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plane waves in lossy material
skin depth reflection
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Maxwell’s equations
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general properties of linear waves
derive linear wave equation c is determined by the media most general solution two forms of energy
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Plane waves in a lossy material
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we cannot neglect the conduction current
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The propagation movie
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Waves in metal
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f=10 GHz
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E H E H X E H
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E H metal X E H
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boundary conditions for time-varying fields
normal D differ by a surface charge density tangential E is continuous normal B is continuous tangential H differ by a surface current density
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E H E H Why? E H
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Etan is continuous E E Htan is continuous X H E H H
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Reflection coefficient
X E H Transmission coefficient
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A pulse propagating from one media to another movie
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impedance meter conductor
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Reflection from a conductor
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Special cases short matched open
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two materials X E H
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Reflection coefficient for wave from left
Transmission coefficient for wave from left
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Reflection coefficient for wave from right
Transmission coefficient for wave from right
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Movie demonstrating reflection and transmission
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F 22 Special cases matched
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