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Lenses and Waves

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THE 'PROJET' OF 1672 137<br />

consisted of six generally accepted principles required to elaborate<br />

mathematical theory. In a way reminiscent of the ‘Projet’, Barrow said that<br />

these hypotheses, as he called them, were empirically founded but also<br />

needed some sort of explanation:<br />

“The hypotheses agree with observation, but we must also fortify them with some<br />

support of reason, by treading on the foundations <strong>and</strong> suppositions laid down.” 105<br />

In his first lecture Barrow discussed these foundations <strong>and</strong> suppositions,<br />

although he mainly defined terms like ‘light’ (in relation to illumination,<br />

images, ‘phasmata’ <strong>and</strong> the like), ‘refraction’ <strong>and</strong> ‘opaque’. He then proposed<br />

a theory of light that is a hybrid of viewing light as a pulse <strong>and</strong> as a pressure<br />

propagated simultaneously in the first <strong>and</strong> second matter of the Cartesian<br />

scheme. 106 Whatever he meant precisely, Barrow did not lend much weight to<br />

this theory.<br />

“Still, since it is desirable for me to lay some preliminary foundations about the nature of<br />

light, to agree with my explanation of hypotheses which I shall later offer, I conceive<br />

the facts to be these, or something like them: …” 107<br />

These preliminary foundations merely needed to be consistent with the<br />

ensuing explanations of the laws of optics <strong>and</strong> Barrow expressly did not<br />

claim any authority in these matters. 108 In what followed, Barrow’s theory of<br />

light came down to considering a ray to be the path traced out by a pulse-like<br />

entity, “… two-dimensional <strong>and</strong> like a sort of rectangular parallelogram lying<br />

in a plane at right angles to the surface of the inflecting medium, …” 109 This<br />

conception of a physical ray traced out by a line of light emitted by a shining<br />

object went back to Hobbes’ theory of light. Barrow’s derivation of the law<br />

of sines can likewise be traced back to Hobbes. 110 With this definition of a<br />

ray, Barrow now could make ‘some attempt to explain’ the laws of optics,<br />

stressing once more that they were empirically founded:<br />

“… I need practically nothing else to explain the hypotheses which all opticians in<br />

common with each other assume <strong>and</strong> which must necessarily be laid down as a<br />

foundation for building up this science. I shall make no effort to prove what I have<br />

said, since … it seems clearer than light itself that such proofs cannot be given,<br />

although a number of experiments show that they are given in actuality.” 111<br />

Besides accounting for the rectilinearity of light rays, he discussed some basic<br />

assumptions of geometrical optics, like the fact that ‘inflections’ take place in<br />

a plane perpendicular to the surface of the ‘inflecting’ medium. Then, in the<br />

second lecture, he moved on to these ‘inflections’ proper, reflection <strong>and</strong><br />

105<br />

Barrow, Lectiones, [26].<br />

106<br />

Barrow, Lectiones, [15-16].<br />

107<br />

Barrow, Lectiones, [15]; (emphasis in original).<br />

108<br />

Barrow, Lectiones, [8, 15].<br />

109<br />

Barrow, Lectiones, [26].<br />

110<br />

Shapiro, “Kinematic optics”, 177-181. Hobbes’ optics is discussed in the next chapter, section 5.2.1.<br />

111 Barrow, Lectiones, [17]

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