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Journal articles on the topic 'Viscoelastic waves'

Author: Grafiati

Published: 2 June 2025

Last updated: 31 July 2025

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1

Akhmedov, Sh R., B. S. Rakhmonov, I. M. Karimov, A. M. Marasulov, and Sh I. Zhuraev. "Exposure to acoustic waves on viscoelastic cylinder." E3S Web of Conferences 401 (2023): 05024. http://dx.doi.org/10.1051/e3sconf/202340105024.

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The problem of the impact of acoustic waves in a homogeneous viscoelastic cylinder is considered. The investigation aims to investigate the diffraction of acoustic harmonic waves in a viscoelastic cylinder. The body is assumed to be in an infinite acoustic space filled with an ideal fluid. Numerical calculations of the angular and frequency characteristics of the scattered field for viscoelastic cylinders under the action of harmonic acoustic waves are carried out. In the case of steady waves, the Helmholtz equation describes the propagation of small disturbances in an acoustic medium. And in

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2

Romeo, Maurizio. "Interfacial viscoelastic SH waves." International Journal of Solids and Structures 40, no. 9 (2003): 2057–68. http://dx.doi.org/10.1016/s0020-7683(03)00062-3.

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3

Berezin, Y. A., and K. Hutter. "Waves on viscoelastic films." Rheologica Acta 44, no. 1 (2004): 112–18. http://dx.doi.org/10.1007/s00397-004-0397-0.

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4

Jones, H. W., H. W. Kwan, and E. Yeatman. "Surface waves in viscoelastic fluid." Journal of the Acoustical Society of America 82, S1 (1987): S101. http://dx.doi.org/10.1121/1.2024527.

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5

PIPKIN, ALLEN C. "ASYMPTOTIC BEHAVIOUR OF VISCOELASTIC WAVES." Quarterly Journal of Mechanics and Applied Mathematics 41, no. 1 (1988): 51–69. http://dx.doi.org/10.1093/qjmam/41.1.51.

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6

Caviglia, Giacomo, Angelo Morro, and Enrico Pagani. "Inhomogeneous waves in viscoelastic media." Wave Motion 12, no. 2 (1990): 143–59. http://dx.doi.org/10.1016/0165-2125(90)90035-3.

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7

Addy, Sushil Kumar, and Nil Ratan Chakraborty. "Rayleigh waves in a viscoelastic half-space under initial hydrostatic stress in presence of the temperature field." International Journal of Mathematics and Mathematical Sciences 2005, no. 24 (2005): 3883–94. http://dx.doi.org/10.1155/ijmms.2005.3883.

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The effect of the temperature and initial hydrostatic stress has been shown on the propagation of Rayleigh waves in a viscoelastic half-space. It has been explained how the velocity of Rayleigh waves depends not only on the parameters pertaining to the viscoelastic properties of the half-space, but on the temperature and the initial hydrostatic stress of the half-space also. The variations of the phase velocity of Rayleigh waves in dimensionless form with respect to the magnitude of the initial hydrostatic stress under certain practical assumptions have been depicted in graphs after numerical

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8

Hu, Ning, Maofa Wang, Baochun Qiu, and Yuanhong Tao. "Numerical Simulation of Elastic Wave Field in Viscoelastic Two-Phasic Porous Materials Based on Constant Q Fractional-Order BISQ Model." Materials 15, no. 3 (2022): 1020. http://dx.doi.org/10.3390/ma15031020.

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The fractional-order differential operator describes history dependence and global correlation. In this paper, we use this trait to describe the viscoelastic characteristics of the solid skeleton of a viscoelastic two-phasic porous material. Combining Kjartansson constant Q fractional order theory with the BISQ theory, a new BISQ model is proposed to simulate elastic wave propagation in a viscoelastic two-phasic porous material. The corresponding time-domain wave propagation equations are derived, and then the elastic waves are numerically simulated in different cases. The integer-order deriva

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9

Tavakoli, Sasan, Luofeng Huang, Fatemeh Azhari, and Alexander V. Babanin. "Viscoelastic Wave–Ice Interactions: A Computational Fluid–Solid Dynamic Approach." Journal of Marine Science and Engineering 10, no. 9 (2022): 1220. http://dx.doi.org/10.3390/jmse10091220.

