Abstract:Let's consider a mechanical stress pulse propagating in an elastic medium. When this pulse encounters a material or phase interface, which generally represents a change of the acoustic impedance, the pulse is split up into two parts. The first part is propagating further into the new material and the second part is reflected. The amplitude ratio of the reflected and the transmitted part is governed by the normalized difference of the acoustic impedance only, provided that the impedance change is a pure step fu… Show more
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