Difference between revisions of "Refraction" - New World Encyclopedia

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[[Image:Refraction-with-soda-straw.jpg|thumb|200px|The straw seems to be broken, due to refraction of light as it emerges into the air.]]
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[[Image:Refraction-with-soda-straw.jpg|thumb|200px|A straw dipped in a colored solution appears to be broken, because of the refraction of light as it passes from the solution to the air.]]
{{For|the property of metals|refraction (metallurgy)}}
 
  
'''Refraction''' is the change in direction of a [[wave]] due to a change in its [[speed]]. This is most commonly seen when a wave passes from one [[optical medium|medium]] to another. Refraction of [[light]] is the most commonly seen example, but any type of wave can refract when it interacts with a medium, for example when [[sound wave]]s pass from one medium into another.
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'''Refraction''' is the change in direction of a [[wave]] due to a change in its [[speed]], as observed when a wave passes from one [[optical medium|medium]] to another. The most common example is the refraction of [[light]], as happens in the formation of [[rainbow]]s in the sky or rainbow-like bands when white light passes through a glass [[triangular prism (optics)|prism]]. Other types of waves also undergo refraction, for example, when [[sound wave]]s pass from one medium into another.
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The refraction of waves through a medium is quantified in terms of what is called the '''refractive index''' (or '''index of [[refraction]]'''). The refractive index of a medium is a measure of how much the speed of light (or other waves) is reduced inside the medium, compared with the speed of light in vacuum or air. For example, if a sample of [[glass]] has a refractive index of 1.5, it means that the speed of light traveling through the glass is <math>1/1.5=0.67</math> times the speed of light in vacuum or air.
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{{toc}}
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Based on knowledge of the properties of refraction and refractive index, a number of applications have been developed. For example, the invention of [[lens (optics)|lens]]es and [[refracting telescope]]s rests on an understanding of refraction. Also, knowledge of the refractive index of various substances is used to evaluate the purity of a substance or measure its concentration in a mixture. In eye tests performed by [[ophthalmology|ophthalmologists]] or [[optometry|optometrists]], the property of refraction forms the basis for the technique known as ''refractometry.''
  
 
==Explanation==
 
==Explanation==
  
In [[optics]], refraction occurs when [[light wave]]s travel from a medium with a given [[refractive index]] to a medium with another. At the boundary between the media, the wave's [[phase velocity]] is altered, it changes direction, and its [[wavelength]] increases or decreases but its [[frequency]] remains constant. For example, a [[ray (optics)|light ray]] will refract as it enters and leaves [[glass]]; understanding of this concept led to the [[invention]] of [[lens (optics)|lens]]es and the [[refracting telescope]].  
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In [[optics]], refraction occurs when [[light wave]]s travel from a medium with a particular [[#Refractive index|refractive index]] to a second medium with another refractive index. At the boundary between the media, the wave's [[phase velocity]] is altered, it changes direction, and its [[wavelength]] increases or decreases, but its [[frequency]] remains constant. For example, a [[ray (optics)|light ray]] will undergo refraction as it enters and leaves [[glass]]. An understanding of this concept led to the [[invention]] of [[lens (optics)|lens]]es and the [[refracting telescope]].
  
 
[[Image:Pencil in a bowl of water.png|left|frame|Refraction of light waves in water. The dark rectangle represents the actual position of a pencil sitting in a bowl of water. The light rectangle represents the apparent position of the pencil. Notice that the end (X) looks like it is at (Y), a position that is considerably shallower than (X).]]
 
[[Image:Pencil in a bowl of water.png|left|frame|Refraction of light waves in water. The dark rectangle represents the actual position of a pencil sitting in a bowl of water. The light rectangle represents the apparent position of the pencil. Notice that the end (X) looks like it is at (Y), a position that is considerably shallower than (X).]]
  
Refraction can be seen when looking into a bowl of water. Air has a refractive index of about 1.0003, and water has a refractive index of about 1.33. If a person looks at a straight object, such as a pencil or straw, which is placed at a slant, partially in the water, the object appears to bend at the water's surface. This is due to the bending of light rays as they move from the water to the air. Once the rays reach the eye, the eye traces them back as straight lines (lines of sight). The lines of sight (shown as dashed lines) intersect at a higher position than where the actual rays originated. This causes the pencil to appear higher and the water to appear shallower than it really is. The depth that the water appears to be when viewed from above is known as the ''apparent depth''.
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Refraction can be seen when looking into a bowl of water. Air has a refractive index of about 1.0003, and water has a refractive index of about 1.33. If a person looks at a straight object, such as a pencil or straw, which is placed at a slant, partially in the water, the object appears to bend at the water's surface. This is due to the bending of light rays as they move from the water to the air. Once the rays reach the eye, the eye traces them back as straight lines (lines of sight). The lines of sight (shown as dashed lines) intersect at a higher position than where the actual rays originated. This causes the pencil to appear higher and the water to appear shallower than it really is. The depth that the water appears to be when viewed from above is known as the ''apparent depth,''
  
 
[[Image:Refraction in a ripple tank.png|thumb|Diagram of refraction of water waves]]
 
[[Image:Refraction in a ripple tank.png|thumb|Diagram of refraction of water waves]]
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== Refractive index ==
 
