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Lenses and Waves

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26 CHAPTER 2<br />

reply, Kepler briefly explained how lenses refract rays of light so that they<br />

can produced magnified images. 53 The explanation in Dissertatio was only a<br />

sketch, but the message was clear. The telescope was a remarkable invention,<br />

but its working needed mathematical clarification. A theory of the telescope<br />

was called for. Within a few months, Kepler developed one. In September<br />

1610, he finished the manuscript of Dioptrice, published the next year.<br />

“Some have disputed over the priority of its invention, others rather applied themselves<br />

to the perfection of the instrument, as there chance mainly counted, here reason<br />

dominated. But Galileo scored the greatest triumph by exploring its use to disclose<br />

secrets, because zeal procured him with the design <strong>and</strong> fortune has not withheld him<br />

the success. I, driven by an honest emulation, have shown the mathematicians a new<br />

field to expose their acuteness, in which the causes <strong>and</strong> principles are retraced to the<br />

laws of geometry, the effects of which are so awaited with much impatience <strong>and</strong> are of<br />

such pleasing diversity.” 54<br />

The goal of Dioptrice was to provide a mathematical account of the working<br />

of the telescope. In Kepler’s view, the working of any instrument used in<br />

astronomy should be understood precisely. A decade earlier, he had<br />

approached the puzzling properties of the pinhole images used in the<br />

observation of solar eclipses. His answer had been a new theory of image<br />

formation, which he had published in Paralipomena (1604). In Dioptrice, Kepler<br />

applied this theory to lenses in order to determine the dioptrical properties<br />

of the telescope. Dioptrice had one substantial shortcoming: Kepler knew that<br />

he did not know the exact law of refraction. He used an approximate rule<br />

instead.<br />

2.2.1 KEPLER AND THE MATHEMATICS OF LENSES<br />

Kepler’s concerns in Paralipomena were induced by a problem of astronomical<br />

observation. In 1598, Tycho Brahe had reported an anomalous observation<br />

of the apparent size of the moon during a solar eclipse. 55 Brahe used a<br />

pinhole to project the image of the eclipsed sun. When he measured the<br />

diameter of the projection he realized that “the moon during a solar eclipse<br />

does not appear to be the same size as it appears at other times during full<br />

moons when it is equally far away”. 56 He tried to produce consistent values<br />

by applying some ad hoc corrections to his measurements. 57 Kepler took a<br />

different approach, analyzing mathematically the way the image was<br />

produced. He had known the anomaly of pinhole images for some time<br />

53<br />

Kepler, Conversation, [19-21].<br />

54<br />

Kepler, Dioptrice, dedication (KGW4, 331). “… circaque eam alij de palma primae inventionis certarent,<br />

alij de perfectione instrumenti sese jactarent amplius, quod ibi casus potissimum insit, hic Ratio<br />

dominetur: GALILAEUS vero super usu patefacto in perquirendis arcanis Astronomicis speciosissimum<br />

triumphum ageret; ut cui consilium suppeditaverat industria, nec successum negaverat fortuna: Ego<br />

doctus honesta quadam aemulatione novum Mathematicis campum aperui exerendi vim ingenij, hoc est<br />

causarum lege geometrica demonstr<strong>and</strong>arum, quibus tam exoptati, tam jucunda varietate multiplices<br />

effectus inniterentur.”<br />

55<br />

Straker, “Kepler’s theory of pinhole images”, 276-278.<br />

56<br />

Cited <strong>and</strong> translated in: Straker, “Kepler’s theory of pinhole images”, 278.<br />

57<br />

Straker, “Kepler’s theory of pinhole images”, 275-276; 280-282.

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