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A computational fluid–solid dynamic model is employed to simulate the interaction between water waves and a consolidated ice cover. The model solves the Navier–Stokes equations for the ocean-wave flow around a solid body, and the solid behavior is formalized by the Maxwell viscoelastic model. Model predictions are compared against experimental flume tests of waves interacting with viscoelastic plates. The decay rate and wave dispersion predicted by the model are shown to be in good agreement with experimental results. Furthermore, the model is scaled, by simulating the wave interaction with an

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10

Wagner, C., H. W. Müller, and K. Knorr. "Faraday Waves on a Viscoelastic Liquid." Physical Review Letters 83, no. 2 (1999): 308–11. http://dx.doi.org/10.1103/physrevlett.83.308.

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11

Carcione, José M. "Rayleigh waves in isotropic viscoelastic media." Geophysical Journal International 108, no. 2 (1992): 453–64. http://dx.doi.org/10.1111/j.1365-246x.1992.tb04628.x.

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12

Li, Qingchun, and Jacek Jarzynski. "Torsional waves in a viscoelastic layer." Journal of the Acoustical Society of America 105, no. 2 (1999): 1190. http://dx.doi.org/10.1121/1.425613.

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13

Destrade, M., P. M. Jordan, and G. Saccomandi. "Compact travelling waves in viscoelastic solids." EPL (Europhysics Letters) 87, no. 4 (2009): 48001. http://dx.doi.org/10.1209/0295-5075/87/48001.

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14

Gubaidullin, D. A., and A. A. Nikiforov. "Acoustic Waves in Viscoelastic Bubbly Media." High Temperature 57, no. 1 (2019): 133–36. http://dx.doi.org/10.1134/s0018151x1806010x.

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15

Ramos, J. I. "Shock waves of viscoelastic Burgers equations." International Journal of Engineering Science 149 (April 2020): 103226. http://dx.doi.org/10.1016/j.ijengsci.2020.103226.

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16

Ostoja-Starzewski, Martin, and Luis Costa. "Shock waves in random viscoelastic media." Acta Mechanica 223, no. 8 (2012): 1777–88. http://dx.doi.org/10.1007/s00707-012-0658-4.

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17

Caviglia, Giacomo, Angelo Morro, and Enrico Pagani. "Time-harmonic waves in viscoelastic media." Mechanics Research Communications 16, no. 1 (1989): 53–58. http://dx.doi.org/10.1016/0093-6413(89)90011-6.

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18

Johannesmann, Sarah, Leander Claes, and Bernd Henning. "Lamb wave based approach to the determination of elastic and viscoelastic material parameters." tm - Technisches Messen 88, s1 (2021): s28—s33. http://dx.doi.org/10.1515/teme-2021-0070.

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Abstract In this paper a measurement procedure is presented to identify both elastic and viscoelastic material parameters of plate-like samples using broadband ultrasonic waves. These Lamb waves are excited via the thermoelastic effect using laser radiation and detected by a piezoelectric transducer. The resulting measurement data is transformed to yield information about multiple propagating Lamb waves as well as their attenuation. These results are compared to simulation results in an inverse procedure to identify the parameters of an elastic and a viscoelastic material model.

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19

Gupta, Asit Kumar, and Pulak Patra. "Influence of gravity on torsional surface waves in a dissipative medium." Geofísica Internacional 60, no. 1 (2021): 1–13. http://dx.doi.org/10.22201/igeof.00167169p.2021.60.1.1916.

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The present paper deals with the possibilities of propagation of torsional surface waves in a viscoelastic medium under gravity field. During the study it will observe that the increase in gravity parameter will increase the velocity of the wave, the increase in viscoelastic parameter, decrease the velocity of the wave until the product of angular frequency and viscoelastic parameter is less than unity. It also notes that as the velocity increases, the curve becomes asymptotic in nature when the period of oscillation increases. In fact the maximum damping in velocity has been identified at thi

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20

Guo, Qing, Hongbo Liu, Guoliang Dai, and Zhongwei Li. "Bulk and Rayleigh Waves Propagation in Three-Phase Soil with Flow-Independent Viscosity." Applied Sciences 12, no. 14 (2022): 7166. http://dx.doi.org/10.3390/app12147166.

