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Surface wave propagation for linear viscoelastic solids
Affiliation:1. Division of Engineering and Applied Science, California Institute of Technology, Pasadena, CA 91125, United States;2. Department of Civil Engineering and Computer Science, University of Rome “Tor Vergata”, Via del Politecnico 1, 00133 Rome, Italy;3. Université Pierre et Marie Curie, Institut D’Alembert, UMR 7190 CNRS, 4 Place Jussieu, 75252 Paris Cedex 05, France;1. Mechanical Engineering Department, College of Engineering and Islamic Architecture, Umm Al-Qura University, Makkah, Saudi Arabia;2. Mathematics Department, Faculty of Education, Alexandria University, Alexandria, Egypt;3. Basic and Applied Science Institute, Arab Academy for Science, Technology and Maritime Transport, P.O. Box 1029, Alexandria, Egypt;1. Département des Génies Civil, Géologique et des Mines, École Polytechnique de Montréal, Montréal, Québec H3C 3A7, Canada;2. Geological Survey of Canada-Atlantic, Bedford Institute of Oceanography, P.O. Box 1006, Dartmouth, Nova Scotia B2Y 4A2, Canada;3. Department of Earth Sciences, Sun Yat-Sen University, Guangzhou 510275, China;4. Institute of Energy Sciences, School of Earth Sciences and Engineering, Nanjing University, Nanjing 210093, China
Abstract:Experiments have been carried out to observe the surface waves produced on large blocks of polyethylene and polymethylmethacrylate (p.m.m.) when specimens of these materials have been subjected to surface impacts of steel balls or when small lead azide charges have been detonated on the free surfaces. It has been shown that if Poisson's ratio, v, is taken to be a real constant the shapes of surface waves can be calculated if the shape of the initial disturbance and the visco-elastic properties of the medium are known. It has further been shown that the complex nature of v results in only second-order effects for the materials used. It has consequently been found possible to forecast the shape of surface waves produced by the impact of steel balls. The agreement with experimentally observed shapes was found to be excellent for the p.m.m. specimen. The theoretical predictions were less accurate for the polyethylene specimen, but the predictions here agreed reasonably well with the experiments. It was not found possible to predict the surface waves produced by the explosive charges chiefly because of uncertainty of the shape of the initial disturbance. The experimental results did, however, show two distinct groups of waves, one travelling with the dilatational velocity and the other with a velocity close to that of the shear velocity. At short distances of travel these two groups overlapped.
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