== Refractive index ==
<<The definition given here needs to be simplified, and technical terms need to be replaced or explained, for the benefit of lay readers.>>
 
  
The '''refractive index''' (or '''index of [[refraction]]''') of a medium is the inverse ratio of the [[phase velocity]] of a [[wave]] phenomenon such as [[light]] or [[sound]] and the phase velocity in a reference medium. It is most commonly used in the context of [[light]] with [[vacuum]] as a reference medium, although historically other reference media (e.g. [[air]] at a standardized [[pressure]] and [[temperature]]) have been common. It is usually given the symbol ''n''. In the case of light, it equals
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The '''refractive index''' (or '''index of [[refraction]]''') of a medium is the inverse ratio of the [[phase velocity]] (defined below) of a [[wave]] phenomenon such as [[light]] or [[sound]], and the phase velocity in a reference medium (substance that the wave passes through). It is most commonly used in the context of light with [[vacuum]] as a reference medium, although historically other reference media (e.g. [[air]] at a standard [[pressure]] and [[temperature]]) have been common. It is usually given the symbol ''n,'' In the case of light, it equals
  
 
:<math> n=\sqrt{\epsilon_r\mu_r}</math>,
 
:<math> n=\sqrt{\epsilon_r\mu_r}</math>,
  
where ''ε<sub>r</sub>'' is the material's relative [[permittivity]], and ''μ<sub>r</sub>'' is its relative [[Permeability (electromagnetism)|permeability]]. For most materials, ''μ<sub>r</sub>'' is very close to 1 at optical frequencies, therefore ''n'' is approximately <math>\sqrt{\epsilon_r}</math>. Contrary to a widespread misconception, ''n'' may be less than 1. This has practical technical applications, such as effective mirrors for [[X-ray]]s based on [[total internal reflection]].
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where ''ε<sub>r</sub>'' is the material's relative [[permittivity]] (how a material affects an electric field), and ''μ<sub>r</sub>'' is its relative [[Permeability (electromagnetism)|permeability]] (how a material reacts to a magnetic field). For most materials, ''μ<sub>r</sub>'' is very close to 1 at optical frequencies, therefore ''n'' is approximately <math>\sqrt{\epsilon_r}</math>. ''n'' may be less than 1 and this has practical technical applications, such as effective mirrors for [[X-ray]]s based on [[total internal reflection]].
  
The [[phase velocity]] is defined as the rate at which the crests of the [[waveform]] propagate; that is, the rate at which the [[phase (waves)|phase]] of the waveform is moving. The ''[[group velocity]]'' is the rate that the ''envelope'' of the waveform is propagating; that is, the rate of variation of the [[amplitude]] of the waveform. It is the group velocity that (almost always) represents the rate that information (and energy) may be transmitted by the wave, for example the velocity at which a pulse of light travels down an [[optical fiber]].
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The [[phase velocity]] is defined as the rate at which any part of the [[waveform]] travels through space; that is, the rate at which the [[phase (waves)|phase]] of the waveform is moving. The ''[[group velocity]]'' is the rate that the ''envelope'' of the waveform is propagating; that is, the rate of variation of the [[amplitude]] (the maximum up and down motion) of the waveform. It is the group velocity, the velocity at which the crests and troughs of a wave move through space, that (almost always) represents the rate that information (and energy) may be transmitted by the wave—for example, the velocity at which a pulse of light travels down an [[optical fiber]].
  
 
===The speed of light===
 
===The speed of light===
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The speed of all electromagnetic radiation in vacuum is the same, approximately 3&times;10<sup>8</sup> meters per second, and is denoted by [[speed of light|''c'']].  
 
The speed of all electromagnetic radiation in vacuum is the same, approximately 3&times;10<sup>8</sup> meters per second, and is denoted by [[speed of light|''c'']].  
Therefore, if ''v'' is the [[phase velocity]] of radiation of a specific frequency in a specific material, the refractive index is given by  
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Therefore, if ''v'' is the phase velocity of radiation of a specific frequency in a specific material, the refractive index is given by  
  
 
:<math>n =\frac{c}{v}</math>.
 
:<math>n =\frac{c}{v}</math>.
  
This number is typically greater than one: the higher the index of the material, the more the light is slowed down. However, at certain frequencies (e.g. near [[absorption (optics)|absorption]] resonances, and for [[X-ray]]s), ''n'' will actually be smaller than one. This does not contradict the [[theory of relativity]], which holds that no [[Signal (electrical engineering)|information-carrying signal]] can ever propagate faster than ''c'', because the [[phase velocity]] is not the same as the [[group velocity]] or the [[signal velocity]].
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This number is typically greater than one: the higher the index of the material, the more the light is slowed down. However, at certain frequencies (e.g., [[X-ray]]s), ''n'' will actually be smaller than one. This does not contradict the [[theory of relativity]], which holds that no [[Signal (electrical engineering)|information-carrying signal]] can ever propagate faster than ''c,'' because the phase velocity is not the same as the group velocity or the [[signal velocity]], same as group velocity except when the wave is passing through an absorptive medium.
  
