Refraction of light at the interface between two media of different
refractive indices, with n
_{2} > n
_{1}. Since the velocity is lower in the second medium (v
_{2} < v
_{1}), the angle of refraction θ
_{2} is less than the angle of incidence θ
_{1}; that is, the ray in the higherindex medium is closer to the normal.
Snell's law (also known as the Snell–Descartes law and the law of refraction) is a formula used to describe the relationship between the angles of incidence and refraction, when referring to light or other waves passing through a boundary between two different isotropic media, such as water, glass and air.
In optics, the law is used in ray tracing to compute the angles of incidence or refraction, and in experimental optics to find the refractive index of a material. The law is also satisfied in metamaterials, which allow light to be bent "backward" at a negative angle of refraction with a negative refractive index.
Although named after Dutch astronomer Willebrord Snellius (1580–1626), the law was first accurately described by the scientist Ibn Sahl at the Baghdad court in 984. In the manuscript On Burning Mirrors and Lenses, Sahl used the law to derive lens shapes that focus light with no geometric aberrations.^{[1]}^{[2]}
Snell's law states that the ratio of the sines of the angles of incidence and refraction is equivalent to the ratio of phase velocities in the two media, or equivalent to the reciprocal of the ratio of the indices of refraction:

\frac{\sin\theta_1}{\sin\theta_2} = \frac{v_1}{v_2} = \frac{n_2}{n_1}
with each \theta as the angle measured from the normal of the boundary, v as the velocity of light in the respective medium (SI units are meters per second, or m/s) and n as the refractive index (which is unitless) of the respective medium.
The law follows from Fermat's principle of least time, which in turn follows from the propagation of light as waves.
Contents

History 1

Explanation 2

Derivations and formula 3

Total internal reflection and critical angle 4

Dispersion 5

Lossy, absorbing, or conducting media 6

See also 7

References 8

External links 9
History
Reproduction of a page of
Ibn Sahl's manuscript showing his discovery of the law of refraction.
Ptolemy, a Greek living in Alexandria, Egypt,^{[3]} had found a relationship regarding refraction angles, but it was inaccurate for angles that were not small. Ptolemy was confident he had found an accurate empirical law, partially as a result of fudging his data to fit theory (see: confirmation bias).^{[4]} Alhazen, in his Book of Optics (1021), came closer to discovering the law of refraction, though he did not take this step.^{[5]}
An 1837 view of the history of "the Law of the Sines"^{[6]}
The law of refraction was first accurately described by Ibn Sahl, of Baghdad, in the manuscript On Burning Mirrors and Lenses (984).^{[1]}^{[2]} He made use of it to work out the shapes of lenses that focus light with no geometric aberrations, known as anaclastic lenses.^{[7]}
The law was rediscovered by Thomas Harriot in 1602,^{[8]} who however did not publish his results although he had corresponded with Kepler on this very subject. In 1621, Willebrord Snellius (Snell) derived a mathematically equivalent form, that remained unpublished during his lifetime. René Descartes independently derived the law using heuristic momentum conservation arguments in terms of sines in his 1637 essay Dioptrics, and used it to solve a range of optical problems. Rejecting Descartes' solution, Pierre de Fermat arrived at the same solution based solely on his principle of least time. Interestingly, Descartes assumed the speed of light was infinite, yet in his derivation of Snell's law he also assumed the denser the medium, the greater the speed of light. Fermat supported the opposing assumptions, i.e., the speed of light is finite, and his derivation depended upon the speed of light being slower in a denser medium.^{[9]}^{[10]} Fermat's derivation also utilized his invention of adequality, a mathematical procedure equivalent to differential calculus, for finding maxima, minima, and tangents.^{[11]}^{[12]}
In his influential mathematics book Geometry, Descartes solves a problem that was worked on by Apollonius of Perga and Pappus of Alexandria. Given n lines L and a point P(L) on each line, find the locus of points Q such that the lengths of the line segments QP(L) satisfy certain conditions. For example, when n = 4, given the lines a, b, c, and d and a point A on a, B on b, and so on, find the locus of points Q such that the product QA*QB equals the product QC*QD. When the lines are not all parallel, Pappus showed that the loci are conics, but when Descartes considered larger n, he obtained cubic and higher degree curves. To show that the cubic curves were interesting, he showed that they arose naturally in optics from Snell's law.^{[13]}
According to Dijksterhuis,^{[14]} "In De natura lucis et proprietate (1662) Isaac Vossius said that Descartes had seen Snell's paper and concocted his own proof. We now know this charge to be undeserved but it has been adopted many times since." Both Fermat and Huygens repeated this accusation that Descartes had copied Snell. In French, Snell's Law is called "la loi de Descartes" or "loi de SnellDescartes."
In his 1678 Traité de la Lumiere, Christiaan Huygens showed how Snell's law of sines could be explained by, or derived from, the wave nature of light, using what we have come to call the Huygens–Fresnel principle.
Explanation
Snell's law is used to determine the direction of light rays through refractive media with varying indices of refraction. The indices of refraction of the media, labeled n_1, n_2 and so on, are used to represent the factor by which a light ray's speed decreases when traveling through a refractive medium, such as glass or water, as opposed to its velocity in a vacuum.
As light passes the border between media, depending upon the relative refractive indices of the two media, the light will either be refracted to a lesser angle, or a greater one. These angles are measured with respect to the normal line, represented perpendicular to the boundary. In the case of light traveling from air into water, light would be refracted towards the normal line, because the light is slowed down in water; light traveling from water to air would refract away from the normal line.
Refraction between two surfaces is also referred to as reversible because if all conditions were identical, the angles would be the same for light propagating in the opposite direction.
Snell's law is generally true only for isotropic or specular media (such as glass). In anisotropic media such as some crystals, birefringence may split the refracted ray into two rays, the ordinary or oray which follows Snell's law, and the other extraordinary or eray which may not be coplanar with the incident ray.
When the light or other wave involved is monochromatic, that is, of a single frequency, Snell's law can also be expressed in terms of a ratio of wavelengths in the two media, λ_{1} and λ_{2}:

