{"id":3881,"date":"2019-04-26T16:37:02","date_gmt":"2019-04-26T14:37:02","guid":{"rendered":"http:\/\/www.mi.uni-koeln.de\/NumSim\/?page_id=3881"},"modified":"2019-11-07T14:00:01","modified_gmt":"2019-11-07T13:00:01","slug":"visitors","status":"publish","type":"page","link":"https:\/\/www.mi.uni-koeln.de\/NumSim\/research\/visitors\/","title":{"rendered":"Visitors"},"content":{"rendered":"\n<table id=\"tablepress-21\" class=\"tablepress tablepress-id-21\">\n<tbody class=\"row-hover\">\n<tr class=\"row-1 odd\">\n\t<td class=\"column-1\"><strong>Visitors<\/strong><\/td><td class=\"column-2\"><\/td>\n<\/tr>\n<tr class=\"row-2 even\">\n\t<td class=\"column-1\">Lea Miko Versbach<\/td><td class=\"column-2\">Lund University\/Sweden<br \/>\n(February 3 - February 7, 2020)<\/td>\n<\/tr>\n<tr class=\"row-3 odd\">\n\t<td class=\"column-1\">Bernhard M\u00fcller<\/td><td class=\"column-2\">Norwegian University of Science and Technologie (NTNU), Trontheim\/Norway<br \/>\n\"Immersed Boundary Method for the Compressible Navier-Stokes Equations Using High Order Summation-By-Parts Operators)\"<br \/>\n(February 4, 2020)<\/td>\n<\/tr>\n<tr class=\"row-4 even\">\n\t<td class=\"column-1\">R\u00fcdiger Pakmor<\/td><td class=\"column-2\">Max-Planck-Institute for Astrophysics, Garching\/Germany<br \/>\n\"The numerical schemes behind the moving mesh code Arepo\"<br \/>\n(January 31, 2020)<\/td>\n<\/tr>\n<tr class=\"row-5 odd\">\n\t<td class=\"column-1\">Almut Gassmann<\/td><td class=\"column-2\">Leibnitz-Institute of Atmospheric Physics, University Rostock, K\u00fchlungsborn\/Germany<br \/>\n\"Entropy production in numerical modeling of a moist atmosphere\"<br \/>\n(December 12 - December 13, 2019)<\/td>\n<\/tr>\n<tr class=\"row-6 even\">\n\t<td class=\"column-1\">Florian Hindenlang<\/td><td class=\"column-2\">Max-Planck-Institute for Plasma Physics, Garching\/Germany<br \/>\n(November 19 - November 20, 2019)<\/td>\n<\/tr>\n<tr class=\"row-7 odd\">\n\t<td class=\"column-1\">Andr\u00e9s Rueda-Ram\u00edrez<\/td><td class=\"column-2\">University of Madrid, School of Aeronautics\/Spain<br \/>\n(November 13 - November 17, 2019)<\/td>\n<\/tr>\n<tr class=\"row-8 even\">\n\t<td class=\"column-1\">Victor Linders<\/td><td class=\"column-2\">Israel Institute of Technology, Haifa\/Israel<br \/>\n(September 15 - September 27, 2019)<\/td>\n<\/tr>\n<tr class=\"row-9 odd\">\n\t<td class=\"column-1\">Juan Manzanero<\/td><td class=\"column-2\">University of Madrid\/Spain<br \/>\n\"The industrial solver for multiphase with split-form DG\"<br \/>\n(August 18 - August 21, 2019)<\/td>\n<\/tr>\n<tr class=\"row-10 even\">\n\t<td class=\"column-1\">Yinhua  Xia<\/td><td class=\"column-2\">Universit\u00e4t of Science and Technology, Hefei\/People's Republic of China<br \/>\n\"Positivity Preserving Limiters for Time-Implicit Higher Order Accurate Discontinuous Galerkin Discretizations\u201c<br \/>\n(August 12 - August 31, 2019)<\/td>\n<\/tr>\n<tr class=\"row-11 odd\">\n\t<td class=\"column-1\">Yan Xu<\/td><td class=\"column-2\">Universit\u00e4t of Science and Technology, Hefei\/People's Republic of China<br \/>\n\"Globally divergence-free discontinuous Galerkin methods for ideal magneto- hydrodynamics equations\u201c<br \/>\n(August 12 - August 31, 2019)<\/td>\n<\/tr>\n<tr class=\"row-12 even\">\n\t<td class=\"column-1\">Nico Krais<\/td><td class=\"column-2\">Institute of Aerodynamics and Gasdynamics, University of Stuttgart\/Germany<br \/>\n\"Application and Development of the High Order Discontinuous Galerkin Spectral Element Method for Compressible Multiscale Flows\u201c<br \/>\n(Juli 8 - July 12, 2019)<\/td>\n<\/tr>\n<tr class=\"row-13 