We may find on many textbooks what is resumed here as the four Maxwell's equations on the integral form:
- (Gauss’s law for electric fields) "\\oint_S \\vec{E}\u22c5\\vec{dA}= \\dfrac {q_{enc}}{\u03b5_0}"
- (Gauss’s law for magnetic fields) "\\oint_S \\vec{B}\u22c5\\vec{dA}=0"
- (Faraday’s law) "\\oint_C \\vec{E}\u22c5\\vec{dl}= -\\frac{d}{dt} \\oint_S \\vec{B}\u22c5\\vec{dA}"
- (The Ampere–Maxwell law) "\\oint_C \\vec{B}\u22c5\\vec{dl}= \\mu_0( I_{enc}+\u03b5_0\\frac{d}{dt} \\oint_S \\vec{E}\u22c5\\vec{dA} )"
Reference:
- Fleisch, D. (2008). A student's guide to Maxwell's equations. Cambridge University Press.
- Serway, R. A., & Jewett, J. W. (2018). Physics for scientists and engineers. Cengage learning.
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