Sometimes, a "group velocity refractive index", usually called the ''group index'' is defined:
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Sometimes, a "group velocity refractive index," usually called the ''group index'' is defined:
  
 
:<math>n_g=\frac{c}{v_g}</math>
 
:<math>n_g=\frac{c}{v_g}</math>
  
where ''v<sub>g</sub>'' is the group velocity. This value should not be confused with ''n'', which is always defined with respect to the phase velocity.  
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where ''v<sub>g</sub>'' is the group velocity. This value should not be confused with ''n,'' which is always defined with respect to the phase velocity.  
  
At the microscale, an electromagnetic wave's phase velocity is slowed in a material because the [[electric field]] creates a disturbance in the charges of each atom (primarily the [[electron]]s) proportional to the [[permittivity]]. The charges will, in general, oscillate slightly out of [[phase (waves)|phase]] with respect to the driving electric field. The charges thus radiate their own electromagnetic wave that is at the same frequency but with a phase delay. The macroscopic sum of all such contributions in the material is a wave with the same frequency but shorter wavelength than the original, leading to a slowing of the wave's phase velocity. Most of the radiation from oscillating material charges will modify the incoming wave, changing its velocity. However, some net energy will be radiated in other directions (see [[scattering]]).
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At the microscale, an electromagnetic wave's phase velocity is slowed in a material because the [[electric field]] creates a disturbance in the charges of each atom (primarily the [[electron]]s) proportional (a <math>y=kx</math> relationship) to the [[permittivity]]. The charges will, in general, oscillate slightly out of [[phase (waves)|phase]] with respect to the driving electric field. The charges thus radiate their own electromagnetic wave that is at the same frequency but with a phase delay. The macroscopic sum of all such contributions in the material is a wave with the same frequency but shorter wavelength than the original, leading to a slowing of the wave's phase velocity. Most of the radiation from oscillating material charges will modify the incoming wave, changing its velocity. However, some net energy will be radiated in other directions (see [[scattering]]).
  
 
If the refractive indices of two materials are known for a given frequency, then one can compute the angle by which radiation of that frequency will be [[refraction|refracted]] as it moves from the first into the second material from [[Snell's law]].
 
If the refractive indices of two materials are known for a given frequency, then one can compute the angle by which radiation of that frequency will be [[refraction|refracted]] as it moves from the first into the second material from [[Snell's law]].
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===Negative Refractive Index===
 
===Negative Refractive Index===
  
Recent research has also demonstrated the existence of [[negative refractive index]] which can occur if ''ε'' and ''μ'' are ''simultaneously'' negative. Not thought to occur naturally, this can be achieved with so called [[metamaterial]]s and offers the possibility of perfect lenses and other exotic phenomena such as a reversal of [[Snell%27s_law|Snell's law]]. [http://www.newscientisttech.com/article/dn10816.html]
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Recent research has also demonstrated the existence of negative refractive index, which can occur if ''ε'' and ''μ'' are ''simultaneously'' negative. Not thought to occur naturally, it can be achieved with so called [[metamaterial]]s. It offers the possibility of perfect lenses and other exotic phenomena such as a reversal of [[Snell%27s_law|Snell's law]].
  
 
== List of indices of refraction ==
 
== List of indices of refraction ==
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|}
 
|}
  
Many materials have a well-characterized [[refractive index]], but these indices depend strongly upon the [[frequency]] of light. Therefore, any numeric value for the index is meaningless unless the associated frequency is specified.
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Many materials have well-characterized refractive indices, but these indices depend strongly on the [[frequency]] of light. Therefore, any numeric value for the index is meaningless unless the associated frequency is specified.
  
There are also weaker dependencies on [[temperature]], [[pressure]]/[[stress (physics)|stress]], et cetera, as well on precise material compositions (presence of [[dopant]]s et cetera); for many materials and typical conditions, however, these variations are at the percent level or less. Thus, it is especially important to cite the source for an index measurement if precision is required.
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There are also weaker dependencies on [[temperature]], [[pressure]]/[[stress (physics)|stress]], and so forth, as well as on precise material compositions. For many materials and typical conditions, however, these variations are at the percent level or less. It is therefore especially important to cite the source for an index measurement, if precision is required.
  
In general, an index of refraction is a [[complex number]] with both a real and imaginary part, where the latter indicates the strength of absorption loss at a particular wavelength&mdash;thus, the imaginary part is sometimes called the [[extinction coefficient]] ''k''Such losses become particularly significant, for example, in metals at short (e.g. visible) wavelengths, and must be included in any description of the [[refractive index]].
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In general, an index of refraction is a [[complex number]] with both a real and an imaginary part, where the latter indicates the strength of absorption loss at a particular wavelength&mdash;thus, the imaginary part is sometimes called the [[extinction coefficient]] ''k.'' Such losses become particularly significant—for example, in metals at short wavelengths (such as visible light)—and must be included in any description of the refractive index.
  
