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∇⋅E=ρϵ0 \nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} ∇⋅B=0 \nabla \cdot \mathbf{B} = 0

∇×E=−∂B∂t \nabla \times \mathbf{E} = - \frac{\partial \mathbf{B}}{\partial t}

∇×B=μ0J+μ0ϵ0∂E∂t \nabla \times \mathbf{B} = \mu_0\mathbf{J} +\mu_0\epsilon_0 \frac{\partial \mathbf{E}}{\partial t}