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The flow-independent viscosity of the soil skeleton has significant influence on the elastic wave propagation in soils. This work studied the bulk and Rayleigh waves propagation in three-phase viscoelastic soil by considering the contribution of the flow-independent viscosity from the soil skeleton. Firstly, the viscoelastic dynamic equations of three-phase unsaturated soil are developed with theoretical derivation. Secondly, the explicit characteristic equations of bulk and Rayleigh waves in three-phase viscoelastic soil are yielded theoretically by implementing Helmholtz resolution for the d

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21

Liu, Xu, Stewart Greenhalgh, Manjeet Kumar, et al. "Reflection and transmission coefficients of spherical waves at an interface separating two dissimilar viscoelastic solids." Geophysical Journal International 230, no. 1 (2022): 252–71. http://dx.doi.org/10.1093/gji/ggac071.

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SUMMARY Spherical wave reflection and transmission (R/T) coefficients at an interface are not only of theoretical significance but also play an important role in the amplitude variation with offset (AVO) analysis of wide-angle reflection seismic data and cross-borehole surveys. For sources close to the interface the resulting wavefields cannot be adequately described in terms of a single incident plane wave. Rather, the spherical waves must be viewed as the superposition of an infinite number of plane waves. Moreover, the R/T coefficients for each individual plane wave in viscoelastic media ha

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22

Gad-el-Hak, Mohamed. "The Response of Elastic and Viscoelastic Surfaces to a Turbulent Boundary Layer." Journal of Applied Mechanics 53, no. 1 (1986): 206–12. http://dx.doi.org/10.1115/1.3171714.

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The unstable response of elastic and viscoelastic surfaces to a turbulent boundary layer was experimentally investigated in an 18-m towing tank. The compliant surface deformation was measured using a remote optical technique. The “Laser Displacement Gauge” employs a Reticon camera equipped with a linear array of 256 photodiodes spaced 25 microns apart. The device was used to measure the characteristics of two classes of hydroelastic instability waves that form on elastic or viscoelastic surfaces as a reuslt of the interaction with a turbulent boundary layer. The instability waves developing on

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23

Xu, Ying, Shuang Zhang, Linfeng Zhou, Haoran Ning, and Kai Wu. "Dynamic Behavior and Mechanism of Transient Fluid–Structure Interaction in Viscoelastic Pipes Based on Energy Analysis." Water 16, no. 11 (2024): 1468. http://dx.doi.org/10.3390/w16111468.

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The term “viscoelastic pipe” refers to high polymer pipes that exhibit both elastic and viscoelastic properties. Owing to their widespread use in water transport systems, it is important to understand the transient flow characteristics of these materials for pipeline safety. Despite extensive research, these characteristics have not been sufficiently explored. This study evaluates the impact of friction models on the transient flow of viscoelastic pipes across various Reynolds numbers by employing an energy analysis approach. Given the complexity and computational demands of two-dimensional mo

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24

Krebes, E. S., and D. J. Hearn. "On the geometrical spreading of viscoelastic waves." Bulletin of the Seismological Society of America 75, no. 2 (1985): 391–96. http://dx.doi.org/10.1785/bssa0750020391.

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Abstract Krebes and Hron (1980) derived a formula for the geometrical spreading factor L for a seismic wave propagating through a layered viscoelastic medium. They assumed the angle γ0 between the propagation and attenuation vectors of the initial ray segment was constant. In this paper, the general formula for L is derived, in which γ0 is a function of the take-off angle θ0 (the functional form depends on source conditions). For the special case γ0 = θ0, which corresponds, for example, to an air-shot source just above the surface, the formula for L simplifies considerably. A few numerical eva

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25

Sharifineyestani, Elham, and Navid Tahvildari. "A NUMERICAL STUDY ON SURFACE WAVE EVOLUTION OVER VISCOELASTIC MUD." Coastal Engineering Proceedings, no. 36 (December 30, 2018): 64. http://dx.doi.org/10.9753/icce.v36.waves.64.