 
==Dispersion and absorption==
 
==Dispersion and absorption==
  
In real materials, the [[polarization (electrostatics)|polarization]] does not respond instantaneously to an applied field.  This causes [[dielectric loss]], which can be expressed by a [[permittivity]] that is both [[complex number|complex]] and [[frequency]] dependent.  Real materials are not perfect [[Electrical insulation|insulator]]s either, i.e. they have non-zero [[direct current]] [[electrical conductivity|conductivity]]. Taking both aspects into consideration, we can define a complex index of refraction:
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In real materials, the [[polarization (electrostatics)|polarization]] does not respond instantaneously to an applied field.  This causes [[dielectric loss]], which can be expressed by a [[permittivity]] that is both [[complex number|complex]] and [[frequency]] dependent.  Real materials are not perfect [[Electrical insulation|insulator]]s either, meaning they have non-zero Direct Current (DC) conductivity. Taking both aspects into consideration, we can define a complex index of refraction:
  
 
:<math>\tilde{n}=n-i\kappa</math>
 
:<math>\tilde{n}=n-i\kappa</math>
  
Here, ''n'' is the refractive index indicating the phase velocity as above, while ''κ'' is called the [[extinction coefficient]], which indicates the amount of [[absorption (optics)|absorption]] loss when the electromagnetic wave propagates through the material.  Both ''n'' and ''κ'' are dependent on the frequency ([[wavelength]]).
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Here, ''n'' is the refractive index indicating the phase velocity, while ''κ'' is called the [[extinction coefficient]], which indicates the amount of [[absorption (optics)|absorption]] loss when the electromagnetic wave propagates through the material.  Both ''n'' and ''κ'' are dependent on the frequency.
  
The effect that ''n'' varies with [[frequency]] (except in vacuum, where all frequencies travel at the same speed, ''c'') is known as [[dispersion (optics)|dispersion]], and it is what causes a [[Triangular prism (optics)|prism]] to divide white light into its constituent spectral [[color]]s, explains [[rainbow]]s, and is the cause of [[chromatic aberration]] in [[Lens (optics)|lenses]]. In regions of the spectrum where the material does not absorb, the real part of the refractive index tends to increase with frequency. Near absorption peaks, the curve of the refractive index is a complex form given by the [[Kramers-Kronig relations]], and can decrease with frequency.
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The effect that ''n'' varies with [[frequency]] (except in vacuum, where all frequencies travel at the same speed ''c'') is known as [[dispersion (optics)|dispersion]], and it is what causes a [[Triangular prism (optics)|prism]] to divide white light into its constituent spectral [[color]]s, which is how [[rainbow]]s are formed in rain or mists. Dispersion is also the cause of [[chromatic aberration]] in [[Lens (optics)|lenses]].  
  
 
Since the refractive index of a material varies with the frequency (and thus wavelength) of light, it is usual to specify the corresponding vacuum wavelength at which the refractive index is measured. Typically, this is done at various well-defined spectral [[emission line]]s; for example, ''n''<sub>D</sub> is the refractive index at the [[Fraunhofer lines|Fraunhofer]] "D" line, the centre of the yellow [[sodium]] double emission at 589.29 [[nanometre|nm]] wavelength.
 
Since the refractive index of a material varies with the frequency (and thus wavelength) of light, it is usual to specify the corresponding vacuum wavelength at which the refractive index is measured. Typically, this is done at various well-defined spectral [[emission line]]s; for example, ''n''<sub>D</sub> is the refractive index at the [[Fraunhofer lines|Fraunhofer]] "D" line, the centre of the yellow [[sodium]] double emission at 589.29 [[nanometre|nm]] wavelength.
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The real and imaginary parts of the complex refractive index are related through use of the [[Kramers-Kronig relations]]. For example, one can determine a material's full complex refractive index as a function of wavelength from an absorption spectrum of the material.
 
The real and imaginary parts of the complex refractive index are related through use of the [[Kramers-Kronig relations]]. For example, one can determine a material's full complex refractive index as a function of wavelength from an absorption spectrum of the material.
  
==Anisotropy==
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==Birefringence==
 
[[Image:Calcite.jpg|thumb|A calcite crystal laid upon a paper with some letters showing [[birefringence]].]]
 
[[Image:Calcite.jpg|thumb|A calcite crystal laid upon a paper with some letters showing [[birefringence]].]]
  
The refractive index of certain media may be different depending on the [[polarization]] and direction of propagation of the light through the medium. This is known as [[birefringence]] or anisotropy and is described by the field of [[crystal optics]]. In the most general case, the ''[[dielectric constant]]'' is a rank-2 [[tensor]] (a 3 by 3 matrix), which cannot simply be described by refractive indices except for polarizations along principal axes.
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The refractive index of certain media may be different depending on the [[polarization]] and direction of propagation of the light through the medium. This is known as [[birefringence]] and is described by the field of [[crystal optics]].
 
 
In magneto-optic (gyro-magnetic) and [[optical activity|optically active]] materials, the principal axes are complex (corresponding to elliptical polarizations), and the dielectric tensor is complex-[[Hermitian]] (for lossless media); such materials break time-reversal symmetry and are used e.g. to construct [[Faraday isolator]]s.
 
  
 
==Nonlinearity==
 
==Nonlinearity==
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==Inhomogeneity==
 
==Inhomogeneity==
[[Image:Grin-lens.png|thumb|A gradient-index lens with a parabolic variation of refractive index (''n'') with radial distance (''x''). The lens focuses light in the same way as a conventional lens.]]
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[[Image:Grin-lens.png|thumb|A gradient-index lens with a parabolic variation of refractive index ''(n)'' with radial distance ''(x)''. The lens focuses light in the same way as a conventional lens.]]
  
