Six Lectures on Light - Delivered In The United States In 1872-1873 by John Tyndall
page 72 of 237 (30%)
page 72 of 237 (30%)
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a transparent substance, the particles would be sucked in and
transmitted; turning their repelled poles, they would be driven away or reflected. Thus, by the ascription of poles, the transmission and reflection of the self-same particle at different times might be accounted for. Consider these rings of Newton as seen in pure red light: they are alternately bright and dark. The film of air corresponding to the outermost of them is not thicker than an ordinary soap-bubble, and it becomes thinner on approaching the centre; still Newton, as I have said, measured the thickness corresponding to every ring, and showed the difference of thickness between ring and ring. Now, mark the result. For the sake of convenience, let us call the thickness of the film of air corresponding to the first dark ring _d_; then Newton found the distance corresponding to the second dark ring 2 _d_; the thickness corresponding to the third dark ring 3 _d_; the thickness corresponding to the tenth dark ring 10 _d_, and so on. Surely there must be some hidden meaning in this little distance, _d_, which turns up so constantly? One can imagine the intense interest with which Newton pondered its meaning. Observe the probable outcome of his thought. He had endowed his light-particles with poles, but now he is forced to introduce the notion of _periodic recurrence_. Here his power of transfer from the sensible to the subsensible would render it easy for him to suppose the light-particles animated, not only with a motion of translation, but also with a motion of rotation. Newton's astronomical knowledge rendered all such conceptions familiar to him. The earth has such a double motion. In the time occupied in passing over a million and a half of miles of its orbit--that is, in twenty-four hours--our planet performs a complete rotation; and in the time required to pass over the distance _d_, Newton's light-particle |
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