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A numerical modeling approach is applied to investigate the combined effect of wave-current-mud on the evolution of nonlinear waves. A frequency-domain phase-resolving wave-current model that solves nonlinear wave-wave interactions is used to solve wave evolution. A comparison between the results of numerical wave model and the laboratory experiments confirms the accuracy of the numerical model. The model is then applied to consider the effect of mud properties on nonlinear surface wave evolution. It is shown that resonance effect in viscoelastic mud creates a complex frequency-dependent dissi

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26

Hosking, R. J., A. D. Sneyd, and D. W. Waugh. "Viscoelastic response of a floating ice plate to a steadily moving load." Journal of Fluid Mechanics 196 (November 1988): 409–30. http://dx.doi.org/10.1017/s0022112088002757.

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Viscoelastic theory is used to describe the response of a floating ice sheet to a moving vehicle. We adopt a two-parameter memory function to describe the behaviour of the ice, subjected to a steadily moving line or point load. The viscoelastic dissipation produces an asymmetric quasi-static response at subcritical speed, renders a finite response at the critical speed, and damps the shorter leading waves rather more severely than the longer trailing waves at supercritical speed. We extend earlier asymptotic theory to consider the anisotropic damping of the flexural waves. There is enhanced ag

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27

Levin, Vladimir A., Anatoly V. Vershinin, and Konstantin M. Zingerman. "Numerical Analysis of Propagation of Nonlinear Waves in Prestressed Solids." Modern Applied Science 10, no. 4 (2016): 158. http://dx.doi.org/10.5539/mas.v10n4p158.

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<p>The details of numerical algorithms implemented in CAE FIDESYS for the analysis of the propagation of nonlinear waves in elastic and viscoelastic bodies are discussed. It’s taken into account that waves propagation lead to new strains which superimpose on existing stresses (induced anisotropy) in the media. For the formulation of problem we used the theory of repeated superposition of large strains. The details of numerical algorithms for the analysis of the propagation of nonlinear waves in elastic and viscoelastic bodies are discussed. The implementation of the spectral element meth

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28

Červený, Vlastislav, and Ivan Pšenčík. "Boundary attenuation angles for inhomogeneous plane waves in anisotropic dissipative media." GEOPHYSICS 76, no. 3 (2011): WA51—WA62. http://dx.doi.org/10.1190/1.3555174.

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We study behavior of attenuation (inhomogeneity) angles [Formula: see text], i.e., angles between real and imaginary parts of the slowness vectors of inhomogeneous plane waves propagating in isotropic or anisotropic, perfectly elastic or viscoelastic, unbounded media. The angle [Formula: see text] never exceeds the boundary attenuation angle [Formula: see text]. In isotropic viscoelastic media [Formula: see text]; in anisotropic viscoelastic media [Formula: see text] may be greater than, equal to, or less than [Formula: see text]. Plane waves with [Formula: see text] do not exist. Because [For

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29

Magdenkov, Vladimir A. "The New Type of Constrained Vibration-Damping Coating." Journal of Low Frequency Noise, Vibration and Active Control 15, no. 3 (1996): 107–13. http://dx.doi.org/10.1177/026309239601500301.

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Samples of new self-adhesive, constrained vibration-damping coatings (VDC) and layers for “sandwich” type plates for damping flexural waves in plates are described. These coatings consist of aluminium foil, perforated cardboard and layers of self-adhesive viscoelastic material. The results of measurements of the temperature-frequency characteristics of the loss factor of flexural waves in plates which are damped with these coatings are given. Methods of calculation of viscoelastic characteristics of multi-layer constructions are considered. The peculiarities of use of constrained and hard vibr

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30

Deep, Shikha, and Sandeep Kumar Paul. "An analytical approach for Love wave disper¬sion in a viscoelastic layer lying on an elastic layer with imperfect interface: under stress-free and clamped boundary conditions." Structural Integrity and Life 25, Special Issue A (2025): S35—S43. https://doi.org/10.69644/ivk-2025-sia-0035.