If the refractive index of a medium is not constant, but varies gradually with position, the material is known as a gradient-index medium and is described by [[gradient index optics]]. Light travelling through such a medium can be bent or focussed, and this effect can be exploited to produce [[lens (optics)|lenses]], some [[optical fiber]]s and other  devices. Some common [[mirage]]s are caused by a spatially-varying refractive index of [[Earth's atmosphere|air]].
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If the refractive index of a medium is not constant, but varies gradually with position, the material is known as a gradient-index medium and is described by [[gradient index optics]]. Light traveling through such a medium can be bent or focussed, and this effect can be exploited to produce [[lens (optics)|lenses]], some [[optical fiber]]s and other  devices. Some common [[mirage]]s are caused by a spatially varying refractive index of [[Earth's atmosphere|air]].
  
 
==Applications==
 
==Applications==
  
The refractive index of a material is the most important property of any [[optics|optical]] system that uses [[refraction]]. It is used to calculate the focusing power of lenses, and the dispersive power of prisms.  
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The refractive index of a material is the most important property of any [[optics|optical]] system that uses the property of refraction. It is used to calculate the focusing power of lenses and the dispersive power of prisms.
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Since refractive index is a fundamental physical property of a substance, it is often used to identify a particular substance, confirm its purity, or measure its concentration. Refractive index is used to measure solids (glasses and gemstones), liquids, and gases. Most commonly, it is used to measure the concentration of a [[solute]] in an [[aqueous]] [[solution]]. A [[refractometer]] is the instrument used to measure refractive index. For a solution of sugar, the refractive index can be used to determine the sugar content.
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In [[medicine]], particularly [[ophthalmology]] and [[optometry]], the technique of ''refractometry'' utilizes the property of refraction for administering eye tests. This is a clinical test in which a [[phoropter]] is used to determine the eye's [[refractive error]] and, based on that, the best [[corrective lens]]es to be prescribed. A series of test lenses in graded [[optical power]]s or [[focal length]]s are presented, to determine which ones provide the sharpest, clearest vision.
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== Alternative meaning: Refraction in metallurgy ==
  
Since refractive index is a fundamental physical property of a substance, it is often used to identify a particular substance, confirm its purity, or measure its concentration. Refractive index is used to measure solids (glasses and gemstones), liquids, and gases. Most commonly it is used to measure the concentration of a [[solute]] in an [[aqueous]] [[solution]]. A [[refractometer]] is the instrument used to measure refractive index. For a solution of sugar, the refractive index can be used to determine the sugar content.
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In [[metallurgy]], the term ''refraction'' has another meaning. It is a property of [[metal]]s that indicates their ability to withstand [[heat]]. Metals with a high degree of refraction are referred to as ''[[refractory]].'' These metals have high melting points, derived from the strong interatomic forces that are involved in metal bonds. Large quantities of energy are required to overcome these forces.
  
In [[medicine]], particularly [[ophthalmology]] and [[optometry]], ''refraction'' (or the technique of ''refractometry'') is a clinical test in which a [[phoropter]] is used to determine the eye's [[refractive error]] and the best [[corrective lens]]es to be prescribed. A series of test lenses in graded [[optical power]]s or [[focal length]]s are presented to determine which provide the sharpest, clearest vision.<ref>{{cite web|url=http://www.eyeglossary.net/#R|title=Eye Glossary|accessdate=2006-05-23}}</ref>
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Examples of refractory metals include [[molybdenum]], [[niobium]], [[tungsten]], and [[tantalum]]. [[Hafnium(IV) carbide|Hafnium carbide]] is the most refractory [[binary compound]] known, with a melting point of 3,890 degrees C.[http://periodic.lanl.gov/elements/72.html][http://www.mdatechnology.net/techsearch.asp?articleid=648]
  
 
== See also ==
 
== See also ==
  
* [[Sellmeier equation]]
 
* [[Total internal reflection]]
 
* [[Negative refractive index]] or [[Metamaterial]]
 
* [[Index-matching material]]
 
 
* [[Birefringence]]
 
* [[Birefringence]]
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* [[Light]]
 
* [[Reflection (physics)]]
 
* [[Reflection (physics)]]
* [[Willebrord Snellius]]
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* [[Sound]]
* [[Total refraction]]
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* [[Huygens-Fresnel principle]]
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==References==
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* Fishbane, Paul M., et al. 2005. ''Physics for Scientists and Engineers,'' 3rd ed. Upper Saddle River, NJ: Pearson Education. ISBN 0131418815.
 +
 
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* Hecht, Jeff. 2006. [http://www.newscientisttech.com/article/dn10816.html Red Light Debut for Exotic 'Metamaterial.'] ''NewScientist.com News Service''. 13:38. Retrieved March 28, 2007.
  
== Footnotes ==
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* Henderson, Tom. 2004. [http://www.physicsclassroom.com/Class/refrn/refrntoc.html Refraction and the Ray Model of Light.] ''The Physics Classroom''. Retrieved February 20, 2007.
<references/>
 
  
==References==
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* Ward, David W., Keith A. Nelson, and Kevin J. Webb. 2005. [http://www.iop.org/EJ/abstract/1367-2630/7/1/213 On the Physical Origins of the Negative Index of Refraction.] ''New Journal of Physics'' 7:213. Retrieved March 28, 2007.
*David W. Ward and Keith A. Nelson. 2005. [http://www.iop.org/EJ/abstract/1367-2630/7/1/213 On the Physical Origins of the Negative Index of Refraction], ''New Journal of Physics'', '''Vol. 7''', p. 213.
 
