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Ampere's Law

Ampere's Law

Jan 27, 20241 min read

  • Physics

Topics

  • Ampere’s Law in Matter

∮B⋅dl=μ0​∫J⋅dA

  • Integral form
  • Can be derived from differential form using Stoke’s Theorem

∇×B=μ0​(J+ε0​∂t∂E​)

  • B is the magnetic field
  • μ0​ is the magnetic constant
  • ε0​∂t∂E​ is called the Displacement Current

∇×B=μ0​J

  • In the static case

Graph View

  • Topics
  • ∮B⃗⋅dl⃗=μ0∫J⃗⋅ dA⃗\displaystyle \oint\vec{B}\cdot \mathrm{d}\vec{l}={\mu}_{0}\int \vec{J}\cdot \, \mathrm{d}\vec{A}∮B⋅dl=μ0​∫J⋅dA
  • ∇×B⃗=μ0(J⃗+ε0∂E⃗∂t)\displaystyle \nabla \times \vec{B}={\mu}_{0}\left( \vec{J}+{\varepsilon}_{0}\frac{ \partial \vec{E} }{ \partial t } \right)∇×B=μ0​(J+ε0​∂t∂E​)
  • ∇×B⃗=μ0J⃗\displaystyle \nabla \times \vec{B}={\mu}_{0}\vec{J}∇×B=μ0​J

Backlinks

  • Continuity Equation
  • Displacement Current
  • Maxwell's Equations

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