In a medium of dielectric constant $K$, the electric field is $\vec E$ . If ${ \varepsilon _0}$ is permittivity of the free space, the electric displacement vector is
In a medium of dielectric constant $K$, the electric field is $\vec E$ . If ${ \varepsilon _0}$ is permittivity of the free space, the electric displacement vector is
- [AIIMS 2014]
- A
$\frac{{K\vec E}}{{{ \in _0}}}$
- B
$\frac{{\vec E}}{{K\,{ \in _0}}}$
- C
$\frac{{{ \in _0}\,\vec E}}{K}$
- D
$K\,{ \in _0}\,\vec E$
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- [AIPMT 2015]
How does the polarised dielectric modify the original external field inside it ?
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