Total external reflection: Difference between revisions

Revision as of 20:47, 8 August 2005

Revision as of 08:06, 16 August 2005

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At certain angles, electromagnetic radiation (e.g. visible light) can be ''totally'' reflected from an interface between two media of different indices of refraction (see [[Snell's law]]). [[Total internal reflection]] occurs when the first medium has a larger [[refractive index]] than the second medium, for example, light that emerges from under water. The opticaloptically more dense material (water in this case) is the "internal" medium. For visible light, water has an index of refraction of 1.33 and for air it is very close to 1. For vacuum the index of refraction is exactly 1 for all wavelengths.

For [[X-rays]], however, all materials have indices of refraction slightly below 1. This entails that total reflection of X-rays only can occur when they travel through vacuum and impinge on a surface (at a small glancing angle). Since this kind of total reflection takes place outside of the material it is termed ''total external reflection''.