Difference between revisions of "Dictionary:Electric field"
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− | <center> <math>\nabla \times {\mathbf E } = - \frac{\partial {\mathbf B }}{\partial t}. | + | <center> <math>\nabla \times {\mathbf E } = - \frac{\partial {\mathbf B }}{\partial t}. </math> </center> |
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+ | See a classic text, such as Jackson (1962) <ref> Jackson, J. D. (1962). Classical electrodynamics (Vol. 3). New York etc.: Wiley.</ref> | ||
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+ | ==References == | ||
+ | <references /> |
Revision as of 16:48, 25 June 2015
A spatial vector quantity equal to a potential gradient, produced by charged bodies or a time-varying magnetic field. Unit is volts per meter. The electric field induced in a loop equals the negative time derivative of the magnetic flux cutting the loop ( is a length element of the loop):
It is also expressed in terms of the change in the magnetic induction with time :
See a classic text, such as Jackson (1962) [1]
References
- ↑ Jackson, J. D. (1962). Classical electrodynamics (Vol. 3). New York etc.: Wiley.