Thin conducting plate boundary conditions

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SUMMARY

The discussion focuses on the boundary conditions for a thin conducting plate in free space, specifically relating the tangential electric and magnetic fields on either side of the conductor. The standard boundary conditions are clarified, emphasizing that the normal components of the electric and magnetic fields do not equate to free charge density or are zero. The relationship between the tangential components of the electric field (\textbf{E}) and magnetic field (\textbf{H}) is critical, as the conditions provided in the initial attempt were incorrect.

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nutan123
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Homework Statement



A thin conductor plate is in free space. Its conductivity is finite and thickness is approaching zero. Relate the tangential electric field in either side of the conductor. Repeat for tangential magnetic field. How are electric and magnetic fields related.

Homework Equations


Standard boundary conditions
[tex]\textbf{n}[/tex]*([tex]\textbf{h2}[/tex]-[tex]\textbf{h1}[/tex])=[tex]\rho[/tex]
[tex]\textbf{n}[/tex]*([tex]\textbf{e2}[/tex]-[tex]\textbf{e1}[/tex])=0


The Attempt at a Solution


Tried to apply the boundary conditions on each of the boundries. However, could not relate the field from both the sides.
 
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nutan123 said:

Homework Statement



A thin conductor plate is in free space. Its conductivity is finite and thickness is approaching zero. Relate the tangential electric field in either side of the conductor. Repeat for tangential magnetic field. How are electric and magnetic fields related.

Are you given any other information, such as the free charge density or free current density on the plate?

Homework Equations


Standard boundary conditions
[tex]\textbf{n}[/tex]*([tex]\textbf{h2}[/tex]-[tex]\textbf{h1}[/tex])=[tex]\rho[/tex]
[tex]\textbf{n}[/tex]*([tex]\textbf{e2}[/tex]-[tex]\textbf{e1}[/tex])=0

Those are not standard boundary conditions. Assuming [itex]\textbf{n}[/itex] represents the surface unit normal, [itex]\textbf{n}\cdot\left(\textbf{E}_2-\textbf{E}_1\right)[/itex] and [itex]\textbf{n}\cdot\left(\textbf{H}_2-\textbf{H}_1\right)[/itex] represent difference in the normal components of the fields...you are asked to relate the tangential components of the fields.

In any case, [itex]\textbf{n}\cdot\left(\textbf{H}_2-\textbf{H}_1\right)\neq\rho[/itex] (I assume [itex]\rho[/itex] is supposed to represent the free surface charge density?) and [itex]\textbf{n}\cdot\left(\textbf{E}_2-\textbf{E}_1\right)\neq 0[/itex] in general.
 

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