{"id":743,"date":"2015-09-30T22:15:55","date_gmt":"2015-09-30T20:15:55","guid":{"rendered":"http:\/\/toschi.phys.tue.nl\/wordpress\/?p=743"},"modified":"2015-10-01T01:41:33","modified_gmt":"2015-09-30T23:41:33","slug":"pinaki-kumar","status":"publish","type":"post","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/pinaki-kumar\/","title":{"rendered":"Pinaki Kumar"},"content":{"rendered":"<div class=\"kcite-section\" kcite-section-id=\"743\">\n<div class='content-wrap'><p><strong>Earthquake dynamics - Understanding Their physics from modeling soft glassy materials<\/strong><\/p>\n<p><a href=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/09\/pinaki.jpg\"><img data-recalc-dims=\"1\" loading=\"lazy\" decoding=\"async\" data-attachment-id=\"744\" data-permalink=\"https:\/\/toschi.phys.tue.nl\/wordpress\/pinaki-kumar\/pinaki\/\" data-orig-file=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/09\/pinaki.jpg?fit=604%2C711&amp;ssl=1\" data-orig-size=\"604,711\" data-comments-opened=\"0\" data-image-meta=\"{&quot;aperture&quot;:&quot;0&quot;,&quot;credit&quot;:&quot;&quot;,&quot;camera&quot;:&quot;&quot;,&quot;caption&quot;:&quot;&quot;,&quot;created_timestamp&quot;:&quot;0&quot;,&quot;copyright&quot;:&quot;&quot;,&quot;focal_length&quot;:&quot;0&quot;,&quot;iso&quot;:&quot;0&quot;,&quot;shutter_speed&quot;:&quot;0&quot;,&quot;title&quot;:&quot;&quot;,&quot;orientation&quot;:&quot;1&quot;}\" data-image-title=\"pinaki\" data-image-description=\"\" data-image-caption=\"\" data-large-file=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/09\/pinaki.jpg?fit=604%2C711&amp;ssl=1\" class=\"alignleft size-medium wp-image-744\" src=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/09\/pinaki.jpg?resize=255%2C300\" alt=\"pinaki\" width=\"255\" height=\"300\" srcset=\"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/09\/pinaki.jpg?resize=255%2C300&amp;ssl=1 255w, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2015\/09\/pinaki.jpg?w=604&amp;ssl=1 604w\" sizes=\"auto, (max-width: 255px) 100vw, 255px\" \/><\/a>Developing a quantitative connection between the physics of complex soft-glassy materials below yield stress and the dynamics of stick-slip faulting events leading to earthquakes. A novel formulation based on the multicomponent Lattice Boltzmann method is\u00a0used to investigate fundamental issues related to natural seismicity, to find the interaction between spatially and temporally separated faulting events, as well as to determining the response of faults to external perturbations (i.e. induced seismicity) mimicking natural gas extraction and activities in injection wells. This earthquake model will then be fine tuned using inversion of surface seismic recordings.<\/p>\n<\/div><!-- kcite active, but no citations found -->\n<\/div> <!-- kcite-section 743 -->","protected":false},"excerpt":{"rendered":"<p>Earthquake dynamics - Understanding Their physics from modeling soft glassy materials Developing a quantitative connection between the physics of complex soft-glassy materials below yield stress and the dynamics of stick-slip faulting events leading to earthquakes. A novel formulation based on the multicomponent Lattice Boltzmann method is\u00a0used to investigate fundamental issues related to natural seismicity, to [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_exactmetrics_skip_tracking":false,"_exactmetrics_sitenote_active":false,"_exactmetrics_sitenote_note":"","_exactmetrics_sitenote_category":0,"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":"","jetpack_publicize_message":"","jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2}},"categories":[40],"tags":[],"class_list":["post-743","post","type-post","status-publish","format-standard","hentry","category-ph-d"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6tiMI-bZ","jetpack_likes_enabled":true,"jetpack-related-posts":[{"id":297,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/population-dynamics-under-flow-2\/","url_meta":{"origin":743,"position":0},"title":"Population dynamics under flow","author":"toschi","date":"June 6, 2013","format":false,"excerpt":"Various recent studies have revealed amazing phenomena in the dynamics of bacterial colonies where biology meets physics, in particular statistical physics, fluid dynamics, and (soft) con- densed matter. These biological systems reveal analogies with complex fluids (isotropic- nematic phase transitions), spinodal decomposition phenomena in physics and materials sci- ence, and\u2026","rel":"","context":"In &quot;biological fluid mechanics&quot;","block_context":{"text":"biological fluid mechanics","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/research\/biological-fluid-mechanics\/"},"img":{"alt_text":"","src":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/Untitled-3.jpg?fit=558%2C418&ssl=1&resize=350%2C200","width":350,"height":200,"srcset":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/Untitled-3.jpg?fit=558%2C418&ssl=1&resize=350%2C200 