Ultrasonic attenuation of transverse waves in bonding layers of ultrasonic delay lines with piezoelectric transducers

Ultrasonics ◽  
1972 ◽  
Vol 10 (6) ◽  
pp. 288
1970 ◽  
Vol 33 (8) ◽  
pp. 473-474 ◽  
Author(s):  
C. Bearzatto ◽  
J. Joffrin ◽  
A. Levelut

2012 ◽  
Vol 57 (8) ◽  
pp. 848-852 ◽  
Author(s):  
S. G. Suchkov ◽  
V. P. Kamishkertsev ◽  
S. A. Nikitov ◽  
I. G. Svechnikov

1963 ◽  
Vol 132 (5) ◽  
pp. 2039-2046 ◽  
Author(s):  
Moises Levy ◽  
Reynold Kagiwada ◽  
Isadore Rudnick

1988 ◽  
Vol 142 ◽  
Author(s):  
J.-P. Monchalin ◽  
J.-D. Aussel ◽  
R. Héon ◽  
J. F. Bussière ◽  
P. Bouchard

AbstractSeveral material properties and microstructural features can be determined or monitored by measuring ultrasonic velocity and/or ultrasonic attenuation. Conventional techniques which use piezoelectric transducers for generation and reception have several limitations, in particular in the case of materials at elevated temperature, of samples of complex shapes, and in regard to the detection bandwidth. These limitations are eliminated by laser-ultrasonics, a technique which uses lasers for generation and detection of ultrasound. Following a review of the various principles and methods used for generation and detection, we discuss the use of laserultrasonics for velocity and attenuation measurement. Examples of application to various materials are presented.


2020 ◽  
Vol 10 (15) ◽  
pp. 5265
Author(s):  
Kanji Ono

In this paper, ultrasonic attenuation of the transverse waves of engineering materials is evaluated, covering metals, ceramics, polymers, fiber-reinforced plastics, and rocks. After verifying experimental methods, 273 measurements are conducted and their results are tabulated. Fifty of the tests are for the longitudinal mode. Attenuation behavior is determined over broadband spectra. The attenuation spectra are characterized in four patterns, with 2/3 of the tests showing linear frequency dependence and another ¼ linear spectrum plus Rayleigh scattering (Mason-McSkimin relation). The longitudinal and transverse damping factors varied from 0.004 to 0.065, which are 1/3 to 5 times those of polymethyl methacrylate, suggesting that almost all the engineering materials tested may be viscoelastic. The present test results make the term dynamic viscosity more appropriate for exploring the underlying processes. The observed results were compared between the longitudinal and transverse modes and among similar material types. In more than a half of the tests, the transverse attenuation coefficients were higher than the corresponding longitudinal attenuation coefficients by 1.5× or more. Some material groups had similar attenuation coefficients for the two modes. Since the physical basis for viscous damping is hardly understood, especially in hard solids, further studies from new angles are keenly desired. This collection of new attenuation data will be of value for such works. Practically, this will assist in materials selection and in designing structural health monitoring and non-destructive inspection protocols.


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