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**Snell's law** (also known as **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, or air.

In geometric optics, the **angle of incidence** is the angle between a ray incident on a surface and the line perpendicular to the surface at the point of incidence, called the normal. The ray can be formed by any wave: optical, acoustic, microwave, X-ray and so on. In the figure below, the line representing a ray makes an angle θ with the normal. The angle of incidence at which light is first totally internally reflected is known as the critical angle. The angle of reflection and angle of refraction are other angles related to beams.

In physics **refraction** is the change in direction of a wave passing from one medium to another or from a gradual change in the medium. Refraction of light is the most commonly observed phenomenon, but other waves such as sound waves and water waves also experience refraction. How much a wave is refracted is determined by the change in wave speed and the initial direction of wave propagation relative to the direction of change in speed.

In physics, a **wave** is a disturbance that transfers energy through matter or space, with little or no associated mass transport. Waves consist of oscillations or vibrations of a physical medium or a field, around relatively fixed locations. From the perspective of mathematics, waves, as functions of time and space, are a class of signals.

- History
- Explanation
- Derivations and formula
- Derivation from Fermat's principle
- Derivation from Huygens's principle
- Derivation from Maxwell's Equations
- Derivation from conservation of energy and momentum
- Vector form
- Total internal reflection and critical angle
- Dispersion
- Lossy, absorbing, or conducting media
- See also
- References
- External links

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.

In physics, **ray tracing** is a method for calculating the path of waves or particles through a system with regions of varying propagation velocity, absorption characteristics, and reflecting surfaces. Under these circumstances, wavefronts may bend, change direction, or reflect off surfaces, complicating analysis. Ray tracing solves the problem by repeatedly advancing idealized narrow beams called *rays* through the medium by discrete amounts. Simple problems can be analyzed by propagating a few rays using simple mathematics. More detailed analysis can be performed by using a computer to propagate many rays.

In optics, the **refractive index** or **index of refraction** of a material is a dimensionless number that describes how fast light propagates through the material. It is defined as

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:

In mathematics, the **sine** is a trigonometric function of an angle. The sine of an acute angle is defined in the context of a right triangle: for the specified angle, it is the ratio of the length of the side that is opposite that angle to the length of the longest side of the triangle.

The **phase velocity** of a wave is the rate at which the phase of the wave propagates in space. This is the velocity at which the phase of any one frequency component of the wave travels. For such a component, any given phase of the wave will appear to travel at the phase velocity. The phase velocity is given in terms of the wavelength λ (lambda) and time period T as

with each as the angle measured from the normal of the boundary, as the velocity of light in the respective medium (SI units are meters per second, or m/s), as the wavelength of light in the respective medium and 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.

In optics, **Fermat's principle** or the **principle of least time**, named after French mathematician Pierre de Fermat, is the principle that the path taken between two points by a ray of light is the path that can be traversed in the least time. This principle is sometimes taken as the definition of a ray of light. However, this version of the principle is not general; a more modern statement of the principle is that rays of light traverse the path of stationary optical length with respect to variations of the path. In other words, a ray of light prefers the path such that there are other paths, arbitrarily nearby on either side, along which the ray would take almost exactly the same time to traverse.

Ptolemy, a Greek living in Alexandria, Egypt,^{ [1] } 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).^{ [2] } Alhazen, in his * Book of Optics * (1021), came closer to discovering the law of refraction, though he did not take this step.^{ [3] }

**Claudius Ptolemy** was a Greco-Roman mathematician, astronomer, geographer and astrologer. He lived in the city of Alexandria in the Roman province of Egypt, wrote in Koine Greek, and held Roman citizenship. The 14th-century astronomer Theodore Meliteniotes gave his birthplace as the prominent Greek city Ptolemais Hermiou in the Thebaid. This attestation is quite late, however, and, according to Gerald Toomer, the translator of his *Almagest* into English, there is no reason to suppose he ever lived anywhere other than Alexandria. He died there around AD 168.

**Alexandria** is the second-largest city in Egypt and a major economic centre, extending about 32 km (20 mi) along the coast of the Mediterranean Sea in the north central part of the country. Its low elevation on the Nile delta makes it highly vulnerable to rising sea levels. Alexandria is an important industrial center because of its natural gas and oil pipelines from Suez. Alexandria is also a popular tourist destination.

**Confirmation bias**, also called **confirmatory bias** or **myside bias**, is the tendency to search for, interpret, favor, and recall information in a way that confirms one's preexisting beliefs or hypotheses. It is a type of cognitive bias and a systematic error of inductive reasoning. People display this bias when they gather or remember information selectively, or when they interpret it in a biased way. The effect is stronger for emotionally charged issues and for deeply entrenched beliefs. Confirmation bias is a variation of the more general tendency of apophenia.

Although named after Dutch astronomer Willebrord Snellius (1580–1626), the law was first accurately described by the Persian scientist Ibn Sahl ^{[ disputed – discuss ]} 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.^{[ clarification needed ]}^{ [5] }

**Willebrord Snellius** was a Dutch astronomer and mathematician, known in the English-speaking world as **Snell**. In the west, especially the English speaking countries, his name is attached to the law of refraction of light.

**Ibn Sahl** was a Persian mathematician and physicist of the Islamic Golden Age, associated with the Buwayhid court of Baghdad. Nothing in his name allows us to glimpse his country of origin.

**Baghdad** is the capital of Iraq. The population of Baghdad, as of 2016, is approximately 8,765,000, making it the largest city in Iraq, the second largest city in the Arab world, and the second largest city in Western Asia.

