Maxwell's equations
∇・D = ρ
∇・B = 0
∇×E = - ∂B/∂t
∇×H = i + ∂D/∂t
taking divergence of the last equation,
∇・(∇×H ) = 0 = ∇・( i + ∂D/∂t) = ∇・i + ∂(∇・D)/∂t) = ∇・i + ∂ρ/∂t
we get
∇・i + ∂ρ/∂t = 0 (charge conservation)
by way of trial, taking divergence of the third equation,
∇・(∇×E) = - ∂∇・B/∂t
the left is zero using a formula of vector analysis,
the right also zero because ∇・B = 0, the second equation.
the results are trivial.
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