odd\">\n\t<td class=\"column-1\">R\u00e9mi Abgrall<\/td><td class=\"column-2\">University of Zurich\/Switzerland<br \/>\n\"High order method for systems of conservation laws using continuous approximation of data\"<br \/>\n(June 18 - June 21, 2019)<\/td>\n<\/tr>\n<tr class=\"row-14 even\">\n\t<td class=\"column-1\">Magnus Sv\u00e4rd<\/td><td class=\"column-2\">University of Bergen\/Norway<br \/>\n\"On the physicality of the compressible Navier-Stokes Equations\"<br \/>\n(April 28 - May 10, 2019)<\/td>\n<\/tr>\n<tr class=\"row-15 odd\">\n\t<td class=\"column-1\">Raphael Loub\u00e8re<\/td><td class=\"column-2\">University of Bordeaux\/France<br \/>\n(March 17 - March 22, 2019)<\/td>\n<\/tr>\n<tr class=\"row-16 even\">\n\t<td class=\"column-1\">Francois Vilar<\/td><td class=\"column-2\">University of Montpellier\/France<br \/>\n(March 17 - March 22, 2019)<\/td>\n<\/tr>\n<tr class=\"row-17 odd\">\n\t<td class=\"column-1\">Christian Klingenberg<\/td><td class=\"column-2\">University of W\u00fcrzburg\/Germany<br \/>\n\"The compressible Euler equations with gravity: well-balanced schemes and all Mach numer solvers\"<br \/>\n(February 14, 2019)<\/td>\n<\/tr>\n<tr class=\"row-18 even\">\n\t<td class=\"column-1\">Harald Klimach<\/td><td class=\"column-2\">University of Siegen\/Germany<br \/>\n\"Fortran Development Environment for APES?\"<br \/>\n(February 8, 2019)<\/td>\n<\/tr>\n<tr class=\"row-19 odd\">\n\t<td class=\"column-1\">Raul Borsche<\/td><td class=\"column-2\">Technical University of Kaiserslautern\/Germany<br \/>\n\"Kinetic layers and coupling conditions for hyperbolic PDEs on networks\"<br \/>\n(January 25, 2019)<\/td>\n<\/tr>\n<tr class=\"row-20 even\">\n\t<td class=\"column-1\">Claus-Dieter Munz<\/td><td class=\"column-2\">Institute of Aerodynamics and Gasdynamics, University of Stuttgart\/Germany<br \/>\n(January 14, 2019)<\/td>\n<\/tr>\n<tr class=\"row-21 odd\">\n\t<td class=\"column-1\">Maria Veiga<\/td><td class=\"column-2\">University of Zurich\/Switzerland<br \/>\n\"Structure preserving schemes for astophysical flows\"<br \/>\n(December 7, 2018)<\/td>\n<\/tr>\n<tr class=\"row-22 even\">\n\t<td class=\"column-1\">Neeraj Sarna<\/td><td class=\"column-2\">RWTH Aachen\/Germany<br \/>\n\"Entropy stable schemes for linear and linearised kinetic equations\"<br \/>\n(November 16, 2018)<\/td>\n<\/tr>\n<tr class=\"row-23 odd\">\n\t<td class=\"column-1\">Florian Kummer<\/td><td class=\"column-2\">University of Darmstadt\/Germany<br \/>\n\"On the Simulation fo Contact Line Dynamics using Sharp-Interface Methods\"<br \/>\n(November 15, 2018)<\/td>\n<\/tr>\n<tr class=\"row-24 even\">\n\t<td class=\"column-1\">Michael Schlottke-Lakemper<\/td><td class=\"column-2\">RWTH Aachen\/Germany<br \/>\n\"Scalable parallel multiphysics simulations on hierarchical Cartesian grids\"<br \/>\n(November 9, 2018)<\/td>\n<\/tr>\n<tr class=\"row-25 odd\">\n\t<td class=\"column-1\">Mark H. Carpenter<\/td><td class=\"column-2\">NASA Langley Research Center, Hampton, Virginia\/USA<br \/>\n(June 16 - July 7, 2018)<\/td>\n<\/tr>\n<tr class=\"row-26 even\">\n\t<td class=\"column-1\">David C. Del Rey Fern\u00e1ndez<\/td><td class=\"column-2\">NASA Langley Research Center, Hampton, Virginia\/USA<br \/>\n(June 16 - July 7, 2018)<\/td>\n<\/tr>\n<tr class=\"row-27 odd\">\n\t<td class=\"column-1\">David A. Kopriva<\/td><td class=\"column-2\">Department of Mathematics, The Florida State University\/USA<br \/>\n(May 13 - May 18, 2018)<\/td>\n<\/tr>\n<tr class=\"row-28 even\">\n\t<td class=\"column-1\">David A. Kopriva<\/td><td class=\"column-2\">Department of Mathematics, The Florida State University\/USA<br \/>\n(September 19 - Oktober 1, 2017)<\/td>\n<\/tr>\n<tr class=\"row-29 odd\">\n\t<td class=\"column-1\">Florian Hindenlang<\/td><td class=\"column-2\">Max-Planck-Institute for Plasma Physics, Garching\/Germany<br \/>\n(September 25 - September 26, 2017)<\/td>\n<\/tr>\n<tr class=\"row-30 even\">\n\t<td class=\"column-1\">Philipp Birken<\/td><td class=\"column-2\">Lund University\/Sweden<br \/>\n(September 5 - September 6, 2017)<\/td>\n<\/tr>\n<tr class=\"row-31 odd\">\n\t<td class=\"column-1\">Thimot\u00e9e Schmoderer<\/td><td class=\"column-2\">Erasmus-student (traineeship), Institut National des Sciences Appliqu\u00e9es de Rouen\/France<br \/>\n(June 12 - September 8, 2017)<\/td>\n<\/tr>\n<tr class=\"row-32 even\">\n\t<td class=\"column-1\">Florian Hindenlang<\/td><td class=\"column-2\">Max-Planck-Institute for Plasma Physics, Garching\/Germany<br \/>\n(January 18 - January 20, 2017)<\/td>\n<\/tr>\n<tr class=\"row-33 odd\">\n\t<td class=\"column-1\">Rodrigo Costa Moura<\/td><td class=\"column-2\">PhD-student, Department of Aeronautics, Imperial College London\/UK<br \/>\n(December 1 - December 20, 2016)<\/td>\n<\/tr>\n<tr class=\"row-34 even\">\n\t<td class=\"column-1\">David Flad<\/td><td class=\"column-2\">Institute of Aerodynamics and Gasdynamics, University of Stuttgart\/Germany<br \/>\n(December 7 - December 9, 2016)<\/td>\n<\/tr>\n<tr class=\"row-35 odd\">\n\t<td class=\"column-1\">Florian Hindenlang<\/td><td class=\"column-2\">Max-Planck-Institute for Plasma Physics, Garching\/Germany<br \/>\n(June 23 - June 24, 2016)<\/td>\n<\/tr>\n<tr class=\"row-36 even\">\n\t<td class=\"column-1\">David C. Del Rey Fern\u00e1ndez<\/td><td class=\"column-2\">Institute for Aerospace Studies, University of Toronto\/Canada<br \/>\n(May 4 - June 1, 2016)<\/td>\n<\/tr>\n<tr class=\"row-37 odd\">\n\t<td class=\"column-1\">Hadi Minbashian<\/td><td class=\"column-2\">PhD-student, Amirkabir University of Technology, Tehran\/Iran<br \/>\n(June 29, 2015 - July 15, 2016)<\/td>\n<\/tr>\n<tr class=\"row-38 even\">\n\t<td class=\"column-1\">Mania Sabouri <\/td><td class=\"column-2\">PhD-student, Amirkabir University of Technology, Tehran\/Iran<br \/>\n(June 29, 2015 - July 15, 2016)<\/td>\n<\/tr>\n<tr class=\"row-39 odd\">\n\t<td class=\"column-1\">David A. Kopriva<\/td><td class=\"column-2\">Department of Mathematics, The Florida State University\/USA<br \/>\n(August 30 - September 13, 2015)<\/td>\n<\/tr>\n<tr class=\"row-40 even\">\n\t<td class=\"column-1\">Florian Hindenlang<\/td><td class=\"column-2\">Max-Planck-Institute for Plasma Physics, Garching\/Germany<br \/>\n(September 8 - September 9, 2015)<\/td>\n<\/tr>\n<tr class=\"row-41 odd\">\n\t<td class=\"column-1\"><\/td><td class=\"column-2\"><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<!-- #tablepress-21 from cache -->\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":9,"featured_media":0,"parent":183,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"post_mailing_queue_ids":[],"_links":{"self":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/pages\/3881"}],"collection":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/users\/9"}],"replies":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/comments?post=3881"}],"version-history":[{"count":1,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/pages\/3881\/revisions"}],"predecessor-version":[{"id":3882,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/pages\/3881\/revisions\/3882"}],"up":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/pages\/183"}],"wp:attachment":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/media?parent=3881"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}