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The problem is investigated on the propagation of Love type waves in a geometrical configuration composed of an inhomogeneous viscoelastic layer lying over an elastic substrate. The viscoelastic layer and an isotropic substrate are imperfectly attached to each other. An analysis is done in two cases, first, when the top surface of viscoelastic layer is stress-free, and second, when it is clamped. The dispersion and damping relations for both stress-free and clamped cases are separately determined through the use of effective boundary conditions. A special case is also derived when the viscoela

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31

Guo, Peng, George A. McMechan, and Li Ren. "Modeling the viscoelastic effects in P-waves with modified viscoacoustic wave propagation." GEOPHYSICS 84, no. 6 (2019): T381—T394. http://dx.doi.org/10.1190/geo2018-0747.1.

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Accurate full-waveform seismic modeling is a powerful tool for understanding wave propagation and building subsurface images. However, it can be computationally expensive for viscoelastic media. Viscoacoustic seismic modeling is much cheaper, but at the trade-off of using incomplete physics. We have developed a modified viscoacoustic wave simulation algorithm for modeling the viscoelastic effects of P-waves. The algorithm contains two viscoacoustic forward-modeling steps; the first is the same as the traditional viscoacoustic modeling, whereas the second propagation is generated using a residu

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32

Kakar, Rajneesh, Kanwaljeet Kaur, and Kishan Chand Gupta. "Study of viscoelastic model for harmonic waves in non-homogeneous viscoelastic filaments." Interaction and multiscale mechanics 6, no. 1 (2013): 31–50. http://dx.doi.org/10.12989/imm.2013.6.1.031.

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33

Proskuriakov, N. E., and I. V. Lopa. "LONGITUDINAL STRESS WAVES IN VISCOELASTIC PLASTIC RODS." Dynamics of Systems, Mechanisms and Machines 7, no. 1 (2019): 136–41. http://dx.doi.org/10.25206/2310-9793-7-1-136-141.

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34

Sharma, M. D. "Rayleigh Waves in Dissipative Poro-Viscoelastic Media." Bulletin of the Seismological Society of America 102, no. 6 (2012): 2468–83. http://dx.doi.org/10.1785/0120120003.

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35

Warhola, G. T., and A. C. Pipkin. "Approximations for Steady Waves in Viscoelastic Materials." Journal of Applied Mechanics 56, no. 3 (1989): 715–17. http://dx.doi.org/10.1115/1.3176154.

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36

Bielak, Jacobo. "Book Review: Viscoelastic Waves in Layered Media." Earthquake Spectra 26, no. 3 (2010): 901–3. http://dx.doi.org/10.1193/1.3459161.

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37

Kumar, Satish. "Parametrically driven surface waves in viscoelastic liquids." Physics of Fluids 11, no. 8 (1999): 1970–81. http://dx.doi.org/10.1063/1.870061.

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38

Shuvalov, A. "On the properties of homogeneous viscoelastic waves." Quarterly Journal of Mechanics and Applied Mathematics 52, no. 3 (1999): 405–17. http://dx.doi.org/10.1093/qjmam/52.3.405.

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39

Abu Alshaikh, Ibrahim, Dogan Turhan, and Yalcin Mengi. "Transient waves in viscoelastic cylindrical layered media." European Journal of Mechanics - A/Solids 21, no. 5 (2002): 811–30. http://dx.doi.org/10.1016/s0997-7538(02)01238-x.

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40

Liapidevskii, V. Yu, V. V. Pukhnachev, and A.Tani. "Nonlinear waves in incompressible viscoelastic Maxwell medium." Wave Motion 48, no. 8 (2011): 727–37. http://dx.doi.org/10.1016/j.wavemoti.2011.04.002.

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41

Ivanov, Ts P., and R. Savova. "Viscoelastic surface waves of an assigned wavelength." European Journal of Mechanics - A/Solids 24, no. 2 (2005): 305–10. http://dx.doi.org/10.1016/j.euromechsol.2004.11.002.

