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) ∮ S E ⃗ ⋅ d A ⃗ = q e n c ε 0 \oint_S \vec{E}⋅\vec{dA}= \dfrac {q_{enc}}{ε_0} ∮ S E ⋅ d A = ε 0 q e n c
(Gauss’s law for magnetic fields) ∮ S B ⃗ ⋅ d A ⃗ = 0 \oint_S \vec{B}⋅\vec{dA}=0 ∮ S B ⋅ d A = 0
(Faraday’s law) ∮ C E ⃗ ⋅ d l ⃗ = − d d t ∮ S B ⃗ ⋅ d A ⃗ \oint_C \vec{E}⋅\vec{dl}= -\frac{d}{dt} \oint_S \vec{B}⋅\vec{dA} ∮ C E ⋅ d l = − d t d ∮ S B ⋅ d A
(The Ampere–Maxwell law) ∮ C B ⃗ ⋅ d l ⃗ = μ 0 ( I e n c + ε 0 d d t ∮ S E ⃗ ⋅ d A ⃗ ) \oint_C \vec{B}⋅\vec{dl}= \mu_0( I_{enc}+ε_0\frac{d}{dt} \oint_S \vec{E}⋅\vec{dA} ) ∮ C B ⋅ d l = μ 0 ( I e n c + ε 0 d t d ∮ S E ⋅ d A )
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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