PlanetPhysics/Fermat's Principle: Difference between revisions
imported>MathXplore m MathXplore moved page PlanetPhysics/Fermats Principle to PlanetPhysics/Fermat's Principle without leaving a redirect: Misspelled title |
(No difference)
|
Latest revision as of 14:23, 10 October 2023
\newcommand{\sqdiagram}[9]{Failed to parse (unknown function "\diagram"): {\displaystyle \diagram #1 \rto^{#2} \dto_{#4}& \eqno{\mbox{#9}}} }
Fermat's Principle
Initially conceived in optics, Fermat's principle was stated as the principle of least time for traveling light [[../CosmologicalConstant2/|waves]], that is the path or paths taken between two points by light which can be traversed in the least time; in an Euclidean space or a flat Minkowski space, this is the straight line defined by a single ray of light. This can be thought as the trajectory of an emitted photon traveling at the universal maximum [[../Velocity/|speed]] in vacuum. In a Riemannian or Minkowski [[../SR/|spacetime]] this corresponds to the surface of a light cone.
In general relativity, however, a [[../CenterOfGravity/|point particle]] path is a [[../GeodesicEquation/|geodesic]] curve in a Riemannian space that can be curved, for example, by the presence of intense gravitational [[../CosmologicalConstant2/|fields]]. One such effect was observed and reported by modern astrophysicists and is called gravitational lensing .