The electric field \(\mathbf{E}\) and the electric displacement field \(\mathbf{D}\) are related concepts in electromagnetism, particularly in the context of materials. Hereβs how they are related:
1. **Electric Field (\(\mathbf{E}\))**: This is a vector field that represents the force experienced by a unit positive charge placed in a given region of space. It is defined as:
\[
\mathbf{E} = \frac{\mathbf{F}}{q}
\]
where \(\mathbf{F}\) is the force on a test charge \(q\).
2. **Electric Displacement Field (\(\mathbf{D}\))**: This field accounts for the effect of free and bound charge in a material. It is defined in terms of the electric field and the polarization of the material. In a linear, isotropic dielectric material, it is given by:
\[
\mathbf{D} = \varepsilon_0 \mathbf{E} + \mathbf{P}
\]
where \(\varepsilon_0\) is the permittivity of free space and \(\mathbf{P}\) is the polarization vector of the material. In the case of linear dielectrics, this can be simplified to:
\[
\mathbf{D} = \varepsilon \mathbf{E}
\]
where \(\varepsilon\) is the permittivity of the material.
The relationship between \(\mathbf{E}\) and \(\mathbf{D}\) is crucial for understanding how electric fields interact with materials. In free space or in materials without polarization, \(\mathbf{D}\) and \(\mathbf{E}\) are directly proportional, with the proportionality constant being the permittivity of the material. In materials with significant polarization, \(\mathbf{D}\) includes contributions from both the free charges and the bound charges due to polarization.