The law was rediscovered by Thomas Harriot in 1602,^{ [6] } 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. 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.^{ [7] }^{ [8] } Fermat's derivation also utilized his invention of adequality, a mathematical procedure equivalent to differential calculus, for finding maxima, minima, and tangents.^{ [9] }^{ [10] }

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.^{ [11] }

According to Dijksterhuis,^{ [12] } "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 Snell-Descartes."

In his 1678 * Traité de la Lumière *, 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.

With the development of modern optical and electromagnetic theory, the ancient Snell's law was brought into a new stage. In 1962, Bloembergen showed that at the boundary of nonlinear medium, the Snell's law should be written in a general form.^{ [13] } In 2008 and 2011, plasmonic metasurfaces were also demonstrated to change the reflection and refraction directions of light beam.^{ [14] }^{ [15] }

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 , 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 *o*-ray which follows Snell's law, and the other *extraordinary* or *e*-ray which may not be co-planar 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, and :

Snell's law can be derived in various ways.

Snell's law can 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.

As shown in the figure to the right, assume the refractive index of medium 1 and medium 2 are and respectively. Light enters medium 2 from medium 1 via point O.

is the angle of incidence, is the angle of refraction.

The traveling velocities of light in medium 1 and medium 2 are

- and
- respectively.

is the speed of light in vacuum.

Let T be the time required for the light to travel from point Q to point P.

- (stationary point)

Note that

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.^{ [16] } For example, a homogeneous surface perpendicular to the z direction cannot change the transverse momentum. Since the propagation vector is proportional to the photon's momentum, the transverse propagation direction must remain the same in both regions. Assume without loss of generality a plane of incidence in the plane . Using the well known dependence of the wavenumber on the refractive index of the medium, we derive Snell's law immediately.

where is the wavenumber in vacuum. Although no surface is truly homogeneous at the atomic scale, full translational symmetry is an excellent approximation whenever the region is homogeneous on the scale of the light wavelength.

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 and angle of refraction , without explicitly using the sine values or any trigonometric functions or angles:^{ [17] }

Note: 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 . If is negative, then **n** points to the side without the light, so start over with **n** replaced by its negative.

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:

The formula may appear simpler in terms of renamed simple values and , avoiding any appearance of trig function names or angle names:

Example:

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 , which can only happen for rays crossing into a less-dense medium ().

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.

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

which is impossible to satisfy. The critical angle θ_{crit} is the value of θ_{1} for which θ_{2} equals 90°:

In many wave-propagation 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 color-dependent blurring that sometimes is the resolution-limiting effect. This was especially true in refracting telescopes, before the invention of achromatic objective lenses.

In a conducting medium, permittivity and index of refraction are complex-valued. Consequently, so are the angle of refraction and the wave-vector. 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.^{ [18] } The refracted wave is exponentially attenuated, with exponent proportional to the imaginary component of the index of refraction.^{ [19] }^{ [20] }

- List of refractive indices
- The refractive index vs wavelength of light
- Evanescent wave
- Reflection (physics)
- Snell's window
- Calculus of variations
- Brachistochrone curve for a simple proof by Jacob Bernoulli
- Hamiltonian optics
- Computation of radiowave attenuation in the atmosphere
- Shore line effect
- N-slit interferometric equation

- ↑ David Michael Harland (2007). "
*Cassini at Saturn: Huygens results*". p.1. ISBN 0-387-26129-X - ↑ "Ptolemy (ca. 100-ca. 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. - ↑ Rashed, Roshdi (1990). "A pioneer in anaclastics: Ibn Sahl on burning mirrors and lenses".
*Isis*.**81**(3): 464–491. doi:10.1086/355456. - ↑ Kwan, A.; Dudley, J.; Lantz, E. (2002). "Who really discovered Snell's law?".
*Physics World*.**15**(4): 64. doi:10.1088/2058-7058/15/4/44. - ↑ 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).
- ↑ Dijksterhuis, Fokko Jan (2004).
*Lenses and Waves: Christiaan Huygens and the Mathematical Science of Optics in the Seventeenth Century*. Springer. ISBN 1-4020-2697-8. - ↑ Bloembergen, N.; Pershan, P. S. (1962). "Light waves at the boundary of nonlinear media" (PDF).
*Physical Review*.**128**: 606. Bibcode:1962PhRv..128..606B. doi:10.1103/PhysRev.128.606. - ↑ Xu, T.; et al. (2008). "Plasmonic deflector".
*Opt. Express*.**16**: 4753. Bibcode:2008OExpr..16.4753X. doi:10.1364/oe.16.004753. - ↑ Yu, Nanfang; Genevet, Patrice; Kats, Mikhail A.; Aieta, Francesco; Tetienne, Jean-Philippe; Capasso, Federico; Gaburro, Zeno (October 2011). "Light Propagation with Phase Discontinuities: Generalized Laws of Reflection and Refraction".
*Science*.**334**(6054): 333. Bibcode:2011Sci...334..333Y. doi:10.1126/science.1210713. PMID 21885733. - ↑ Joannopoulos, John D; Johnson, SG; Winn, JN; Meade, RD (2008).
*Photonic Crystals: Molding the Flow of Light*(2nd ed.). Princeton NJ: Princeton University Press. ISBN 978-0-691-12456-8. - ↑ Glassner, Andrew S. (1989).
*An Introduction to Ray Tracing*. Morgan Kaufmann. ISBN 0-12-286160-4. - ↑ 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,

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