Snell's law
physics
in optics, a relationship between the path taken by a ray of light in crossing the boundary or surface of separation between two contacting substances and the refractive index (q.v.) of each. This law was discovered in 1621 by the Dutch astronomer and mathematician Willebrord van Roijen Snell (Snell, Willebrord van Roijen) (1580–1626; also called Snellius). The account of Snell's law went unpublished until its mention by Christiaan Huygens in his treatise on light.
![](Images/eb/pics/I4205.jpg)
In the Figure-->
![](Images/eb/pics/I4205.jpg)
,
n1 and
n2 represent the indices of refraction for the two media, and
α1 and
α2 are the angles of incidence and refraction that the ray
R makes with the normal (perpendicular) line
NN at the boundary. Snell's law asserts that
n1/
n2 = sin
α2/sin
α1.
Because the ratio n1/n2 is a constant for any given wavelength of light, the ratio of the two sines is also a constant for any angle. Thus, the path of a light ray is bent toward the normal when the ray enters a substance with an index of refraction higher than the one from which it emerges; and because the path of a ray of light is reversible, the ray is bent away from the normal when bgtering a substance of lower refractive index.
![](Images/eb/pics/I4205.jpg)
The reason light is refracted in going from one medium to another is shown in the Figure-->
![](Images/eb/pics/I4205.jpg)
. According to Huygens' principle, each point on a wave front of light is a source of new wavelets. A parallel beam, consisting of the three rays
R1,
R2, and
R3, is incident on a boundary plane
AF separating two media of indices
n1 and
n2, and it has a plane wave front
ABC. In this example, the speed of light is greater in the first medium than in the second (
n1 is less than
n2). Consequently, according to Huygens' principle, the radius of the wavelets in the first medium is greater than the radius in the second. By the time a point
C on the wave front
ABC has moved from
C to
F on the plane, the point
A of the wave front has moved a distance of only
AD in the second medium. A plane
DEF tangent to the new wavelets represents the new wave front, and lines perpendicular to it represent the paths taken by the rays in the second medium.