Generalized Multi-Symplectic Numerical Implementation of Dynamic Responses for Saturated Poroelastic Timoshenko Beam

被引:0
作者
Liu X. [1 ,2 ]
Deng Z. [1 ]
机构
[1] School of Mechanics and Civil Engineering, Northwestern Polytechnical University, Xi'an
[2] School of Sciences Mechanics, Chang'an University, Xi'an
来源
Xibei Gongye Daxue Xuebao/Journal of Northwestern Polytechnical University | 2020年 / 38卷 / 04期
关键词
Attenuation vibration; Cantilever beam; Darcy permeability coefficient; Dissipation; Dynamic response; Effective stress; Generalized multi-symplectic method; Local conserved structure; Multi-symplectic method; Numerical implementation; Porosity; Saturated poroelastic Timoshenko beam; Saturated porous media; Solid skeleton;
D O I
10.1051/jnwpu/20203840774
中图分类号
学科分类号
摘要
Based on the porous media theory and Timoshenko beam theory, properties of dynamic responses in fluid-solid coupled incompressible saturated poroelastic Timoshenko beam are investigated by generalized multi-symplectic method. Dynamic response equation set of incompressible saturated poroelastic Timoshenko beam is presented at first. Then a first order generalized multi-symplectic form of this dynamic response equation set is constructed, and errors of generalized multi-symplectic conservation law, generalized multi-symplectic local momentum and generalized multi-symplectic local energy are also derived. A Preissmann Box generalized multi-symplectic scheme of the dynamic response equation set is presented, the discrete errors of generalized multi-symplectic conservation law, generalized multi-symplectic local momentum conservation law and generalized multi-symplectic local energy conservation law are also obtained. In view of the dynamic responses of incompressible saturated poroelastic Timoshenko cantilever beam with two ends permeable and free end subjected to the step load, the transverse dynamic response process of the solid skeleton is simulated numerically, the evolution processes of solid effective stress and the equivalent moment of the pore fluid pressure over time are also presented numerically. The effects of fluid-solid coupled interaction parameter and slenderness ratio of the beam on the solid dynamic response process are revealed, as well as the effects on all generalized multi-symplectic numerical errors are checked simultaneously. From results obtained, the processes for solid deflection, solid effective stress and the equivalent moment of the pore fluid pressure approaching to their steady response values are all shortened with increasing of fluid-solid coupled interaction parameter, while the response process of solid deflection and the pore fluid equivalent moment are lengthened with increasing of slenderness ratio of the beam. Moreover, the steady value of solid deflection is much closer to the static deflection value of classic single phase elastic Euler-Bernoulli beam with increasing of the slenderness ratio. As time goes on, the solid skeleton of the beam will support all outside load, so equivalent moment of the pore fluid pressure becomes zero at last. In addition, it is presented all generalized multi-symplectic numerical errors decrease with the decreasing of parameters representing the dissipation effect for the dynamic system. © 2020 Journal of Northwestern Polytechnical University.
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页码:774 / 783
页数:9
相关论文
共 19 条
  • [1] LI L P, CEDERBAUM G, SCHULGASSER K., A Finite Element Model for Poroelastic Beams with Axial Diffusion, Com puters & Structures, 73, 6, pp. 595-608, (1999)
  • [2] YANG Xiao, LI Li, Mathematical Model for Dynamics of Incompressible Saturated Poroelastic Beam and Rod, Acta Mechan ica Solida Sinica, 27, 2, pp. 159-166, (2006)
  • [3] WANG Z H, PREVOST J H, OLIVIER C., Bending of Fluid-Saturated Linear Poroelastic Beams with Compressible Constituents, International Journal for Numerical and Analytical Methods in Geomechanics, 33, 4, pp. 425-447, (2009)
  • [4] ZHOU Fengxi, MI Haizhen, Free Vibration of Poroelastic Beam with Incompressible Saturated Liquid on Elastic Foundation, Journal of Lanzhou University of Technology, 40, 2, pp. 118-122, (2014)
  • [5] LOU P, DAI G L, ZENG Q Y., Finite-Element Analysis for a Timoshenko Beam Subjected to a Moving Mass, Journal of Mechanical Engineering Science, 220, 5, pp. 669-678, (2006)
  • [6] YANG X, WEN Q., Dynamic and Quasi-Static Bending of Saturated Poroelastic Timoshenko Cantilever Beam, Applied Mathematics and Mechanics, 31, 8, pp. 995-1008, (2010)
  • [7] WU Feng, XU Xiaoming, GAO Qiang, Et al., Analyzing the Wave Scattering in Timoshenko Beam Based on the Symplectic Theory, Applied Mathematics and Mechanics, 34, 12, pp. 1225-1352, (2013)
  • [8] KIANI K, AVILI H G, KOJORIAN A N., On the Role of Shear Deformation in Dynamic Behavior of a Fully Saturated Poroelastic Beam Traversed by a Moving Load, International Journal of Mechanical Sciences, 94, 1, pp. 84-95, (2015)
  • [9] CHOUIYAKH H, AZRAR L, ALNEFAIE K, Et al., Vibration and Multi-Crack Identification of Timoshenko Beams under Moving Mass Using the Differential Quadrature Method, International Journal of Mechanical Sciences, 120, 1, pp. 1-11, (2017)
  • [10] GAO Qiang, ZHANG Hongwu, ZHANG Liang, Et al., Dynamic Parametric Variational Principle and Symplectic Algorithm for Trusses with Different Tensional and Compressional Stiffnesses, Journal of Vibration and Shock, 32, 4, pp. 179-184, (2013)