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- ...physics]], more specifically in the theory of [[electromagnetism]], the '''displacement current''' is the time derivative of the [[electric displacement]] '''D''' (a [[vec A few years after he had introduced the displacement current, Maxwell realized from the analogy of electricity with an incompressible fl6 KB (972 words) - 16:59, 27 October 2021
- 128 bytes (16 words) - 12:49, 3 July 2008
- Auto-populated based on [[Special:WhatLinksHere/Displacement current]]. Needs checking by a human.679 bytes (86 words) - 16:01, 11 January 2010
Page text matches
- {{r|Displacement current}}781 bytes (105 words) - 09:49, 7 December 2008
- {{r|Displacement current}}668 bytes (81 words) - 17:45, 17 April 2010
- ...physics]], more specifically in the theory of [[electromagnetism]], the '''displacement current''' is the time derivative of the [[electric displacement]] '''D''' (a [[vec A few years after he had introduced the displacement current, Maxwell realized from the analogy of electricity with an incompressible fl6 KB (972 words) - 16:59, 27 October 2021
- ...j''' is defined as the sum of the conduction current density '''i''' and [[displacement current]] (the time derivative of the electric displacement '''D'''). ...the Maxwell equation that is the extension of [[Ampère's equation]] by the displacement current. The equation takes different forms in different systems of units: sometime4 KB (674 words) - 05:17, 23 February 2009
- {{r|Displacement current}}246 bytes (28 words) - 17:57, 5 June 2010
- ...825. Later (1864) it was augmented by [[James Clerk Maxwell]], who added [[displacement current]] to it. This extended form is one of the four [[Maxwell's equations]] that Ampère's law follows from the following [[Maxwell equation]] with zero [[displacement current]]:3 KB (510 words) - 10:16, 16 July 2008
- {{r|Displacement current}}662 bytes (84 words) - 16:47, 11 January 2010
- Auto-populated based on [[Special:WhatLinksHere/Displacement current]]. Needs checking by a human.679 bytes (86 words) - 16:01, 11 January 2010
- {{r|Displacement current}}849 bytes (109 words) - 21:28, 11 January 2010
- {{r|Displacement current}}2 KB (269 words) - 04:51, 22 March 2011
- {{r|Displacement current}}1 KB (141 words) - 11:57, 28 July 2011
- {{r|Displacement current}}1 KB (180 words) - 11:54, 31 December 2022
- {{r|Displacement current}}1 KB (189 words) - 17:55, 17 April 2010
- {{r|Displacement current}}1 KB (196 words) - 05:55, 3 April 2011
- ...nt current is zero. It was J. Clerk Maxwell who recognized the need of the displacement current. ...roversial—contributions to the theory of electromagnetism were the [[displacement current]] and the theoretical discovery of [[electromagnetic wave]]s. Maxwell's sug18 KB (2,680 words) - 18:46, 16 December 2010
- ...'' given in Eq. (1) is a solution of the [[Maxwell equations]] with zero [[displacement current]]. This is of interest as it confirms the generally accepted notion that th11 KB (1,702 words) - 13:31, 22 April 2011
- * time-dependent electric fields (see [[displacement current]]),9 KB (1,330 words) - 16:37, 31 March 2011
- Note that the [[displacement current]] (time derivative of '''E''') is essential in this equation, if it were ab ...ed by the third and fourth Maxwell equation, which express the fact that a displacement current causes a magnetic field, and a changing magnetic field causes an electric f25 KB (3,994 words) - 17:54, 17 April 2010
- ...us consequences: the usual conduction current has to be augmented with a [[displacement current]] and the ether sustains transversal vibrations propagating with a velocity35 KB (5,595 words) - 12:26, 6 September 2013
- ...us consequences: the usual conduction current has to be augmented with a [[displacement current]] and the ether sustains transversal vibrations propagating with a velocity35 KB (5,571 words) - 12:27, 6 September 2013