A Treatise On Physical Optics
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Let OP be the direction of vibration of the incident light, so that if the light is polarized by a Nicol, OP is its principal section ; and let OS be the principal section of the analyser. Let PO A = a, POS /3 ; also let the vibration which is incident upon the crystal be represented by sin 27r/T.
B On entering the crystal, the incident vibration is resolved into cos a sin 2?r^/T along OA, which constitutes the extraordinary ray, and sin a sin %7rt/r along OB, which constitutes the ordinary ray.... The waves corre- sponding to these rays travel through the crystal with different velocities, and therefore on emergence, the two vibrations may be written ^oA ~->$3 W^. - fi. 6 ***, cos a sin 2?r (t/r Ej\) t and sin a sin 2?r (t/r 0/\) where X is the wave length in air, and and E are the thicknesses of two laminae of air, such that light would occupy the same times in traversing them, as are occupied by the ordinary and extra- ordinary waves in traversing the crystalline plate.
On entering the analyser, only those vibrations can pass through which are parallel to OS] whence resolving the two vibrations in INTENSITY OF EMERGENT LIGHT.
What to read after A Treatise On Physical Optics?
You can find similar books in the "Read Also" column, or choose other free books by Alfred Barnard Basset to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
Let OP be the direction of vibration of the incident light, so that if the light is polarized by a Nicol, OP is its principal section ; and let OS be the principal section of the analyser. Let PO A = a, POS /3 ; also let the vibration which is incident upon the crystal be represented by sin 27r/T.
B On entering the crystal, the incident vibration is resolved into cos a sin 2?r^/T along OA, which constitutes the extraordinary ray, and sin a sin %7rt/r along OB, which constitutes the ordinary ray.... The waves corre- sponding to these rays travel through the crystal with different velocities, and therefore on emergence, the two vibrations may be written ^oA ~->$3 W^. - fi. 6 ***, cos a sin 2?r (t/r Ej\) t and sin a sin 2?r (t/r 0/\) where X is the wave length in air, and and E are the thicknesses of two laminae of air, such that light would occupy the same times in traversing them, as are occupied by the ordinary and extra- ordinary waves in traversing the crystalline plate.
On entering the analyser, only those vibrations can pass through which are parallel to OS] whence resolving the two vibrations in INTENSITY OF EMERGENT LIGHT.
What to read after A Treatise On Physical Optics?
You can find similar books in the "Read Also" column, or choose other free books by Alfred Barnard Basset to read onlineMoreLess
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