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Convection of internal variable methodology in Computational Fluid Dynamics solutions for thixoforming modelling

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Warianty tytułu
PL
Metoda konwekcji zmiennej wewnętrznej w rozwiązaniu z zakresu komputerowej mechaniki płynów (CFD) dla tiksoformingu
Konferencja
14th KomPlasTech Conference, Zakopane, January 14-17, 2007
Języki publikacji
EN
Abstrakty
EN
During thixoforming, the deformed material is in semi-solid state. From numerical point of view, such materials are difficult to simulate because of gathering some features of solid materials and some of fluids. Materials properties are history dependent like in solids, while deformations could be extremely high, like in fluids. The typical solutions of structural analysis, based on Lagrangian motion description are difficult because of remeshing, which is needed in short time intervals. Frequent remeshing operations increase time consumptions and decrease the accuracy of solution. On the other hand, typical Computational Fluid Dynamics (CFD) solutions, usually based on Eulerian motion description, are ineffective when domain borders are changing. Because of material points are detached from mesh nodes, the history dependent parameters of the material are also very difficult to introduce. On the contrary, in the third possible formulation, Arbitrary Lagrangian Eulerian (ALE), the material points are not bound with mesh nodes and domain geometry could change. In ALE formulation each time step is divided into Lagrangian and Eulerian steps, what assures that history of material could be included and the calculation domain is reproduced properly by the mesh. Therefore, ALE formulation seems to be the best solution in the most thixoforming cases. The disadvantages of this method are the time consumptions and some inaccuracy of approximation needed between both steps. In the cases when the domain of solution is unchangeable, Eulerian formulation could be more promising than ALE. The Eulerian solution is easier to implement, as well as computational round-offs are less significant. The difficulties connected with history dependent parameters could be solved with “internal variable convection”. After classical time step, when new velocities in nodes are computed, the convection step is carried out. While velocity field is known, the convection of internal variable values could be calculated. The changes of internal variable due to material processes could be included as a source stream. The internal variable convection methodology allows to adapt typical CFD codes for thixoforming simulations, with complying viscosity changes in time. This approach also makes very high deformations relatively easy to compute. In this paper, the assumption and proposition of implementation of internal variable convection into thixoforming modelling is presented.
PL
Tiksoforming jest stosunkowo nową metodą formowania. Polega ona na nadawaniu znacznego stopnia odkształcenia materiałowi w stanie stało-ciekłym. Z numerycznego punktu widzenia, procesy te są trudne do modelowania, co jest efektem występowania zjawisk charakterystycznych zarówno dla cieczy, jak i ciał stałych. Własności materiału są zależne od czasu, podobnie jak w materiałach stałych, podczas gdy odkształcenie może być bardzo duże, podobnie jak w cieczach. W artykule zaprezentowano przegląd obecnie istniejących rozwiązań numerycznych, opartych głównie na metodach dynamiki płynów, z zastosowaniem opisu kinetyki wg metody Eulera lub Arbitrary Lagrangian Eulerian (ALE). Wykazana została potrzeba opracowania nowej metody symulacyjnej dla zależnych od czasu materiałów poddawanych formowaniu tiksotropowemu. Opisana została metoda konwekcji zmiennej wewnętrznej dla eulerowskiego opisu kinetyki. Przedstawiona została implementacja metody jako procedur użytkownika komercyjnego pakietu ADINA-F. Zaprezentowano przykładowe wyniki dla prostych przepływów tiksotropowych.
Wydawca
Rocznik
Strony
112--118
Opis fizyczny
Bibliogr. 23 poz., rys.
Twórcy
autor
  • Interdisciplinary Centre for Materials Modelling, AGH University of Science and Technology, Faculty of Metals Engineering and Industrial Computer Science, al. Mickiewicza 30, 30-059 Kraków, pmaciol@metal.agh.edu.pl
Bibliografia
  • Baravian, C., Quemada, D., Parker A., 1996, Modelling thixotropy using a novel Structural kinetics approach: basis and application to a solution of iota carrageenan, J. Texture Stud. 27, 371-390.
  • Barnes, H., 1997, Thixotropy - a review, J. non-Newton. Fluid Mech., 70, 1-33.
