{"id":402,"date":"2020-01-10T11:59:02","date_gmt":"2020-01-10T16:59:02","guid":{"rendered":"https:\/\/engineering.jhu.edu\/tryggvason\/?page_id=402"},"modified":"2025-06-20T11:12:43","modified_gmt":"2025-06-20T15:12:43","slug":"multiscale-modeling","status":"publish","type":"page","link":"https:\/\/engineering.jhu.edu\/tryggvason\/multiscale-modeling\/","title":{"rendered":"Multiscale Modeling"},"content":{"rendered":"\n<p>Multiphase flows, such as atomizing jets, are notorious for generating structures&nbsp;that are&nbsp;much smaller than the dominant scales in the flow. Those features often&nbsp;have significant&nbsp;influence on the overall atomization and must therefore be&nbsp;captured in some way, but&nbsp;their smallness makes them very expensive to&nbsp;resolve using standard numerical&nbsp;approaches.<\/p>\n\n\n\n<p>In many cases, however, these small scale features are relatively simple, since&nbsp;surface&nbsp;tension effects are strong and keep the geometry simple and viscous dominate so flow is&nbsp;simple. Simple flows in simple geometries can often be modeled using analytical&nbsp;or semi-analytical methods and we have explored ways to combine analytical&nbsp;or semi-analytical&nbsp;models with numerical solution that resolves the rest of the&nbsp;flow accurately.&nbsp;<\/p>\n\n\n\n<p>Our work includes early work on strained-diffusion&nbsp;combustion [1,2], and more recent&nbsp;studies of the draining of thin films [3] and mass transfer&nbsp;from&nbsp;gas bubbles in high&nbsp;Schmidt number liquids [4,5].&nbsp;<\/p>\n\n\n\n<h4 class=\"wp-block-heading\">References<\/h4>\n\n\n\n<p>[1] C. Chang, W. Dahm, and G. Tryggvason. Lagrangian model&nbsp;simulations of molecular&nbsp;mixing, in-&nbsp;cluding finite rate chemical&nbsp;reactions, in a temporally developing shear layer.&nbsp;Physics of&nbsp;Fluids A,&nbsp;3:1300\u20131311, 1991.<\/p>\n\n\n\n<p>&nbsp;[2] W. Dahm, G. Tryggvason, and M. Zhuang. Integral&nbsp;method solution of time-dependent strained&nbsp;diffusion-reaction equations with multi-step kinetics.&nbsp;SIAM J. Appl.&nbsp;Math., 56(4):1039\u20131059, 1996.&nbsp;<\/p>\n\n\n\n<p>[3] S. Thomas, A. Esmaeeli, and G. Tryggvason. Multiscale&nbsp;computations of thin films in&nbsp;multiphase&nbsp;flows.&nbsp;International&nbsp;Journal of Multiphase Flow, 36:71\u201377, 2010.<\/p>\n\n\n\n<p>[4] B. Aboulhasanzadeh, S. Hosoda, A. Tomiyama, and G.&nbsp;Tryggvason. A validation of an&nbsp;embedded&nbsp;analytical&nbsp;description approach to the computations of mass transfer&nbsp;from&nbsp;bubbles in high schmidt&nbsp;number liquids.&nbsp;Chemical&nbsp;Engineering Science, 101:165\u2013174,&nbsp;2013.<\/p>\n\n\n\n<p>[5] B. Aboulhasanzadeh, S. Thomas, M. Taeibi-Rahni, and&nbsp;G. Tryggvason. Multiscale&nbsp;computations of&nbsp;mass transfer&nbsp;from buoyant bubbles.&nbsp;Chemical Engineering Science,&nbsp;75:456\u2013467, 2012.&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Multiphase flows, such as atomizing jets, are notorious for generating structures&nbsp;that are&nbsp;much smaller than the dominant scales in the flow. Those features often&nbsp;have significant&nbsp;influence on the overall atomization and must therefore be&nbsp;captured in some way, but&nbsp;their smallness makes them very expensive to&nbsp;resolve using standard numerical&nbsp;approaches. In many cases, however, these small scale features are relatively [&hellip;]<\/p>\n","protected":false},"author":16,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"template-full.php","meta":{"_uag_custom_page_level_css":"","footnotes":""},"class_list":["post-402","page","type-page","status-publish","hentry"],"uagb_featured_image_src":{"full":false,"thumbnail":false,"medium":false,"medium_large":false,"large":false,"1536x1536":false,"2048x2048":false},"uagb_author_info":{"display_name":"atran23","author_link":"https:\/\/engineering.jhu.edu\/tryggvason\/author\/atran23\/"},"uagb_comment_info":0,"uagb_excerpt":"Multiphase flows, such as atomizing jets, are notorious for generating structures&nbsp;that are&nbsp;much smaller than the dominant scales in the flow. Those features often&nbsp;have significant&nbsp;influence on the overall atomization and must therefore be&nbsp;captured in some way, but&nbsp;their smallness makes them very expensive to&nbsp;resolve using standard numerical&nbsp;approaches. In many cases, however, these small scale features are relatively&hellip;","_links":{"self":[{"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/pages\/402","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/users\/16"}],"replies":[{"embeddable":true,"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/comments?post=402"}],"version-history":[{"count":5,"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/pages\/402\/revisions"}],"predecessor-version":[{"id":947,"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/pages\/402\/revisions\/947"}],"wp:attachment":[{"href":"https:\/\/engineering.jhu.edu\/tryggvason\/wp-json\/wp\/v2\/media?parent=402"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}