Reflection coefficient
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Ratio of the reflected and transmitted wave to the incident wave are depicted as follows:
where ƒ¡ is the reflection coefficient at the boundary between media-1 and 2:
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We will derive the ratio of the reflected and transmitted wave to incident wave.
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Let 'a1' be a incident wave, 'b1' be a reflected wave and 'a2' be a transmitted wave.

The voltage and current must be continuous at the boundary.
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Here note that the sign of backward current is negative.
Eliminating va2, we obtain the ratio of reflected wave to incident wave voltage, which is defined as reflection coefficient ƒ¡.
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Because Z1,Z2 are positive, the magnitude of the reflection coefficient is less than unity.
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The ratio of current is just different from that of voltage in sign.
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Therefore the reflection coefficient of power is:
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Similarly, eliminating vb1, we obtain the ratio of transmitted wave to the incident wave:
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Note that the power flow satisfies the conservation law of energy.