Jump to content

Paraxial approximation

From Wikipedia, the free encyclopedia
This is an old revision of this page, as edited by DrBob (talk | contribs) at 23:23, 8 September 2005 (add stub). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
(diff) ← Previous revision | Latest revision (diff) | Newer revision → (diff)

In geometric optics, the paraxial approximation is an approximation used in ray tracing of light through an optical system (such as a lens).

A paraxial ray is one which makes a small angle (θ) to the optical axis of the system, and lies close to the axis throughout the system. Generally, this allows the approximation (for θ in radians) sin(θ)≈tan(θ)≈θ and cos(θ)≈1 for calculation of the ray's path.

The approximation is known as first-order raytracing or Gaussian optics. Ray transfer matrix analysis is one method that uses the approximation.