Calculate the polarisation angle (Brewster's angle) for light travelling between any two optical media. At Brewster's angle, reflected light is completely s-polarised and no p-polarised component is reflected.
Enter the refractive indices of both media, or choose a common preset, to get the Brewster angle in degrees instantly.
The refractive index (n) of a medium is the ratio of the speed of light in a vacuum to the speed of light in that medium. Air is approximately 1.000, water is 1.333, and common glass ranges from 1.45 to 1.9 depending on type.
Brewster's angle is measured from the normal (perpendicular) to the surface, not from the surface itself.
At Brewster's angle, the refracted and reflected rays are at exactly 90 degrees to each other.
Brewster's angle (symbol theta_B, also called the polarisation angle) is named after Scottish physicist Sir David Brewster, who discovered it experimentally in 1815. It is the angle of incidence at which light travelling between two dielectric (non-conducting) media produces a reflected ray that is completely polarised in the s-direction (perpendicular to the plane of incidence). At this angle, no p-polarised (parallel) component appears in the reflected ray; it is entirely transmitted into the second medium.
The physical reason is that p-polarised oscillating dipoles in the second medium, when aligned in the direction of the reflected beam, cannot radiate energy in that direction. This only occurs when the reflected and refracted rays are exactly 90 degrees apart, which is the geometric condition that Brewster's Law captures.
Brewster's Law states:
tan(θB) = n2 / n1
where n1 is the refractive index of the incident medium (the medium the light is coming from) and n2 is the refractive index of the transmitted medium (the medium the light is entering). Rearranging gives:
θB = arctan(n2 / n1)
At Brewster's angle, the refracted angle satisfies Snell's Law (n1 sin(θB) = n2 sin(θr)), and the two angles sum to exactly 90 degrees: theta_B + theta_r = 90 degrees.
For light passing from air (n1 = 1.000) into ordinary crown (window) glass (n2 = 1.500):
This matches the calculator's default output for the air-to-glass preset.
| Media (n1 to n2) | n1 | n2 | Brewster's Angle |
|---|---|---|---|
| Air to water | 1.000 | 1.333 | 53.12 deg |
| Air to glass (n=1.5) | 1.000 | 1.500 | 56.31 deg |
| Air to fused silica | 1.000 | 1.460 | 55.60 deg |
| Air to diamond | 1.000 | 2.417 | 67.52 deg |
| Water to glass | 1.333 | 1.500 | 48.37 deg |
| Glass to air (internal) | 1.500 | 1.000 | 33.69 deg |
Note that the Brewster angle for glass-to-air is exactly 90 minus the air-to-glass Brewster angle (33.69 + 56.31 = 90). This is because n2/n1 is the reciprocal in each direction, and arctan(x) + arctan(1/x) = 90 degrees for any positive x.
Method and sources: Formula: theta_B = arctan(n2/n1), from Brewster's Law (1815). Refractive index values from the NIST Handbook of Optical Constants and CRC Handbook of Chemistry and Physics. The relationship theta_B + theta_r = 90 deg follows from Snell's Law and is the geometric basis of complete polarisation at this angle.
This calculator assumes monochromatic light and non-absorbing (dielectric) media. Refractive indices are wavelength-dependent; for precise work use n values at your specific wavelength. Metals and other absorbing media require a complex refractive index treatment and do not produce a simple Brewster angle.
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