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
But here, as in the case of thin films, the different lengths of the
waves of light come into play. Red will require a greater thickness to
produce the retardation necessary for extinction than blue;
consequently when the longer waves have been withdrawn by
interference, the shorter ones remain, the film of gypsum shining with
the colours which the short waves confer. Conversely, when the shorter
waves have been withdrawn, the thickness is such that the longer waves
remain. An elementary consideration suffices to show, that when the
directions of vibration of the prisms and the gypsum enclose an angle
of forty-five degrees, the colours are at their maximum brilliancy.
When the film is turned from this direction, the colours gradually
fade, until, at the point where the directions of vibration in plate
and prisms are parallel, they disappear altogether.
(The best way of obtaining a knowledge of these phenomena is to
construct a model of thin wood or pasteboard, representing the plate
of gypsum, its planes of vibration, and also those of the polarizer
and analyzer. Two parallel pieces of the board are to be separated by
an interval which shall represent the thickness of the film of gypsum.
Between them two other pieces, intersecting each other at a right
angle, are to represent the planes of vibration within the film; while
attached to the two parallel surfaces outside are two other pieces of
board, which represent the planes of vibration of the polarizer and
analyzer. On the two intersecting planes the waves are to be drawn,
showing the resolution of the first polarized beam into two others,
and then the subsequent reduction of the two systems of vibrations to
a common plane by the analyzer. Following out rigidly the interaction
of the two systems of waves, we are taught by such a model that all
the phenomena of colour obtained by the combination of the waves, when
the planes of vibration of the two Nicols are parallel, are displaced
by the _complementary_ phenomena, when the planes of vibration are
perpendicular to each other.)
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