The dielectric constant, often represented by the symbol \( \kappa \) or \( \varepsilon_r \), is a measure of a material's ability to store electrical energy in an electric field. It can be defined in terms of permittivity.
The relationship is given by the formula:
\[
\kappa = \frac{\varepsilon}{\varepsilon_0}
\]
Where:
- \( \kappa \) (or \( \varepsilon_r \)) is the relative permittivity or dielectric constant of the material.
- \( \varepsilon \) is the absolute permittivity of the material.
- \( \varepsilon_0 \) is the permittivity of free space (vacuum), approximately equal to \( 8.854 \times 10^{-12} \, \text{F/m} \).
### Explanation:
- **Permittivity (\( \varepsilon \))**: This is a property of the material that indicates how much electric field is reduced within the material compared to a vacuum.
- **Permittivity of Free Space (\( \varepsilon_0 \))**: This is a constant that represents the capability of a vacuum to permit electric field lines.
The dielectric constant \( \kappa \) is a dimensionless quantity, and it indicates how many times more capable the material is at storing electrical energy compared to a vacuum. For example, a dielectric constant of 2 means that the material can store twice the electric energy of a vacuum under the same electric field conditions.