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			== Paraxial approximation ==
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'''Paraxial approximation''' is a simplification used in [[optics]] and [[wave physics]] to analyze and describe the behavior of [[light rays]] and [[waves]] under certain conditions. This approximation is particularly useful in the study of [[lens]] systems, [[microscopes]], [[telescopes]], and other optical instruments where it aids in understanding the formation of [[image]]s and the properties of optical systems without the need for complex mathematical calculations.

==Overview==
The paraxial approximation assumes that light rays and waves propagate at small angles to the optical axis of a system, and that these angles are so small that their [[sine]], [[tangent]], and other trigonometric functions can be approximated by the angle itself, measured in radians. This simplification allows for the linearization of the equations governing light propagation, making them easier to solve.

==Application==
In practical terms, the paraxial approximation is applied in the design and analysis of optical systems to predict how light will behave as it passes through lenses and reflects off mirrors. It is a cornerstone of [[geometrical optics]], which deals with the approximation of light as rays. This approach simplifies the study of optical systems by reducing the complex wave nature of light to straight-line paths that obey simple rules.

==Limitations==
While the paraxial approximation greatly simplifies optical calculations, it has its limitations. It is only accurate for small angles and does not account for phenomena such as [[diffraction]] and [[aberration]], which become significant in high-precision or wide-angle optical systems. For these cases, more comprehensive models and numerical methods are required to accurately predict the behavior of light.

==Mathematical Formulation==
Mathematically, the paraxial approximation involves simplifying the [[Snell's law]] and the equations for [[curved mirrors]] and lenses. For example, in the case of Snell's law, the approximation \(\sin(\theta) \approx \theta\) is used, where \(\theta\) is the angle of incidence or refraction measured from the normal to the surface.

==See Also==
* [[Geometrical optics]]
* [[Lens (optics)]]
* [[Optical aberration]]
* [[Wave optics]]

==References==
<references/>

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