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The velocity attenuation equation is fitted to forecast the flight distance of EFP.
iii) The numerical examples are considered to compute the propagation characteristics (velocity, attenuation) of each of the four inhomogeneous waves in SAGT medium.
The numerical examples are considered to compute the propagation characteristics (velocity, attenuation) of each of the four inhomogeneous waves in SAGT medium.
Finally, the numerically simulated results regarding phase velocity, attenuation coefficient, specific loss and thermo-mechanical coupling factors of thermoelastic diffusive waves have been obtained and presented graphically.
The plots in Fig. 6 present the percent change in velocity, attenuation amount (Q−1) and attenuation angle due to the presence of pre-stress.
Anisotropy and diffusion effects on the phase velocity, attenuation coefficient and amplitudes of wave propagation are presented graphically in order to illustrate and compare the analytically results.
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The work presented relates the geophysical properties (anisotropy, initial-stress, thermoelasticity) of a realistic medium to its propagation characteristics (velocities, attenuation, polarizations, phase shift, reflection coefficients).
The measured parameters such as ultrasonic velocities, attenuation and elastic constants as a function of temperature reveal the possibility of utilizing the proposed technique for complete characterization of materials over wide range of temperatures.
Finally, the numerical solution is carried out for copper (solvent) and zinc (solute) materials and the obtained phase velocities, attenuation coefficients and specific loss factor of various thermoelastic diffusive waves are presented graphically.
Open image in new window Fig. 5 Velocity and attenuation factor under different fluid density Open image in new window Fig. 6 Velocity and attenuation factor under different fluid viscosity.
The change in conductivity of ZnO NPs induced by pH solutions affects SAW velocity and attenuation.
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