*Fishbane, Paul M., ''et al''. 2005. ''Physics for Scientists and Engineers (3rd Ed.)''. Upper Saddle River, NJ: Pearson Education, Inc. ISBN 0131418815.
 
*Henderson, Tom. 2004. [http://www.physicsclassroom.com/Class/refrn/refrntoc.html Refraction and the Ray Model of Light]. The Physics Classroom. Retrieved February 20, 2007.
 
  
 
==External links==
 
==External links==
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All links retrieved December 7, 2022.
  
* [http://www.phy.ntnu.edu.tw/ntnujava/viewtopic.php?t=32 Java explanatory animation]
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* [http://www.phy.hk/wiki/englishhtm/RefractionByPrism.htm Refraction through a Prism.] (Java simulation.)
* [http://www.falstad.com/ripple/ex-refraction.html Java ilustration of refraction]
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* [http://scienceworld.wolfram.com/physics/IndexofRefraction.html Index of Refraction - Eric Weisstein's World of Physics.]  
*[http://www.phy.hk/wiki/englishhtm/RefractionByPrism.htm Java simulation of refraction through a prism]
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* [http://hyperphysics.phy-astr.gsu.edu/hbase/tables/indrf.html#c1 Index of Refraction - Hyperphysics.] (List of refractive indices.)
*[http://scienceworld.wolfram.com/physics/IndexofRefraction.html Science World]
 
*[http://hyperphysics.phy-astr.gsu.edu/hbase/tables/indrf.html#c1 Hyperphysics list of refractive indices]
 
 
 
  
 
[[Category:Physical sciences]]
 
[[Category:Physical sciences]]
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[[Category:Optics]]
 
[[Category:Optics]]
  
{{credit3|Refraction|105507381|Refractive_index|106077905|List_of_indices_of_refraction|102384239}}
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{{credits|Refraction|105507381|Refractive_index|106077905|List_of_indices_of_refraction|102384239|Refraction_(metallurgy)|106398626}}

Latest revision as of 03:01, 8 December 2022

A straw dipped in a colored solution appears to be broken, because of the refraction of light as it passes from the solution to the air.

Refraction is the change in direction of a wave due to a change in its speed, as observed when a wave passes from one medium to another. The most common example is the refraction of light, as happens in the formation of rainbows in the sky or rainbow-like bands when white light passes through a glass prism. Other types of waves also undergo refraction, for example, when sound waves pass from one medium into another.

The refraction of waves through a medium is quantified in terms of what is called the refractive index (or index of refraction). The refractive index of a medium is a measure of how much the speed of light (or other waves) is reduced inside the medium, compared with the speed of light in vacuum or air. For example, if a sample of glass has a refractive index of 1.5, it means that the speed of light traveling through the glass is times the speed of light in vacuum or air.

Based on knowledge of the properties of refraction and refractive index, a number of applications have been developed. For example, the invention of lenses and refracting telescopes rests on an understanding of refraction. Also, knowledge of the refractive index of various substances is used to evaluate the purity of a substance or measure its concentration in a mixture. In eye tests performed by ophthalmologists or optometrists, the property of refraction forms the basis for the technique known as refractometry.

Explanation

In optics, refraction occurs when light waves travel from a medium with a particular refractive index to a second medium with another refractive index. At the boundary between the media, the wave's phase velocity is altered, it changes direction, and its wavelength increases or decreases, but its frequency remains constant. For example, a light ray will undergo refraction as it enters and leaves glass. An understanding of this concept led to the invention of lenses and the refracting telescope.

Refraction of light waves in water. The dark rectangle represents the actual position of a pencil sitting in a bowl of water. The light rectangle represents the apparent position of the pencil. Notice that the end (X) looks like it is at (Y), a position that is considerably shallower than (X).

Refraction can be seen when looking into a bowl of water. Air has a refractive index of about 1.0003, and water has a refractive index of about 1.33. If a person looks at a straight object, such as a pencil or straw, which is placed at a slant, partially in the water, the object appears to bend at the water's surface. This is due to the bending of light rays as they move from the water to the air. Once the rays reach the eye, the eye traces them back as straight lines (lines of sight). The lines of sight (shown as dashed lines) intersect at a higher position than where the actual rays originated. This causes the pencil to appear higher and the water to appear shallower than it really is. The depth that the water appears to be when viewed from above is known as the apparent depth,

Diagram of refraction of water waves

The diagram on the right shows an example of refraction in water waves. Ripples travel from the left and pass over a shallower region inclined at an angle to the wavefront. The waves travel more slowly in the shallower water, so the wavelength decreases and the wave bends at the boundary. The dotted line represents the normal to the boundary. The dashed line represents the original direction of the waves. The phenomenon explains why waves on a shoreline never hit the shoreline at an angle. Whichever direction the waves travel in deep water, they always refract towards the normal as they enter the shallower water near the beach.

Refraction is also responsible for rainbows and for the splitting of white light into a rainbow-spectrum as it passes through a glass prism. Glass has a higher refractive index than air and the different frequencies of light travel at different speeds (dispersion), causing them to be refracted at different angles, so that you can see them. The different frequencies correspond to different colors observed.

