pardesi
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consider a region where charge is distributed then we have by gauss' law
\nabla \cdot \vec E =\frac{\rho}{\epsilon_{o}}
what is \vec E here.if it is the net electric field then how is that the field is defined at a point where charges are itself present
\nabla \cdot \vec E =\frac{\rho}{\epsilon_{o}}
what is \vec E here.if it is the net electric field then how is that the field is defined at a point where charges are itself present
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