\frac{\sin\theta_1}{\sin\theta_2} = \frac{v_1}{v_2} = \frac{\lambda_1}{\lambda_2}
Derivations and formula
Snell's law may be derived from Fermat's principle, which states that the light travels the path which takes the least time. By taking the derivative of the optical path length, the stationary point is found giving the path taken by the light (though it should be noted that the result does not show light taking the least time path, but rather one that is stationary with respect to small variations as there are cases where light actually takes the greatest time path, as in a spherical mirror). In a classic analogy, the area of lower refractive index is replaced by a beach, the area of higher refractive index by the sea, and the fastest way for a rescuer on the beach to get to a drowning person in the sea is to run along a path that follows Snell's law.
Alternatively, Snell's law can be derived using interference of all possible paths of light wave from source to observer—it results in destructive interference everywhere except extrema of phase (where interference is constructive)—which become actual paths.
Another way to derive Snell’s Law involves an application of the general boundary conditions of Maxwell equations for electromagnetic radiation.
Yet another way to derive Snell's law is based on translation symmetry considerations.^{[15]} For example, a homogeneous surface perpendicular to the z direction cannot change the transverse momentum. Since the propagation vector \vec{k} is proportional to the photon's momentum, the transverse propagation direction (k_x,k_y,0) must remain the same in both regions. Assuming without loss of generality a plane of incidence in the z,x plane k_{x\text{Region}_1} = k_{x\text{Region}_2}. Using the well known dependence of the wave number on the refractive index of the medium, we derive Snell's law immediately.

