretation of the analogies, Descartes’ analysis is not directly<br />

at odds with the system he expounded in Principia Philosophiae <strong>and</strong> Le Monde.<br />

There he had made the same distinction between quantity <strong>and</strong> directional<br />

magnitude. The first law of nature states that the quantity of force of motion<br />

is constant when a body is in uniform rectilinear motion; the third law states<br />

that a force of motion is conserved in a unique direction (tangent to the path<br />

of motion). 92 According to Schuster, the tension between the analogies <strong>and</strong><br />

the tendency theory can be resolved when Descartes’ heuristic use of the<br />

analogies is interpreted in the terms of his theory of motion. 93 In the light of<br />

the Galilean conception of motion Huygens <strong>and</strong> Newton employed (as do<br />

we), Descartes’ claim that he derived the laws of optics from his mechanistic<br />

principles was untenable. Sabra has sufficiently pointed this out. 94 Yet, this<br />

was not so much because his system was incoherent or inconsistent as,<br />

rather, because the interpretation of the underlying principles had changed.<br />

Descartes usually considered motion at an instant of impact <strong>and</strong> discussed it<br />

in terms of the body’s force to move. In the light of this science of motion,<br />

the mathematical derivation of the sine law can indeed be physically<br />

interpreted in a plausible manner. Yet, through his crude presentation in La<br />

Dioptrique Descartes made little effort to prevent misunderst<strong>and</strong>ings <strong>and</strong><br />

misinterpretations.<br />

89<br />

Schuster, “Descartes opticien”, 261-272 Schuster, Descartes, 273; Mahoney, Fermat, 387-393; Sabra,<br />

Theories, 78-89.<br />

90<br />

Descartes, AT6, 94-95.<br />

91<br />

Schuster, “Descartes opticien”, 258-261; Schuster, Descartes, 293<br />

92<br />

Schuster, Descartes, 288.<br />

93<br />

Schuster, “Descartes opticien” 261-265.<br />

94<br />

Sabra, Theories, 112-116.

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