1980
DOI: 10.1121/1.384507
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Effective area to be used in diffraction corrections

Abstract: Measurements of ultrasonic velocity and attenuation require ’’diffraction corrections’’ for the finite size of the source and receiver. These diffraction corrections depend on the area of the source which is usually taken as the physical area of the piezoelectric element of the the transducer. Measurements are reported which indicate that the effective area of a disk-shaped element may vary with the exciting frequency and may differ by 40% from the physical area of the disk. The method reported may be of value… Show more

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Cited by 45 publications
(11 citation statements)
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“…This same phenomena was noted previously by Amin et al [7] for focussed probes and by Chivers et al' [8] for planar transducers.…”
Section: Effective Transducer Radius and Focal Lengthsupporting
confidence: 70%
See 1 more Smart Citation
“…This same phenomena was noted previously by Amin et al [7] for focussed probes and by Chivers et al' [8] for planar transducers.…”
Section: Effective Transducer Radius and Focal Lengthsupporting
confidence: 70%
“…(19), which can be done with a simple root solver. Also, the above procedure is merely an extension of the methods previously used to determine the effective radius of unfocussed probes [8]. Table 1 shows the results of this method for a typical commercially available focussed probe (Panametrics V309, nominal radius = 0.25 inches, nominal focal length = 4.0 inches, "center" frequency -5 MHz) using a 1/8" diameter steel sphere scanned along the transducer axis.…”
Section: Effective Transducer Radius and Focal Lengthmentioning
confidence: 99%
“…It is also worthwhile to note that these patterns can further be used to calculate an effective diameter of a hydrophone or transmitter. The importance of knowing the effective diameter of the ultrasonic transducers was already pointed out (20).…”
Section: P a Lewinmentioning
confidence: 98%
“…Then the diffraction effect and the attenuation effect can be further separated. The pressure amplitude of the second harmonic is expressed as [7,18] :…”
Section: Measurement Theorymentioning
confidence: 99%
“…Combining the attenuation with the diffraction correction, the model of the measured non-linearity parameter B/A for the finite amplitude insert-substitution method [7,18] is given by:…”
Section: Measurement Theorymentioning
confidence: 99%