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42

Konjik, Sanja, Ljubica Oparnica, and Dusan Zorica. "Waves in fractional Zener type viscoelastic media." Journal of Mathematical Analysis and Applications 365, no. 1 (2010): 259–68. http://dx.doi.org/10.1016/j.jmaa.2009.10.043.

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43

Burridge, Robert, Maarten V. de Hoop, Kai Hsu, Lawrence Le, and Andrew Norris. "Waves in stratified viscoelastic media with microstructure." Journal of the Acoustical Society of America 94, no. 5 (1993): 2884–94. http://dx.doi.org/10.1121/1.408230.

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44

Gladden, J. R., C. E. Skelton, and J. Mobley. "Shear waves in viscoelastic wormlike micellar fluids." Journal of the Acoustical Society of America 128, no. 5 (2010): EL268—EL273. http://dx.doi.org/10.1121/1.3492794.

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45

Sugimoto, N., and T. Kakutani. "‘Generalized Burgers' equation’ for nonlinear viscoelastic waves." Wave Motion 7, no. 5 (1985): 447–58. http://dx.doi.org/10.1016/0165-2125(85)90019-8.

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46

Scalia, Antonio. "Shock waves in viscoelastic materials with voids." Wave Motion 19, no. 2 (1994): 125–33. http://dx.doi.org/10.1016/0165-2125(94)90061-2.

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47

Yu, J. G., F. E. Ratolojanahary, and J. E. Lefebvre. "Guided waves in functionally graded viscoelastic plates." Composite Structures 93, no. 11 (2011): 2671–77. http://dx.doi.org/10.1016/j.compstruct.2011.06.009.

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48

Pshenichnov, S. G. "WAVES IN AN INHOMOGENEOUS VISCOELASTIC HOLLOW SPHERE." Problems of Strength and Plasticity 87, no. 1 (2025): 103–12. https://doi.org/10.32326/1814-9146-2025-87-1-103-112.

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The problem of propagation of nonstationary longitudinal waves in a sphere with a concentric cavity consisting of homogeneous viscoelastic spherical layers with continuity conditions for displacement and normal stresses at the boundaries between the contacting layers is solved. A uniformly distributed normal load acts on the surface of the sphere, the cavity remains free. The solution of the problem is constructed using the integral Laplace transform in time. The solution in originals is presented in a new form, which is especially convenient for numerical implementation with a large number of

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49

Groos, Lisa, Martin Schäfer, Thomas Forbriger, and Thomas Bohlen. "The role of attenuation in 2D full-waveform inversion of shallow-seismic body and Rayleigh waves." GEOPHYSICS 79, no. 6 (2014): R247—R261. http://dx.doi.org/10.1190/geo2013-0462.1.

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Full-waveform inversion (FWI) of Rayleigh waves is attractive for shallow geotechnical investigations due to the high sensitivity of Rayleigh waves to the S-wave velocity structure of the subsurface. In shallow-seismic field data, the effects of anelastic damping are significant. Dissipation results in a low-pass effect as well as frequency-dependent decay with offset. We found this by comparing recorded waveforms with elastic and viscoelastic wave simulation. The effects of anelastic damping must be considered in FWI of shallow-seismic Rayleigh waves. FWI using elastic simulation of wave prop

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50

Zhou, Yunying, Dongying Liu, Dinggui Hou, Jiahuan Liu, Xiaoliang Li, and Zhijie Yue. "Wave Propagation in the Viscoelastic Functionally Graded Cylindrical Shell Based on the First-Order Shear Deformation Theory." Materials 16, no. 17 (2023): 5914. http://dx.doi.org/10.3390/ma16175914.

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Based on the first-order shear deformation theory (FSDT) and Kelvin–Voigt viscoelastic model, one derives a wave equation of longitudinal guide waves in viscoelastic orthotropic cylindrical shells, which analytically solves the wave equation and explains the intrinsic meaning of the wave propagation. In the numerical examples, the velocity curves of the first few modes for the elastic cylindrical shell are first calculated, and the results of the available literature are compared to verify the derivation and programming. Furthermore, the phase velocity curves and attenuation coefficient curves

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