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What is the electric susceptibility of a dielectric medium?

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Electric susceptibility (\(\chi_e\)) is a measure of how much a dielectric material becomes polarized when an electric field is applied. It quantifies the extent to which the dielectric material can be polarized by an external electric field, which in turn affects its dielectric properties.

Mathematically, electric susceptibility is defined as the ratio of the polarization \(P\) of the material to the applied electric field \(E\):

\[ \chi_e = \frac{P}{\epsilon_0 E} \]

where:
- \(P\) is the polarization vector of the material,
- \(\epsilon_0\) is the permittivity of free space,
- \(E\) is the applied electric field.

The susceptibility is a dimensionless quantity and is a key parameter in determining the material's relative permittivity \(\epsilon_r\), which is related to the electric susceptibility by:

\[ \epsilon_r = 1 + \chi_e \]

In summary, electric susceptibility describes how a dielectric material responds to an electric field in terms of polarization, and it's crucial for understanding the material's behavior in various electrical and electronic applications.
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Electric susceptibility (\( \chi \)) is a measure of how easily a dielectric material can be polarized by an electric field. It quantifies the relationship between the electric field applied to the material and the resulting polarization within the material. The electric susceptibility is defined as:

\[
\mathbf{P} = \epsilon_0 \chi \mathbf{E}
\]

where:
- \( \mathbf{P} \) is the polarization density (dipole moment per unit volume),
- \( \epsilon_0 \) is the permittivity of free space,
- \( \mathbf{E} \) is the electric field strength.

The electric susceptibility is dimensionless and varies with the type of dielectric material. A higher susceptibility indicates that the material can be polarized more easily, enhancing its ability to store electric energy. It is an important parameter in characterizing dielectric materials and understanding their behavior in electric fields.
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