"मैक्सवेल के समीकरण": अवतरणों में अंतर

 

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|&emsp;<math>\nabla \cdot \mathbf{E} = \frac {\rho} {\epsilon_0}</math>

|-

|&emsp;<math>\nabla \cdot \mathbf{B} = 0</math>

|-

|&emsp;<math>\nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}} {\partial t}</math>

|-

|&emsp;<math>\nabla \times \mathbf{B} = \mu_0 \mathbf{J} + \mu_0 \epsilon_0 \frac{\partial \mathbf{E}} {\partial t}</math>&emsp;<math></math>

|}