Deriving Wave Equation - Electric Field Inside Metal

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SUMMARY

The discussion focuses on deriving the wave equation for an electromagnetic wave interacting with a metallic surface characterized by conductivity σ. The wave equation is derived from Maxwell's equations, leading to the expression ∇²E = μσ∂E/∂t + με∂²E/∂t². The challenge lies in solving this wave equation for the electric field inside the metal, with hints suggesting the use of separation of variables and Fourier Series methods to incorporate boundary conditions. The propagation depth of the electric field within the metal is also a key consideration.

PREREQUISITES
  • Understanding of Maxwell's Equations in matter
  • Familiarity with vector calculus
  • Knowledge of electromagnetic wave theory
  • Experience with partial differential equations and Fourier Series
NEXT STEPS
  • Study the application of separation of variables in solving partial differential equations
  • Learn about the boundary conditions relevant to electromagnetic waves in conductive materials
  • Explore the concept of skin depth in conductive materials
  • Review the derivation and implications of the wave equation in different media
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Students and professionals in physics and engineering, particularly those focusing on electromagnetism, wave propagation, and materials science.

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Homework Statement



Consider an electromagnetic wave hitting a metallic surface with conductivity σ
at normal incidence.
a) Derive the wave equation describing this situation. Hint: Use Ohm’s law, J = σE to
eliminate the current.
b) Solve the wave equation for the electric field to obtain the electric field inside the metal.
How far into the metal does the field propagate?

Homework Equations



The Maxwell Equations in matter:
[itex]\epsilon\nabla \cdot\vec{E} = \rho_f[/itex]
[itex]\nabla \times \vec{E} = -\mu\dfrac{\partial \vec{H}}{\partial t}[/itex]
[itex]\nabla \cdot \vec{H} = 0[/itex]
[itex]\nabla \times \vec{H} = \sigma\vec{E} + \epsilon \dfrac{\partial \vec{E}}{\partial t}[/itex]

The Attempt at a Solution



By manipulating the maxwell's equations above and using vector calculus, i can obtain the following:

[itex]\nabla^2\vec{E} = \mu\sigma\dfrac{\partial\vec{E}}{\partial t}+\mu\epsilon\dfrac{\partial^2 \vec{E}}{\partial t^2}[/itex] and
[itex]\nabla^2\vec{H} = \mu\sigma\dfrac{\partial\vec{H}}{\partial t}+\mu\epsilon\dfrac{\partial^2 \vec{H}}{\partial t^2}[/itex].

But i can't proceed on with part (b). How do i solve the wave equation for the electirc field? Is the solution to this wave equation exponential?

Thanks!
 
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Hi I solved past year in the course of partial differential equations, I rembember tha we use the separation of variables methods, I will search it, and if a I get I will tell you.
 
Sorry, I forget to say that the way we solved was a Fourier Series, (boundary conditions included)
 

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