Experimental dispersion curves of non-penetrable soils from direct dynamic measurements using the seismic dilatometer (SDMT)

2021 ◽  
Vol 143 ◽  
pp. 106616
Author(s):  
Angelo Aloisio ◽  
Ferdinando Totani ◽  
Gianfranco Totani
2013 ◽  
Vol 300-301 ◽  
pp. 955-958
Author(s):  
Pei Hsun Tsai ◽  
Chih Chun Lou

In the paper the shear wave velocity profile is studied using the MASW test. The experimental dispersion curves were obtained from the signal process proposed by Ryden. Theoretical dispersion curve can be constructed by thin layer stiffness matrix method. A real-parameter genetic algorithm is required to minimize the error between the theoretical and experimental dispersion curves. To reduce the error of experimental and theoretical dispersion curve using real-parameter genetic algorithm is feasible. The results show that the soil layers of the study area can be modeled as a sandy fill overlaid on an underlying half space. Test results also show that the asymptotes at high frequencies of the fundamental mode approach the phase velocities for the fill of 190 m/s. The depths of weathered bedrock estimating from dispersion curves match well with that of borehole data.


1965 ◽  
pp. 57-61 ◽  
Author(s):  
JOHN L. YARNELL ◽  
JOHN L. WARREN ◽  
SEYMOUR H. KOENIG

2022 ◽  
Vol 164 ◽  
pp. 108218
Author(s):  
Vijaya V.N. Sriram Malladi ◽  
Mohammad I. Albakri ◽  
Manu Krishnan ◽  
Serkan Gugercin ◽  
Pablo A. Tarazaga

Materials ◽  
2020 ◽  
Vol 13 (6) ◽  
pp. 1436
Author(s):  
Kassahun Demissie Tola ◽  
Dai Quoc Tran ◽  
Byoungjoon Yu ◽  
Seunghee Park

Corrosion detection using a pulsed laser scanning system can be performed via ultrasonic wave propagation imaging. This method outputs illustrations of the wave field within the host structure; thus, it can depict wave–corrosion area interactions. Additionally, post-processing can be performed to enhance the visualization of corroded areas. The wavefield energy computed using RMS (Root Mean Square) is a validated post-processing tool capable of displaying the location and area of corrosion-damaged regions. Nonetheless, to characterize corrosion, it is necessary to determine its depth. The measurement of depth in conjunction with that of the corroded area via the RMS distribution enables the determination of all dimensions of corrosion damage. Thereafter, the flaw severity can be evaluated. This study employed a wavefield within a plate on which corrosion was developed artificially to generate frequency–wavenumber dispersion curves. The curves were compared with their counterparts from a corrosion-free plate. Alternatively, they could be compared with dispersion curves drawn using the depth and material properties of a pristine plate via a computer program. Frequency–wavenumber pairs were extracted from the dispersion curves produced using the portion of the wavefield within the corroded area. These were inserted into the Rayleigh–Lamb equation, from which depths were calculated and averaged.


1967 ◽  
Vol 47 (2) ◽  
pp. 281-293 ◽  
Author(s):  
M. Bini ◽  
L. Millanta ◽  
N. Rubino ◽  
I. Kaufman

1963 ◽  
Vol 1 (6) ◽  
pp. 158
Author(s):  
John L. Yarnell ◽  
John L. Warren ◽  
Seymour H. Koenig

Materials ◽  
2018 ◽  
Vol 11 (11) ◽  
pp. 2219 ◽  
Author(s):  
Sonja Gombar ◽  
Petar Mali ◽  
Milan Pantić ◽  
Milica Pavkov-Hrvojević ◽  
Slobodan Radošević

The dispersion relation for noninteracting excitons and the influence of perturbative corrections are examined in the case of pentacene structure. The values of exchange integrals are determined by nonlinear fits to the experimental dispersion data, obtained by the inelastic electron scattering reported in recent experiments. We obtain theoretical dispersion curves along four different directions in the Brillouin zone which possess the same periodicity as the experimental data. We also show that perturbative corrections are negligible since the exciton gap in the dispersion relation is huge in comparison to the exchange integrals.


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