Article : A large eddy based lattice-Boltzmann simulation of velocity distribution in an open channel flow with rigid and flexible vegetation
Authors : Saenger, E.ETH Zurich Geological Institute, Zurich, Switzerland, email@example.com, Madonna, C.ETH Zurich Geological Institute, Zurich, Switzerland, Almqvist, B.ETH Zurich Geological Institute, Zurich, Switzerland, Montahaei, M.Institute of Geophysics, University of Tehran, Tehran, Iran, firstname.lastname@example.org, Oskooi, B.Institute of Geophysics, University of Tehran, Tehran, Iran, email@example.com, Pal, P.Department of Applied Mathematics, Indian School of Mines, Dhanbad, India, firstname.lastname@example.org, Mandal, D.Department of Applied Mathematics, Indian School of Mines, Dhanbad, India, email@example.com, Tsapanos, T.Aristotle University of Thessaloniki, School of Geology, Geophysical Laboratory, Thessaloniki, Greece, firstname.lastname@example.org, Bayrak, Y.Karadeniz Technical University, Department of Geophysics, Trabzon, Turkey, email@example.com, Cinar, H.Karadeniz Technical University, Department of Geophysics, Trabzon, Turkey, firstname.lastname@example.org, Koravos, G.Aristotle University of Thessaloniki, School of Geology, Geophysical Laboratory, Thessaloniki, Greece, email@example.com, Bayrak, E.Karadeniz Technical University, Department of Geophysics, Trabzon, Turkey, firstname.lastname@example.org, Marzec, P.AGH University of Science and Technology, Faculty of Geology, Geophysics, and Environment Protection, Kraków, Poland, email@example.com, Niepsuj, M.AGH University of Science and Technology, Faculty of Geology, Geophysics, and Environment Protection, Kraków, Poland, firstname.lastname@example.org, Bała, M.AGH University of Science and Technology, Faculty of Geology, Geophysics, and Environment Protection, Kraków, Poland, email@example.com, Pietsch, K.AGH University of Science and Technology, Faculty of Geology, Geophysics, and Environment Protection, Kraków, Poland, firstname.lastname@example.org, Xiao, L.Key Laboratory of Geo-detection (China University of Geosciences), Ministry of Education, Beijing, China, email@example.com, Liu, X.-P.Geological Exploration and Development Research Institute Sichuan-Changqing Drilling and Exploration Engineering Co., Chengdu, China, Zou, C.-C.Key Laboratory of Geo-detection (China University of Geosciences), Ministry of Education, Beijing, China, Hu, X.-X.Geological Exploration and Development Research Institute Sichuan-Changqing Drilling and Exploration Engineering Co., Chengdu, China, Mao, Z. Q.State Key Laboratory of Petroleum Resources and Prospecting, China University of Petroleum, Beijing, China, Shi, Y.-J.Research Institute of Exploration and Development, Changqing Oilfield, PetroChina, Xi’an, China, Guo, H.-P.Research Institute of Exploration and Development, Changqing Oilfield, PetroChina, Xi’an, China, Li, G.-R.Research Institute of Exploration and Development, Changqing Oilfield, PetroChina, Xi’an, China, Alam, K.Geophysics Division, Geological Survey of Pakistan, Lahore, Pakistan, firstname.lastname@example.org, Ahmad, N.Institute of Geology, University of the Punjab, Lahore, Pakistan, email@example.com, Shaban, A.Conseil National des Recherches Scientifiques, Beirut, Lebanon, Telesca, L.Consiglio Nazionale delle Ricerche, Istituto di Metodologie per l’Analisi Ambientale Tito, Italy, firstname.lastname@example.org, Darwich, T.Conseil National des Recherches Scientifiques, Beirut, Lebanon, Amacha, N.Litani River Authority, Beirut, Lebanon, Gac, J.Faculty of Chemical and Process Engineering, Warsaw University of Technology, Warszawa Poland, J.Gac@ichip.pw.edu.pl,
Abstract : The large eddy simulation method, based on a lattice-Boltzmann algorithm, was used to compute the vertical velocity profile in an open channel flow with submerged and emerged vegetation. The numerical method is characterized by the relatively short time of computation and low complexity. On the other hand, it allows a more realistic description of the vegetation properties relative to the methods commonly used in 1-D numerical models. For the proper conditions, the method developed in this work gives results similar to other numerical methods. These results are also in good agreement with the experimental data presented in other papers.
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Qute : Saenger, E. ,Madonna, C. ,Almqvist, B. ,Montahaei, M. ,Oskooi, B. ,Pal, P. ,Mandal, D. ,Tsapanos, T. ,Bayrak, Y. ,Cinar, H. ,Koravos, G. ,Bayrak, E. ,Marzec, P. ,Niepsuj, M. ,Bała, M. ,Pietsch, K. ,Xiao, L. ,Liu, X.-P. ,Zou, C.-C. ,Hu, X.-X. ,Mao, Z. Q. ,Shi, Y.-J. ,Guo, H.-P. ,Li, G.-R. ,Alam, K. ,Ahmad, N. ,Shaban, A. ,Telesca, L. ,Darwich, T. ,Amacha, N. ,Gac, J. ,Gac, J. , A large eddy based lattice-Boltzmann simulation of velocity distribution in an open channel flow with rigid and flexible vegetation. Acta Geophysica Vol. 62, no. 1/2014