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{{Short description|Small angle approximation in geometric optics}}
In [[geometric optics]], the '''paraxial approximation''' is a [[small-angle approximation]] used in [[Gaussian optics]] and [[Ray tracing (physics)|ray tracing]] of light through an optical system (such as a [[lens (optics)|lens]]).<ref name=Greivenkamp>{{cite book | first=John E. | last=Greivenkamp | year=2004 | title=Field Guide to Geometrical Optics | publisher=SPIE | others=SPIE Field Guides vol. '''FG01''' | isbn=0-8194-5294-7 |pages=19–20 }}</ref> The word ''paraxial'' derives from the Greek word παρά, ''para'' (near) and the Latin word ''axis''. ▼
[[File:Small angle compare error.svg|thumbnail|The error associated with the paraxial approximation. In this plot the cosine is approximated by {{nowrap|1 - θ<sup>2</sup>/2}}.]]
▲In [[geometric optics]], the '''paraxial approximation''' is a [[small-angle approximation]] used in [[Gaussian optics]] and [[Ray tracing (physics)|ray tracing]] of light through an optical system (such as a [[lens (optics)|lens]]).<ref name="Greivenkamp">{{
| last=Weisstein
| author-link=Eric W. Weisstein
| first=Eric W.
| title=Paraxial Approximation
| url=http://scienceworld.wolfram.com/physics/ParaxialApproximation.html
| work=[[ScienceWorld]]
| publisher=[[Wolfram Research]]
| accessdate=15 January 2014|year=2007}}</ref>
A '''paraxial ray''' is a [[Ray (optics)|ray]]
:<math>
\sin \theta
\tan \theta
▲:<math>\cos \theta \approx 1</math>
The paraxial approximation is used in [[Gaussian optics]] and ''first-order''
In some cases, the second-order approximation is also called "paraxial".
:<math> \cos \theta \approx 1 - { \theta^2 \over 2 } \ .</math>
The
{{cite web
| title=Paraxial approximation error plot
| url=http://www.wolframalpha.com/input/?i=Plot%5B{%28x+Deg+-+Sin%5Bx+Deg%5D%29%2FSin%5Bx+Deg%5D%2C+%28Tan%5Bx+Deg%5D+-+x+Deg%29%2FTan%5Bx+Deg%5D%2C+%281+-+Cos%5Bx+Deg%5D%29%2FCos%5Bx+Deg%5D}%2C+{x%2C+0%2C+15}%5D
| work=[[Wolfram Alpha]]
| publisher=[[Wolfram Research]]
| accessdate=26 August 2014}}</ref>
<!-- This plots the error plot of the paraxial approximation, i.e. the 3 curves for small angles: Plot[{(x Deg - Sin[x Deg])/Sin[x Deg], (Tan[x Deg] - x Deg)/Tan[x Deg], (1 - Cos[x Deg])/Cos[x Deg]}, {x, 0, 15}] -->
For larger angles it is often necessary to distinguish between [[meridional ray]]s, which lie in a plane containing the [[optical axis]], and [[sagittal ray]]s, which do not.
Use of the small angle approximations replaces dimensionless trigonometric functions with angles in radians. In [[dimensional analysis]] on optics equations radians are dimensionless and therefore can be ignored.
A paraxial approximation is also commonly used in [[physical optics]]. It is used in the derivation of the paraxial wave equation from the homogeneous [[Maxwell's equations]] and, consequently, [[Gaussian beam]] optics.
==References==
{{
== External links ==
* [http://demonstrations.wolfram.com/ParaxialApproximationAndTheMirror/ Paraxial Approximation and the Mirror] by David Schurig, [[The Wolfram Demonstrations Project]].
[[Category:Geometrical optics]]▼
▲[[Category:Geometrical optics]]
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