A string of impedance ends in a two-layer stack

PHYSICS · Multi-part · Fermi University Physics · Oscillations, Waves & Acoustics · Superposition, boundaries and interference · Superposition, boundaries and interference

Modes, Packets and Media, Ch Reflection, transmission, matching and tunnelling at boundaries

Problem

A string of impedance Z0=1.0 kg s−1Z_0=1.0\,\mathrm{kg\,s^{-1}} ends in a two-layer stack. The first layer met by the wave has impedance ZA=1.5 kg s−1Z_A=1.5\,\mathrm{kg\,s^{-1}} and is a quarter of a wavelength thick in its own material; behind it, a layer of impedance ZB=2.0 kg s−1Z_B=2.0\,\mathrm{kg\,s^{-1}} is an eighth of a wavelength thick in its own material; the stack is backed by a long string of impedance ZL=4.0 kg s−1Z_{\rm L}=4.0\,\mathrm{kg\,s^{-1}}. ((a)) Find the input impedance ZinZ_{\rm in} presented at the front of the stack. ((b)) Find the fraction RR of the incident power reflected, and compare it with the bare join of Z0Z_0 directly to ZLZ_{\rm L}.

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