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Brewster's angle

From Biocrawler, the free encyclopedia.

An illustration of the polaristion of light which is incident on an interface at Brewster's angle.
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An illustration of the polaristion of light which is incident on an interface at Brewster's angle.

Brewster's angle (also known as Polarization angle) is an optical phenomenon first discovered by the Scottish Physicist, Sir David Brewster (1781-1868).

When light moves between two media of differing refractive index, light which is p-polarised with respect to the interface will not be reflected from the interface at one particular incident angle, known as Brewster's angle.

It may be calculated by:

\theta_B = \arctan \left( \frac{n_2}{n_1} \right),

where n1 and n2 are the refractive indices of the two media.

Note that, since all p-polarised light is refracted, any light reflected from the interface at this angle must be s-polarised. A glass plate placed at Brewster's angle in a light beam can thus be used as a polariser.

For a randomly polarized ray incident at Brewster's angle, the reflected and refracted rays are at 90° with respect to one another.

For a glass medium (n2≈1.5) in air (n1≈1), Brewster's angle for visible light is approximately 56° to the normal. The refractive index for a given medium changes depending on the wavelength of light, but typically does not vary much. The difference in the refractive index between ultra violet (≈100nm) and infra red (≈1000nm) in glass, for example, is ≈0.01.

See also:

fr:Angle de Brewster

Wikipedia (http://en.wikipedia.org/wiki/Main_Page) Brewster's_angle (http://en.wikipedia.org/wiki/Brewster's_angle) version history (http://en.wikipedia.org/w/index.php?title=Brewster's_angle&action=history) GNU Free Documentation Lizenz (http://en.wikipedia.org/wiki/Wikipedia:Text_of_the_GNU_Free_Documentation_License) CC-by-sa (http://creativecommons.org/licenses/by-sa/2.5/)

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