Conventionally, ultrasonic techniques extract material features from the echo return which consists of impulse signals convolved with the transfer function of the medium being investigated. In most cases, only a single parameter such as the boundary reflection coefficient, acoustic impedance, or velocity of propagation is used for material identification. For a more complex medium, however, it is desirable to utilize as many parameters as possible from a single trace of echo return to characterize material such that a higher precision of identification can be achieved. The advantage of our approach is that the information obtained is based solely on the echo return from the successive acoustic interfaces without using the signature of the incident pulse which is rather difficult to capture experimentally. An additional feature of this method is that it works rather well even in a noisy environment.>
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King et al. (1993) studied this question.
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