k_{x\text{Region}_1} = k_{x\text{Region}_2} \,

n_1 k_0\sin\theta_1 = n_2 k_0\sin\theta_2 \,

n_1\sin\theta_1 = n_2\sin\theta_2 \,
where k_0=\frac{2\pi}{\lambda_0}=\frac{\omega}{c} is the wavenumber in vacuum. Note that no surface is truly homogeneous, in the least at the atomic scale. Yet full translational symmetry is an excellent approximation whenever the region is homogeneous on the scale of the light wavelength.
Vector form
Given a normalized light vector l (pointing from the light source toward the surface) and a normalized plane normal vector n, one can work out the normalized reflected and refracted rays, via the cosines of the angle of incidence \theta_1 and angle of refraction \theta_2, without explicitly using the sine values or any trigonometric functions or angles:^{[16]}

\cos\theta_1 = \mathbf{n}\cdot \mathbf{l}
Note: \cos\theta_1 must be positive, which it will be if n is the normal vector that points from the surface toward the side where the light is coming from, the region with index n_1. If \cos\theta_1 is negative, then n points to the side without the light, so start over with n replaced by its negative.

\mathbf{v}_{\mathrm{reflect}}=\mathbf{l} + 2\cos\theta_1 \mathbf{n}
This reflected direction vector points back toward the side of the surface where the light came from.
Now apply Snell's law to the ratio of sines to derive the formula for the refracted ray's direction vector:

\sin\theta_2 = \left(\frac{n_1}{n_2}\right) \sin\theta_1 = \left( \frac{n_1}{n_2} \right) \sqrt{ 1  \left(\cos\theta_1 \right)^2 }

\cos\theta_2 = \sqrt{1\sin\theta_2^2} = \sqrt{1  \left( \frac{n_1}{n_2} \right)^2 \left( 1  \left( \cos\theta_1 \right)^2 \right)}

\mathbf{v}_{\mathrm{refract}} = \left( \frac{n_1}{n_2} \right) \mathbf{l} + \left( \frac{n_1}{n_2} \cos\theta_1  \cos\theta_2 \right) \mathbf{n}
The formula may appear simpler in terms of renamed simple values r = n_1 / n_2 and c = \mathbf{n}\cdot \mathbf{l}, avoiding any appearance of trig function names or angle names:

\mathbf{v}_{\mathrm{refract}} = r \mathbf{l} + \left( r c  \sqrt{1  r^2 \left( 1  c^2 \right)} \right) \mathbf{n}
Example:

\mathbf{l} = \{0.707107, 0.707107\}, ~ \mathbf{n} = \{0,1\}, ~ r = \frac{n_1}{n_2} = 0.9

c = \cos\theta_1=0.707107, ~ \sqrt{1  r^2 \left( 1  c^2 \right)} = \cos\theta_2 = 0.771362

\mathbf{v}_{\mathrm{reflect}}=\{0.707107, 0.707107\} ,~\mathbf{v}_{\mathrm{refract}}=\{0.636396, 0.771362\}
The cosine values may be saved and used in the Fresnel equations for working out the intensity of the resulting rays.
Total internal reflection is indicated by a negative radicand in the equation for \cos\theta_2, which can only happen for rays crossing into a lessdense medium ( n_2 < n_1).
Total internal reflection and critical angle
Demonstration of no refraction at angles greater than the critical angle.
When light travels from a medium with a higher refractive index to one with a lower refractive index, Snell's law seems to require in some cases (whenever the angle of incidence is large enough) that the sine of the angle of refraction be greater than one. This of course is impossible, and the light in such cases is completely reflected by the boundary, a phenomenon known as total internal reflection. The largest possible angle of incidence which still results in a refracted ray is called the critical angle; in this case the refracted ray travels along the boundary between the two media.
Refraction of light at the interface between two media.
For example, consider a ray of light moving from water to air with an angle of incidence of 50°. The refractive indices of water and air are approximately 1.333 and 1, respectively, so Snell's law gives us the relation

\sin\theta_2 = \frac{n_1}{n_2}\sin\theta_1 = \frac{1.333}{1}\cdot\sin\left(50^\circ\right) = 1.333\cdot 0.766 = 1.021,
which is impossible to satisfy. The critical angle θ_{crit} is the value of θ_{1} for which θ_{2} equals 90°:

