The electric permittivity of a medium and its dielectric constant are closely related concepts, and understanding their connection helps in studying how materials respond to electric fields.
- Electric Permittivity (\(\varepsilon\)):
- It is a property of a material that describes how much the material resists or permits the formation of an electric field within it.
- The electric permittivity of free space (vacuum) is denoted as \(\varepsilon_0\), and it has a fixed value of \(8.85 \times 10^{-12} \, \text{F/m}\) (farads per meter).
- The electric permittivity of a material is typically written as \(\varepsilon\), and it can be expressed as:
\[
\varepsilon = \varepsilon_0 \cdot \varepsilon_r
\]
where:
- \(\varepsilon_0\) is the permittivity of free space.
- \(\varepsilon_r\) is the
relative permittivity or
dielectric constant of the material.
- Dielectric Constant (\(\varepsilon_r\)):
- It is a dimensionless number that describes how much a material can "store" electric energy compared to vacuum.
- The dielectric constant is the ratio of the permittivity of the material to the permittivity of free space (\(\varepsilon_0\)).
- Mathematically:
\[
\varepsilon_r = \frac{\varepsilon}{\varepsilon_0}
\]
Summary:
- The dielectric constant (\(\varepsilon_r\)) is a ratio of the material's electric permittivity to the permittivity of free space.
- The relationship between them is:
\[
\varepsilon = \varepsilon_0 \cdot \varepsilon_r
\]
In other words, the electric permittivity of a medium is the product of the permittivity of free space and the dielectric constant of the medium.