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Finite element analysis of elastic solid/Stokes flow interaction problem 원문보기

Korea-Australia rheology journal, v.19 no.4, 2007년, pp.233 - 242  

Myung, Jin-Suk (School of Chemical and Biological Engineering, Seoul National University) ,  Hwang, Wook-Ryol (School of Mechanical and Aerospace Engineering, Research Center for Aircraft Parts Technology (ReCAPT), Gyeongsang National University) ,  Won, Ho-Youn (Hanwha Chemical, Research and Development Center) ,  Ahn, Kyung-Hyun (School of Chemical and Biological Engineering, Seoul National University) ,  Lee, Seung-Jong (School of Chemical and Biological Engineering, Seoul National University)

Abstract AI-Helper 아이콘AI-Helper

We performed a numerical investigation to find out the optimal choice of the spatial discretization in the distributed-Lagrangian-multiplier/fictitious-domain (DLM/FD) method for the solid/fluid interaction problem. The elastic solid bar attached on the bottom in a pressure-driven channel flow of a ...

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제안 방법

  • solid/Stokes flow interaction problem. The purpose of this numerical work is to find 이it the proper condition in using the DLM/FD scheme to the solid/fluid interaction problem. The robustness of this simulation algorithm has been verified through the mesh convergence and pseudo­ time step dependence test.
  • Also, to assess the necessity of considering fluid stress in the solid domain, we denote a problem with sub-matrices I and P by SV and a problem without I and P by V The four sets, two different con­ditions for each factor, have been listed in Table 1. To understand the effect of each factor and to find the opti­ mum condition, we performed numerical experiments for the four sets and checked the mesh convergence and the pseudo-time step dependence to evaluate the robustness of the present formulation. The results are presented from all four sets together for the proper comparison.

이론/모형

  • Using the ficti­tious domain method, one can avoid remeshing and solve the problem with a simple regular mesh, which is espe­cially beneficial in 3D simulation. In this study, the fic­titious domain method will be used with which constraints on the solid boundary (or over the solid domain) are rep­resented by the distributed Lagrangian multipliers (Glow­ inski et aL.,1999). The overview of the distributed- Lagrangian-multiplier/fictitious-domain(DLM/FD) method is well documented in Glowinski et al.
  • In this study, we apply the distributed-Lagrangian-mul-tiplier/fictitious-domain (DLMZFD) method to a simple elastic solid/Stokes flow interaction problem. We investi­ gate the effect of the distribution of the Lagrangian mul­tipliers and the effect of interfacial conditions between the fluid and solid meshes.
  • The purpose of this numerical work is to find 이it the proper condition in using the DLM/FD scheme to the solid/fluid interaction problem. The robustness of this simulation algorithm has been verified through the mesh convergence and pseudo­ time step dependence test. All four sets showed good mesh convergence, and there was no pseudo-time step depen­ dence.
  • In the solid domain a regular rectangular discretization is also used but with the bi-linear interpolation of the displace­ ment and the constant pressure element (Qi~PQ element). To impose no-slip constraint on the solid boundary, we applied the distributed Lagrangian multiplier method. For the computational convenience, multipliers are imposed on every nodal point on the solid boundary (or on the solid domain).
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참고문헌 (14)

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  2. Amestoy, P. R. and I. S. Duff, 1989, Vectorization of a Mu1tiprocessor Multifrontal Code, Intern. J Supercomput. Applicat. 3(3), 41-59 

  3. Amestoy, P. R. and I. S. Duff, 1993, Memory Management Issues in Sparse Multifrontal Methods on Multiprocessors, Intern. J Supercomput. Applicat. 7(1), 64-82 

  4. Amestoy, P. R. and C. Puglisi, 2003, An unsymmetrized multifrontal LU factorization, SIAM J Matrix Anal. Applicat. 24(2), 553-569 

  5. Baaijens, F. P. T., 2001, A fictitious domain/mortar element method for fluid-structure interaction, Int. J Numer. Methods Fluids 35(7), 743-761 

  6. Donea, J., S. Giuliani and J. P. Halleux, 1981, Arbitrary Lagrangian-Eulerian fmite element method for transient dynamic fluid-structure interactions, Comput. Methods Appl. Mech. Eng. 33(1-3), 689-723 

  7. Glowinski, R., T. W. Pan, T. I. Hesla and D. D. Joseph, 1999, A distributed Lagrange multiplier fictitious domain method for particulate flows, Int. J Multiph. Flow 25(5), 755-794 

  8. Hu, H. H., 1996, Direct simulation of flows of solid-liquid mixtures, Int. J. Multiph. Flow 22(2), 335-352 

  9. Hughes, T. J. R., 2000, The Finite Element Method: linear static and dynamic finite element analysis, Dover publications, New York, US 

  10. Hiitter, M., 1999, Brownian Dynamics Simulation of Stable and of Coagulating Colloids in Aqueous Suspension, PhD Thesis, ETH, ZURICH 

  11. Hwang, W. R., M. A. Hulsen and H. E. H. Meijer, 2004, Direct simulation of particle suspensions in sliding bi-periodic frames, J. Comput. Phys. 194(2), 742-772 

  12. Laso, M. and H. C. Ottinger, 1993, Calculation of Viscoelastic Flow Using Molecular-Models - the Connffessit Approach, J. Non-Newtonian Fluid Mech. 47, 1-20 

  13. Trofimov, S. Y., 2003, Thermodynamic consistency in dissipative particle dynamics, PhD Thesis, Technische Universiteit Eindhoven, Eindhoven 

  14. Yu, Z., 2005, A DLM/FD method for fluid/flexible-body interactions, J. Com put. Phys. 207(1), 1-27 

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