202
DOUBLE REFRACTION AND CIRCULAR POLARIZATION
If we set
![{\displaystyle a={\frac {\text{A}}{2\pi }}-{\frac {2\pi {\text{A}}'}{p^{2}}},}](https://wikimedia.org/api/rest_v1/media/math/render/svg/37ba6c4b28b9ca10ef4a1f98c5dbf7f8ddca56bc) etc.,
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(14)
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and
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(15)
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the equation reduces to
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(16)
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where
are constant, and
a quadratic function of
for a given medium and light of a given period.
13. Now this equation, which expresses a relation between the constants of the equations of wave-motion (1), will apply, with those equations, not only to such vibrations as actually take place, but also to such as we may imagine to take place under the influence of constraints determining the type of vibration. The free or unconstrained vibrations, with which alone we are concerned, are characterized by this, that infinitesimal variations (by constraint) of the type of vibration, that is, of the ratios of the quantities
will not affect the period by any quantity of the same order of magnitude.[1] These variations must however be consistent with equations (4), which require that
![{\displaystyle {\text{L }}d\alpha _{1}+{\text{M }}d\beta _{1}+{\text{N }}d\gamma _{1}=0,}](https://wikimedia.org/api/rest_v1/media/math/render/svg/ed8a40bdb90cd4572a8cc29e68a3b10c8aa7610f)
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(17)
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Hence, to obtain the conditions which characterize free vibration, we may differentiate equation (16) with respect to
regarding all other letters as constant, and give to
such values as are consistent with equations (17). Now
are independent of
and for either three variations, values proportional either to
or to
are possible. If, then, we differentiate equation (16) with respect to
and substitute first
and then
for
and also differentiate with respect to
with similar substitutions, we shall obtain all the independent equations which this principle will yield.
If we differentiate with respect to
and write
for
we obtain
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(18)
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- ↑ Compare § 11 of the former paper, page 189 of this volume.