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On the behaviour of infinitely long rigid-plastic beams under transverse concentrated load
Affiliation:1. Laboratorio de Anatomía Comparada y Evolución de los Vertebrados, Museo Argentino de Ciencias Naturales “Bernardino Rivadavia”, Av. Ángel Gallardo 470, C1405DJR Buenos Aires, Argentina;2. CONICET, Consejo Nacional de Investigaciones Científicas y Técnicas, Argentina;1. Experimental Geophysics Group, Institute for Geology, Mineralogy, and Geophysics, Ruhr-Universität Bochum, D44780 Bochum, Germany;2. School of Civil Engineering, Sun Yat-sen University, Guangzhou 510275, China;3. Key Laboratory of Deep Coal Resource Ming (China University of Mining and Technology), Ministry of Education, China;4. School of Mining Engineering, Key Laboratory of Deep Coal Resource Mining (Ministry of Education), China University of Mining and Technology, Xuzhou, Jiangsu 221116, China;1. Department of Civil, Architectural and Environmental Engineering, The University of Texas at Austin, USA;2. Department of Petroleum and Geosystems Engineering, The University of Texas at Austin, USA
Abstract:This paper is concerned with the behaviour of an infinitely long uniform beam, made of a non-hardening plastic-rigid material, under the action of a single transverse concentrated load. The effects of transverse shearing deformation and rotatory inertia are assumed negligible, and the yield condition is assumed to depend only upon the bending moment. This problem is solved subject to the condition that the ratio of the impact velocity of the concentrated load to the time is non-increasing in time. The impact velocity is allowed to vary with the time. The associated problem concerning the motion of the beam following the removal of the concentrated load is also solved. Hitherto the only problem of the present type whose solution has been published is that involving constant impact velocity, but even there the solution of the unloading problem was not found. The general analysis of this paper is applied to solve completely the constant impact velocity problem, and some detailed results for other cases are also given. The motion, subject to the above restriction upon the impact velocity, is such that there are always a central, fixed yield-hinge and two lateral, outwards-moving yield-hinges, and is also such that the beam does not come to rest in any finite time.
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