1x, https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/Untitled-3.jpg?fit=558%2C418&ssl=1&resize=525%2C300 1.5x"},"classes":[]},{"id":101,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/analysis-modeling-and-simulation-of-collective-dynamics-from-bacteria-to-crowds-2012\/","url_meta":{"origin":743,"position":1},"title":"Analysis, Modeling and Simulation of Collective Dynamics from Bacteria to Crowds  2012","author":"toschi","date":"February 9, 2012","format":false,"excerpt":"Analysis, Modeling and Simulation of Collective Dynamics from Bacteria to Crowds July 9, 2012 \u2014 July 13, 2012 Coordinators: Federico Toschi\u00a0(Eindhoven University of Technology, The Netherlands) Adrian Muntean\u00a0(Eindhoven University of Technology, The Netherlands) The collective motion of individuals (correlated motion of ants or migration of bacteria, flocks of birds, just\u2026","rel":"","context":"In &quot;conferences&quot;","block_context":{"text":"conferences","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/conferences\/"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":805,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/3mt100-chaos\/","url_meta":{"origin":743,"position":2},"title":"3MT100 - Chaos","author":"toschi","date":"February 3, 2016","format":false,"excerpt":"Chaos is the erratic behavior of simple nonlinear dynamical systems. This course covers the basic fundamentals of chaos theory, including the concept of scaling and universal route to chaos, and its connection to these non-linear, deterministic but unpredictable dynamical systems. From simple chaotic maps, to the physics of fractals and\u2026","rel":"","context":"In &quot;master&quot;","block_context":{"text":"master","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/teaching\/master\/"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":452,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/3cs03-caput-theoretical-physics-theory-of-liquids\/","url_meta":{"origin":743,"position":3},"title":"3CS03 - Caput Theoretical Physics: Theory of liquids","author":"toschi","date":"December 1, 2013","format":false,"excerpt":"Liquids lack the long-range order typical for solids. Collisional processes and short-range correlations distinguish liquids from dilute gases. Therefore, no idealized models comparable with the perfect gas or the harmonic solid are available for even simple liquids. During the last half of the 20th century a rapid progress has been\u2026","rel":"","context":"In &quot;master&quot;","block_context":{"text":"master","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/teaching\/master\/"},"img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":480,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/kim-alards\/","url_meta":{"origin":743,"position":4},"title":"Kim Alards","author":"toschi","date":"December 1, 2013","format":false,"excerpt":"Lagrangian analysis of rotating Rayleigh-B\u00e9nard turbulence Dynamics of particles in cylindrical rotating Rayleigh-B\u00e9nard convection (RRBC) is studied using DNS, not only to understand the physics of RRBC, but also to investigate whether particles with a feedback reaction on the flow can influence the dynamics within the cell. Lagrangian statistics is\u2026","rel":"","context":"In &quot;ph.d.&quot;","block_context":{"text":"ph.d.","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/students\/ph-d\/"},"img":{"alt_text":"KimAlards","src":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/12\/KimAlards-242x300.jpg?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":373,"url":"https:\/\/toschi.phys.tue.nl\/wordpress\/373\/","url_meta":{"origin":743,"position":5},"title":"Physics of crowds","author":"toschi","date":"June 11, 2013","format":false,"excerpt":"[sz-video url=\"http:\/\/vimeo.com\/68242210\"\/]","rel":"","context":"In &quot;ongoing work&quot;","block_context":{"text":"ongoing work","link":"https:\/\/toschi.phys.tue.nl\/wordpress\/category\/research\/ongoing-work\/"},"img":{"alt_text":"kSnap-19-23-34-108_66","src":"https:\/\/i0.wp.com\/toschi.phys.tue.nl\/wordpress\/wp-content\/uploads\/2013\/06\/kSnap-19-23-34-108_66.png?resize=350%2C200","width":350,"height":200},"classes":[]}],"_links":{"self":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts\/743","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/comments?post=743"}],"version-history":[{"count":5,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts\/743\/revisions"}],"predecessor-version":[{"id":753,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/posts\/743\/revisions\/753"}],"wp:attachment":[{"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/media?parent=743"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/categories?post=743"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/toschi.phys.tue.nl\/wordpress\/wp-json\/wp\/v2\/tags?post=743"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}