While refraction allows for beautiful phenomena such as rainbows it may also produce peculiar optical phenomena, such as mirages and Fata Morgana. These are caused by the change of the refractive index of air with temperature.

Refraction in a Perspex (acrylic) block.

Snell's law is used to calculate the degree to which light is refracted when traveling from one medium to another.

Recently some metamaterials have been created which have a negative refractive index. With metamaterials, we can also obtain the total refraction phenomena when the wave impedances of the two media are matched. There is no reflected wave.

Also, since refraction can make objects appear closer than they are, it is responsible for allowing water to magnify objects. First, as light is entering a drop of water, it slows down. If the water's surface is not flat, then the light will be bent into a new path. This round shape will bend the light outwards and as it spreads out, the image you see gets larger.

Refractive index

The refractive index (or index of refraction) of a medium is the inverse ratio of the phase velocity (defined below) of a wave phenomenon such as light or sound, and the phase velocity in a reference medium (substance that the wave passes through). It is most commonly used in the context of light with vacuum as a reference medium, although historically other reference media (e.g. air at a standard pressure and temperature) have been common. It is usually given the symbol n, In the case of light, it equals

,

where εr is the material's relative permittivity (how a material affects an electric field), and μr is its relative permeability (how a material reacts to a magnetic field). For most materials, μr is very close to 1 at optical frequencies, therefore n is approximately . n may be less than 1 and this has practical technical applications, such as effective mirrors for X-rays based on total internal reflection.

The phase velocity is defined as the rate at which any part of the waveform travels through space; that is, the rate at which the phase of the waveform is moving. The group velocity is the rate that the envelope of the waveform is propagating; that is, the rate of variation of the amplitude (the maximum up and down motion) of the waveform. It is the group velocity, the velocity at which the crests and troughs of a wave move through space, that (almost always) represents the rate that information (and energy) may be transmitted by the wave—for example, the velocity at which a pulse of light travels down an optical fiber.

The speed of light

Refraction of light at the interface between two media of different refractive indices, with n2 > n1. The velocity is lower in the second medium (v2 < v1), therefore the angle of refraction θ2 is less than the angle of incidence θ1; that is, the ray in the higher-index medium is closer to the normal.

The speed of all electromagnetic radiation in vacuum is the same, approximately 3×108 meters per second, and is denoted by c. Therefore, if v is the phase velocity of radiation of a specific frequency in a specific material, the refractive index is given by

.

This number is typically greater than one: the higher the index of the material, the more the light is slowed down. However, at certain frequencies (e.g., X-rays), n will actually be smaller than one. This does not contradict the theory of relativity, which holds that no information-carrying signal can ever propagate faster than c, because the phase velocity is not the same as the group velocity or the signal velocity, same as group velocity except when the wave is passing through an absorptive medium.


Sometimes, a "group velocity refractive index," usually called the group index is defined:

where vg is the group velocity. This value should not be confused with n, which is always defined with respect to the phase velocity.

At the microscale, an electromagnetic wave's phase velocity is slowed in a material because the electric field creates a disturbance in the charges of each atom (primarily the electrons) proportional (a relationship) to the permittivity. The charges will, in general, oscillate slightly out of phase with respect to the driving electric field. The charges thus radiate their own electromagnetic wave that is at the same frequency but with a phase delay. The macroscopic sum of all such contributions in the material is a wave with the same frequency but shorter wavelength than the original, leading to a slowing of the wave's phase velocity. Most of the radiation from oscillating material charges will modify the incoming wave, changing its velocity. However, some net energy will be radiated in other directions (see scattering).

If the refractive indices of two materials are known for a given frequency, then one can compute the angle by which radiation of that frequency will be refracted as it moves from the first into the second material from Snell's law.

Negative Refractive Index

Recent research has also demonstrated the existence of negative refractive index, which can occur if ε and μ are simultaneously negative. Not thought to occur naturally, it can be achieved with so called metamaterials. It offers the possibility of perfect lenses and other exotic phenomena such as a reversal of Snell's law.

List of indices of refraction

Some representative refractive indices
Material n at f=5.09x1014 Hz
Vacuum 1 (exactly)
Helium 1.000036
Air @ STP 1.0002926
Carbon dioxide 1.00045
Water Ice 1.31
Liquid Water (20°C) 1.333
Cryolite 1.338
Acetone 1.36
Ethanol 1.36
Teflon 1.35 - 1.38
Glycerol 1.4729
Acrylic glass 1.490 - 1.492
Rock salt 1.516
Crown glass (pure) 1.50 - 1.54
Salt (NaCl) 1.544
Polycarbonate 1.584 - 1.586
Flint glass (pure) 1.60 - 1.62
Crown glass (impure) 1.485 - 1.755
Bromine 1.661
Flint glass (impure) 1.523 - 1.925
Cubic zirconia 2.15 - 2.18
Diamond 2.419
Moissanite 2.65 - 2.69
Cinnabar (Mercury sulfide) 3.02
Gallium(III) phosphide 3.5
Gallium(III) arsenide 3.927
Silicon 4.01

Many materials have well-characterized refractive indices, but these indices depend strongly on the frequency of light. Therefore, any numeric value for the index is meaningless unless the associated frequency is specified.

