The
permittivity of a dielectric material is a property that describes how much electric field is "permitted" or allowed to pass through that material. It essentially tells us how easily a material can become polarized in response to an applied electric field.
In simple terms, when you apply an electric field to a dielectric material (like air, rubber, glass, etc.), the material doesn't conduct electricity (unlike metals) but it does affect the electric field. The permittivity quantifies the material's ability to store electric energy when an electric field is applied.
Two Key Types of Permittivity:
- Absolute Permittivity (ε): This is the actual permittivity of the material and depends on the material's properties.
\[
\varepsilon = \varepsilon_0 \times \varepsilon_r
\]
where:
- \(\varepsilon_0\) is the permittivity of free space (vacuum), approximately \(8.854 \times 10^{-12}\ \text{F/m}\) (farads per meter).
- \(\varepsilon_r\) is the relative permittivity or dielectric constant, which compares the permittivity of the material to the permittivity of free space.
- Relative Permittivity (εr): This is a dimensionless number that tells you how much more or less a material can store electric energy compared to a vacuum. For example, if \(\varepsilon_r = 2\), it means the material can store twice as much energy as a vacuum under the same electric field.
Why is Permittivity Important?
- Capacitance: In capacitors, the permittivity of the dielectric material between the plates directly affects the capacitance. A higher permittivity results in a higher capacitance.
- Electric Fields: Permittivity helps determine how the electric field behaves inside materials, influencing how electric forces act in different media.
In simple terms, the higher the permittivity of a dielectric, the better it can store energy in the presence of an electric field.