Maxwellen ekuazioak: berrikuspenen arteko aldeak
Ezabatutako edukia Gehitutako edukia
t →Kasu orokorra: barne lotura zuzenketak |
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36. lerroa:
| [[Gaussen lege]]a:
| <math>\nabla \cdot \mathbf{D} = \rho</math>
| <!--<math>\oint_S \mathbf{D} \cdot \mathrm{d}\mathbf{A} = q = \int_V \rho\, \mathrm{d}V</math>--><math>\;\iint_S\!\!\!\!\!\!\!\!\!\bigcirc\;\;\;\mathbf D\cdot\mathrm{d}\mathbf A = q = \iiint_V \rho\, \mathrm{d}V</math>
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| Gaussen legea magnetismorako<br /> (monopolo magnetikorik ez dagoenaren frogapena):
| <math>\nabla \cdot \mathbf{B} = 0</math>
| <!--<math>\oint_S \mathbf{B} \cdot \mathrm{d}\mathbf{A} = 0</math>--><math>\;\iint_S\!\!\!\!\!\!\!\!\!\bigcirc\;\;\;\mathbf B\cdot\mathrm{d}\mathbf A = 0</math>
|-
| [[Faradayren legea|Faraday-ren indukzio legea]]:
| <math>\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}} {\partial t}</math>
| <math>\oint_C \mathbf{E} \cdot \mathrm{d}\mathbf{l} = - \
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| [[Ampère-Maxwell legea]]:
| <math>\nabla \times \mathbf{H} = \mathbf{J} + \frac{\partial \mathbf{D}} {\partial t}</math>
| <math>\oint_C \mathbf{H} \cdot \mathrm{d}\mathbf{l} = \
\
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