There are also weaker dependencies on temperature, pressure/stress, and so forth, as well as on precise material compositions. For many materials and typical conditions, however, these variations are at the percent level or less. It is therefore especially important to cite the source for an index measurement, if precision is required.

In general, an index of refraction is a complex number with both a real and an imaginary part, where the latter indicates the strength of absorption loss at a particular wavelength—thus, the imaginary part is sometimes called the extinction coefficient k. Such losses become particularly significant—for example, in metals at short wavelengths (such as visible light)—and must be included in any description of the refractive index.

Dispersion and absorption

In real materials, the polarization does not respond instantaneously to an applied field. This causes dielectric loss, which can be expressed by a permittivity that is both complex and frequency dependent. Real materials are not perfect insulators either, meaning they have non-zero Direct Current (DC) conductivity. Taking both aspects into consideration, we can define a complex index of refraction:

Here, n is the refractive index indicating the phase velocity, while κ is called the extinction coefficient, which indicates the amount of absorption loss when the electromagnetic wave propagates through the material. Both n and κ are dependent on the frequency.

The effect that n varies with frequency (except in vacuum, where all frequencies travel at the same speed c) is known as dispersion, and it is what causes a prism to divide white light into its constituent spectral colors, which is how rainbows are formed in rain or mists. Dispersion is also the cause of chromatic aberration in lenses.

Since the refractive index of a material varies with the frequency (and thus wavelength) of light, it is usual to specify the corresponding vacuum wavelength at which the refractive index is measured. Typically, this is done at various well-defined spectral emission lines; for example, nD is the refractive index at the Fraunhofer "D" line, the centre of the yellow sodium double emission at 589.29 nm wavelength.

The Sellmeier equation is an empirical formula that works well in describing dispersion, and Sellmeier coefficients are often quoted instead of the refractive index in tables. For some representative refractive indices at different wavelengths, see list of indices of refraction.

As shown above, dielectric loss and non-zero DC conductivity in materials cause absorption. Good dielectric materials such as glass have extremely low DC conductivity, and at low frequencies the dielectric loss is also negligible, resulting in almost no absorption (κ ≈ 0). However, at higher frequencies (such as visible light), dielectric loss may increase absorption significantly, reducing the material's transparency to these frequencies.

The real and imaginary parts of the complex refractive index are related through use of the Kramers-Kronig relations. For example, one can determine a material's full complex refractive index as a function of wavelength from an absorption spectrum of the material.

Birefringence

A calcite crystal laid upon a paper with some letters showing birefringence.

The refractive index of certain media may be different depending on the polarization and direction of propagation of the light through the medium. This is known as birefringence and is described by the field of crystal optics.

Nonlinearity

The strong electric field of high intensity light (such as output of a laser) may cause a medium's refractive index to vary as the light passes through it, giving rise to nonlinear optics. If the index varies quadratically with the field (linearly with the intensity), it is called the optical Kerr effect and causes phenomena such as self-focusing and self phase modulation. If the index varies linearly with the field (which is only possible in materials that do not possess inversion symmetry), it is known as the Pockels effect.

Inhomogeneity

A gradient-index lens with a parabolic variation of refractive index (n) with radial distance (x). The lens focuses light in the same way as a conventional lens.

If the refractive index of a medium is not constant, but varies gradually with position, the material is known as a gradient-index medium and is described by gradient index optics. Light traveling through such a medium can be bent or focussed, and this effect can be exploited to produce lenses, some optical fibers and other devices. Some common mirages are caused by a spatially varying refractive index of air.

Applications

The refractive index of a material is the most important property of any optical system that uses the property of refraction. It is used to calculate the focusing power of lenses and the dispersive power of prisms.

Since refractive index is a fundamental physical property of a substance, it is often used to identify a particular substance, confirm its purity, or measure its concentration. Refractive index is used to measure solids (glasses and gemstones), liquids, and gases. Most commonly, it is used to measure the concentration of a solute in an aqueous solution. A refractometer is the instrument used to measure refractive index. For a solution of sugar, the refractive index can be used to determine the sugar content.

In medicine, particularly ophthalmology and optometry, the technique of refractometry utilizes the property of refraction for administering eye tests. This is a clinical test in which a phoropter is used to determine the eye's refractive error and, based on that, the best corrective lenses to be prescribed. A series of test lenses in graded optical powers or focal lengths are presented, to determine which ones provide the sharpest, clearest vision.

Alternative meaning: Refraction in metallurgy

In metallurgy, the term refraction has another meaning. It is a property of metals that indicates their ability to withstand heat. Metals with a high degree of refraction are referred to as refractory. These metals have high melting points, derived from the strong interatomic forces that are involved in metal bonds. Large quantities of energy are required to overcome these forces.

Examples of refractory metals include molybdenum, niobium, tungsten, and tantalum. Hafnium carbide is the most refractory binary compound known, with a melting point of 3,890 degrees C.[1][2]

See also

References
ISBN links support NWE through referral fees

  • Fishbane, Paul M., et al. 2005. Physics for Scientists and Engineers, 3rd ed. Upper Saddle River, NJ: Pearson Education. ISBN 0131418815.

External links

All links retrieved December 7, 2022.

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