\theta_\text{crit} = \arcsin\left(\frac{n_2}{n_1}\sin\theta_2\right) = \arcsin\frac{n_2}{n_1} = 48.6^\circ.
Dispersion
In many wavepropagation media, wave velocity changes with frequency or wavelength of the waves; this is true of light propagation in most transparent substances other than a vacuum. These media are called dispersive. The result is that the angles determined by Snell's law also depend on frequency or wavelength, so that a ray of mixed wavelengths, such as white light, will spread or disperse. Such dispersion of light in glass or water underlies the origin of rainbows and other optical phenomena, in which different wavelengths appear as different colors.
In optical instruments, dispersion leads to chromatic aberration; a colordependent blurring that sometimes is the resolutionlimiting effect. This was especially true in refracting telescopes, before the invention of achromatic objective lenses.
Lossy, absorbing, or conducting media
In a conducting medium, permittivity and index of refraction are complexvalued. Consequently, so are the angle of refraction and the wavevector. This implies that, while the surfaces of constant real phase are planes whose normals make an angle equal to the angle of refraction with the interface normal, the surfaces of constant amplitude, in contrast, are planes parallel to the interface itself. Since these two planes do not in general coincide with each other, the wave is said to be inhomogeneous.^{[17]} The refracted wave is exponentially attenuated, with exponent proportional to the imaginary component of the index of refraction.^{[18]}^{[19]}
See also
References

^ ^{a} ^{b} Wolf, K. B. (1995), "Geometry and dynamics in refracting systems", European Journal of Physics 16: 14–20.

^ ^{a} ^{b} Rashed, Roshdi (1990). "A pioneer in anaclastics: Ibn Sahl on burning mirrors and lenses".

^ David Michael Harland (2007). "Cassini at Saturn: Huygens results". p.1. ISBN 038726129X

^ "Ptolemy (ca. 100ca. 170)". Eric Weinstein's World of Scientific Biography.

^ A. I. Sabra (1981), Theories of Light from Descartes to Newton, Cambridge University Press. (cf. Pavlos Mihas, Use of History in Developing ideas of refraction, lenses and rainbow, p. 5, Demokritus University, Thrace, Greece.)

^ William Whewell, History of the Inductive Science from the Earliest to the Present Times, London: John H. Parker, 1837.

^ Sara Cerantola, "La ley física de Ibn Sahl: estudio y traducción parcial de su Kitāb alḥarraqāt / The physics law of Ibn Sahl: Study and partial translation of his Kitāb alḥarraqāt", Anaquel de Estudios Árabes, 15 (2004): 5795.

^ Kwan, A., Dudley, J., and Lantz, E. (2002). "Who really discovered Snell's law?".

^ Florian Cajori, A History of Physics in its Elementary Branches: Including the Evolution of Physical Laboratories (1922)

^ Ferdinand Rosenberger, Geschichte der Physik (1882) Part. II, p.114

^ Carl Benjamin Boyer, The Rainbow: From Myth to Mathematics (1959)

^ Florian Cajori, "Who was the First Inventor of Calculus" The American Mathematical Monthly (1919) Vol.26

^ The Geometry of Rene Descartes (Dover Books on Mathematics) by Rene Descartes, David Eugene Smith and Marcia L. Latham (Jun 1, 1954).

^ Fokko Jan Dijksterhuis (2004). Lenses and Waves: Christiaan Huygens and the Mathematical Science of Optics in the Seventeenth Century. Springer.

^ John D Joannopoulos, Johnson SG, Winn JN & Meade RD (2008). Photonic Crystals: Molding the Flow of Light (2nd ed.). Princeton NJ: Princeton University Press.

^ Andrew S. Glassner (1989). An Introduction to Ray Tracing. Morgan Kaufmann.

^ Born and Wolf, sec.13.2, "Refraction and reflection at a metal surface"

^ Hecht, Optics, sec. 4.8, Optical properties of metals.

^ S. J. Orfanidis, Electromagnetic Waves & Antennas, sec. 7.9, Oblique Incidence on a Lossy Medium, [1]
External links
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