  • Bellet, M., Moto Mpong, S., 2001, Determination of the consti-tutive equation parameters of a thixotropic Al alloy and FEM modelling of the thixoforming process, in: Proc. NUMIFORM 2001, ed. Mori, Lisse, 1087-1092.
  • Donea, J., Huerta, A., 2003, Finite Element Methods for Flow Problems, John Wiley & Sons Ltd., Chichester.
  • Goodeve, C. F., 1939, A general theory of thixotropy and vis-cosity, Trans. Faraday Soc., 35, 342-358.
  • Huilgol, R.R., You, Z., 2005, Application of the augmented Lagrangian method to steady pipe flows of Bingham, Casson and Herschel-Bulkley fluids. J. non-Newton. Fluid Mech., 128(2-3), 126-143.
  • Joly, P. A., Mehrabian, R., 1976, The rheology of partially solid alloy. J. Mater. Sci., 11, 1393-1418.
  • Kapranos, P., Liu, T.Y., Atkinson, H.V., Kirkwood, D.H., 2001, Investigation into the rapid compression of semi-solid alloy slugs, J. Mat. Proc. Technol., 111,31-36.
  • Kim, N. S., Kang, C.G., 2000. An investigation of flow characteristics considering the effect of viscosity variation in the thixoforming process. J. Mat. Proc. Technol., 103, 237-246.
  • Koke, J., Modigell, M., 2003, Flow behaviour of semi-solid metal alloys. J. non-Newton. Fluid Mech., 112, 141-160.
  • Kopp, R., Choi, J., Neudenberger, D., 2003. Simple comprssion test and simulation of an Snl5% Pb alloy in the semi-solid state, J. Mat. Proc. Technol., 135, 317-323.
  • Kumar, P., Martin, C. L., Brown, S., 1994, Constitutive modelling and characterization of the flow behaviour of semi-solid metal alloy slurries - I. The flow response, Acta Metall. Mater., 42, 3595-3602.
  • Martin, C. L., Kumar, P., Brown, S., 1994, Constitutive modelling and characterization of the flow behaviour of semi-solid metal alloy slurries - II. Structural evolution under shear deformation, Acta Metall. Mater., 42, 3603-3614.
  • Messmer, G., Simulation of a Thixoforging Process of Aluminium Alloys  with Flow-3D. Internet, http://www. thixoschmieden.de/miscA/Veroeffentlichungpdf/Mrglish. pdf.
  • Modigell, M., Kokę, J., 1999, Time-Dependent Rheological Properties of Semi-Solid Metal Alloys, Mechanics of Time-Dependent Materials, 3, 15-30.
  • Modigell, M, Koke, J., 2001, Rheological modelling on semi-solid metal alloys and simulation of thixocasting processes. J. Mat. Proc. Technol., 111, 53-58.
  • Moore, F., 1959, The rheology of ceramic sleeps and bodies, Trans. Br. Ceramic Soc., 58, 470-494.
  • Mujumdar, A., Beris, A. N., Metzner, A. B., 2002, Transient phenomena in thixotropic systems, J. non-Newton. Fluid Mech., 102, 157-178.
  • Roussel, N., Le Roy, R., Coussot, P., 2004, Thixotropy modelling at local and macroscopic scales, J. non-Newton. Fluid Mech., 117,85-95.
  • Slibar, A., Paslay, P. R., 1964, On the technical description of the flow of thixotropic materials, Proceeding of International Symposium on Second Order Effects in Elasticity, Plasticity and Fluid Dynamics, 1,314-330.
  • Sołek, K., Stuczyński, T., Białobrzeski, A., Kuziak, R., Mitura, Z., 2005, Modelling thixocasting with precise accounting of moving front of materiał, Mater. Sci. Technol., 21, 551-558.
  • Zienkiewicz, O. C., Cormeau, I. C. 1974., Visco-plasticity -plasticity and creep in elastic solids - a unifed numerical solution approach, Int. J. Numer. Methods Eng, 8, 821-845.
  • Zienkiewicz, O. C., Taylor, R., L., 2000, The Finite Element Method, Butterworth-Heinemann, Oxford.
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-article-BUJ5-0013-0055
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