Six Lectures on Light: Delivered In The United States In 1872-1873Tyndall, John
Science
Six Lectures on Light: Delivered In The United States In 1872-1873
Tyndall, John
Light
With profound sagacity, Fresnel, to whose genius we mainly owe the
expansion and final triumph of the undulatory theory of light,
reproduced mentally the mechanism of these crystals, and showed their
action to be due to the circumstance that, in them, the waves of
ether so act upon each other as to produce the condition represented
by our rotating pendulum. Instead of being plane polarized, the light
in rock crystal is _circularly polarized_. Two such rays, transmitted
along the axis of the crystal, and rotating in opposite directions,
when brought to interference by the analyzer, are demonstrably
competent to produce all the observed phenomena.
§ 7. _Complementary Colours of Bi-refracting Spar in Circularly
Polarized Light. Proof that Yellow and Blue are Complementary._
I now remove the analyzer, and put in its place the piece of Iceland
spar with which we have already illustrated double refraction. The two
images of the carbon-points are now before you, produced, as you know,
by two beams vibrating at right angles to each other. Introducing a
plate of quartz between the polarizer and the spar, the two images
glow with complementary colours. Employing the image of an aperture
instead of that of the carbon-points, we have two coloured circles. As
the analyzer is caused to rotate, the colours pass through various
changes: but they are always complementary. When the one is red, the
other is green; when the one is yellow, the other is blue. Here we
have it in our power to demonstrate afresh a statement made in our
first lecture, that although the mixture of blue and yellow pigments
produces green, the mixture of blue and yellow lights produces white.
By enlarging our aperture, the two images produced by the spar are
caused to approach each other, and finally to overlap. The one image
is now a vivid yellow, the other a vivid blue, and you notice that
where these colours are superposed we have a pure white. (See fig. 43,
where N is the end of the polarizer, Q the quartz plate, L a lens, and
B the bi-refracting spar. The two images overlap at O, and produce
white by their mixture.)
[Illustration: Fig. 43.]
§ 8. _The Magnetization of Light._
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