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- from which the Clausius-Mossotti relation follows directly.7 KB (1,105 words) - 10:55, 11 June 2009
- 181 bytes (24 words) - 06:04, 10 December 2008
- Auto-populated based on [[Special:WhatLinksHere/Clausius-Mossotti relation]]. Needs checking by a human.572 bytes (69 words) - 11:55, 11 January 2010
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- Auto-populated based on [[Special:WhatLinksHere/Clausius-Mossotti relation]]. Needs checking by a human.572 bytes (69 words) - 11:55, 11 January 2010
- {{r|Clausius-Mossotti relation}}661 bytes (85 words) - 19:37, 11 January 2010
- {{r|Clausius-Mossotti relation}}606 bytes (73 words) - 18:10, 11 January 2010
- {{r|Clausius-Mossotti relation}}730 bytes (91 words) - 15:58, 11 January 2010
- {{r|Clausius-Mossotti relation}}923 bytes (114 words) - 17:36, 17 April 2010
- {{r|Clausius-Mossotti relation}}668 bytes (81 words) - 17:45, 17 April 2010
- The Lorentz-Lorenz law follows from the [[Clausius-Mossotti relation]] by using that the index of refraction ''n'' is approximately (for non-con3 KB (478 words) - 08:14, 11 December 2008
- {{r|Clausius-Mossotti relation}}1 KB (141 words) - 11:57, 28 July 2011
- from which the Clausius-Mossotti relation follows directly.7 KB (1,105 words) - 10:55, 11 June 2009
- {{r|Clausius-Mossotti relation}}2 KB (269 words) - 04:51, 22 March 2011
- ...the [[Free_space_(electromagnetism)#Classical_case|classical vacuum]]. A [[Clausius-Mossotti relation|refractive index]] of the medium larger than one slows the light.34 KB (5,178 words) - 10:12, 28 February 2024