26.11
Current density becomes discontinuous across an interface of materials with different electrical conductivities. The normal component of the current d…
The current density becomes discontinuous across an interface having different electrical conductivities.
For steady currents, the divergence of the current density is zero. So, the normal component of the current density is continuous across the boundary.
Recall that the tangential component of the electric field is continuous across an interface. Expressing the electric field in terms of the current density and the electrical conductivity gives the boundary condition for the tangential component of the current density.
Now, the normal component of the electric displacement is discontinuous across the interface. So, the normal component of the electric field is also discontinuous across an interface.
Again, using the expression of the electric field and current density, the boundary condition for the normal component of the current density is obtained in terms of permittivity and conductivity.
It shows that a surface charge density is created across an interface having different conductivities and/or permittivities.
The surface charge density is zero for an interface with the same conductivity and permittivity values or with an equal ratio of permittivity to conductivity.
View the full transcript and gain access to JoVE Core videos
Q1: Why is the normal component of current density continuous across a boundary?
For steady currents, the divergence of current density is zero, which means no charge accumulates at the interface. This mathematical constraint requires the normal component of current density to remain continuous across the boundary between two conducting media, even when their electrical conductivities differ.
Q2: What happens to the tangential component of current density at an interface?
The tangential component of current density becomes discontinuous across an interface with different electrical conductivities. Since the tangential component of the electric field is continuous, the tangential current density changes based on the ratio of conductivities in each medium, causing the current to refract at the boundary.
Q3: How does current density refract when crossing materials with different conductivities?
Current density refracts at an interface similar to light refraction. The angle the current makes with the normal changes based on the conductivity ratio of the two media. If one medium has higher electrical conductivity, the current bends toward the normal, becoming more perpendicular to the surface.
Q4: When is surface charge density created at an interface between two conductors?
Surface charge density forms at an interface when the materials have different conductivities and/or permittivities. However, no surface charge develops if both media share identical conductivity and permittivity values or maintain an equal ratio of permittivity to conductivity, resulting in charge-neutral boundaries.
Q5: How do permittivity and conductivity affect the normal component of current density?
The boundary condition for the normal component of current density depends on both permittivity and conductivity of the adjacent media. The normal electric field becomes discontinuous across the interface due to differences in these properties, directly determining how the normal current density component changes at the boundary.
Q6: What is the relationship between electric field and current density at a boundary?
Electric field and current density are related through electrical conductivity at material boundaries. Expressing the electric field in terms of current density and conductivity reveals boundary conditions for both tangential and normal components, showing how current behavior changes across interfaces with different material properties.
Q7: What determines the angle of current density relative to the normal at an interface?
The angle between current density and the normal at an interface is determined by the conductivity ratio of the two media. When one medium has significantly higher conductivity, the current density approaches the normal direction. This relationship allows prediction of current path changes when crossing boundaries between materials with different electrical properties.