To understand the behavior of the electric field (\(\vec{E}\)), electric displacement (\(\vec{D}\)), and polarization (\(\vec{P}\)) at the interface between two dielectric materials, let’s go through the concepts systematically:
- At the interface of two dielectrics, the boundary conditions for the normal and tangential components of the electric field and displacement vectors must be considered:
- The normal component of the electric displacement vector \(\vec{D}\) is discontinuous in the presence of a surface charge. The discontinuity is given by the equation: \(D_{1n} - D_{2n} = \sigma_f\), where \(\sigma_f\) is the free surface charge density.
- The polarization \(\vec{P}\) relates to the bound charge, and changes in medium polarization may cause discontinuities in its normal component.
- While discussing \(\vec{E}\), we know that the tangential components of \(\vec{E}\) are continuous, but normal components may differ due to dielectric constants of the materials, making the normal component discontinuous across the boundary.
- Given these equations and boundary conditions, we can reason about the options:
- The claim that the normal component of both \(\vec{D}\) and \(\vec{E}\) are discontinuous can be supported by boundary conditions. Since both are subject to changes at the dielectric boundary, the statement is indeed true.
- Other options can be ruled out because either they propose continuity where there is typically discontinuity or they incorrectly associate properties of different components.
Conclusion: Based on the above analysis, the correct choice is that the normal component of both \(\vec{D}\) and \(\vec{E}\) are discontinuous at the interface of two dielectrics.