[Electromagnetics] Dielectric boundary condition

In summary, the conversation discusses the concept of closed loop line integration and its application at dielectric boundaries. The reason behind why the value of closed loop line integration is zero at these boundaries is explained, and it is shown that this result is physically justified by the laws of electromagnetism, specifically Faraday's discovery. The conversation also mentions the continuity of tangential electric and magnetic fields at dielectric boundaries, and the result of Snell's law of refraction.
  • #1
kidsasd987
143
4
http://local.eleceng.uct.ac.za/courses/EEE3055F/lecture_notes/2011_old/eee3055f_Ch4_2up.pdf

(Page 4.4 )I am having a trouble with understanding why closed loop line integration is 0 at dielectric boundary.
As far as I know, closed loop line integration is 0 because electric field is conservative.

However, if we have a boundary condition, we'd have two electric vector fields where each has different
permittivity epsilon_1, epsilon_2. and also directional components would be different due to refraction.

If we break down the line integral into two parts of closed loop line integration, one for the top and the other for the bottom dielectric region, the middle boundary part will cancel out and the result Et1=Et2 makes sense.
Also if we do the two closed loop line integration for top and bottom dielectric region, we can show that Et1 and Et2 are equal to the electric field at the boundary for any arbitrary closed loop.*However, it seems a little conunter intuitive to me because E1t and E2t would be diffrent due to refraction. How can I justify the result physically?
 
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  • #2
Look at the first equation on 4-2 right-hand side. The surface integral is zero for an infinitesimally small loop since the surface area can't collect any time-varying B field flux.

A time-varying E-field is not a conservative vector field (it does not have a zero curl). This is in contradiction to electrostatics where the curl of E is always zero. This was one of the major discoveries of Faraday.

I think you are confusing the reason (boundary conditions) with the result (Snell's law of refraction). Remember tangential E (and tangential H) are always continuous on the boundary of homogeneous media without a surface current. The normal components follow as a result.

Of course is you are an electromagnetic purist you would say that the normal components of D and B are always conserved across any interface... :rolleyes:
 

1. What is a dielectric boundary condition?

A dielectric boundary condition is a condition that must be satisfied at the interface between two different materials with different dielectric properties. It describes how an electric field behaves at the boundary between these materials.

2. What is the significance of the dielectric boundary condition?

The dielectric boundary condition is important because it allows us to calculate the electric field and other electromagnetic properties at the interface between two different materials. This is crucial for understanding and predicting the behavior of electromagnetic waves in various situations.

3. How is the dielectric boundary condition derived?

The dielectric boundary condition is derived from Maxwell's equations, specifically the continuity of the electric displacement vector across the boundary. It can also be derived using the principle of conservation of charge.

4. What are the types of dielectric boundary conditions?

There are two types of dielectric boundary conditions: perfect dielectric boundary condition and imperfect dielectric boundary condition. A perfect dielectric boundary condition assumes that there is no surface charge or current at the interface, while an imperfect dielectric boundary condition takes into account any surface charge or current present at the interface.

5. Can the dielectric boundary condition be applied to all materials?

No, the dielectric boundary condition is valid only for materials that exhibit linear and isotropic behavior. This means that the material's dielectric properties do not change with direction or magnitude of an applied electric field.

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