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→In the presence of charges and dielectric media
|width="400"|<math>\boldsymbol{\nabla \times H} - \frac{\partial \boldsymbol{D}}{\partial t}= \boldsymbol{j} </math>
|width="400"|<math>\boldsymbol{\nabla \times H} - \frac{\partial \boldsymbol{D}}{\partial t}= \boldsymbol{j} </math>
|}
|}
<math>\boldsymbol{D = \epsilon_0 E}</math>
<math>\boldsymbol{B = \mu_0 H}</math>