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For a homogeneous and isotropic medium with a charge density $$\rho$$ & dielectric constant $$\epsilon$$, the Poisson’sequation for electrical potential V is :
$$ \triangledown^{2} V=\frac{\rho}{\epsilon}$$
$$ \triangledown^{2} V=-\frac{\rho}{\epsilon}$$
$$\triangledown.V=\frac{\rho}{\epsilon}$$
$$\triangledown.V=-\frac{\rho}{\epsilon}$$
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