{"id":4596,"date":"2020-11-10T11:20:56","date_gmt":"2020-11-10T16:20:56","guid":{"rendered":"https:\/\/engineering.jhu.edu\/lefd\/?page_id=4596"},"modified":"2020-11-10T11:20:56","modified_gmt":"2020-11-10T16:20:56","slug":"veno-arterial-ecmo-flows","status":"publish","type":"page","link":"https:\/\/engineering.jhu.edu\/lefd\/cardiovascular-and-cerebrovascular-flows\/veno-arterial-ecmo-flows\/","title":{"rendered":"Veno-arterial ECMO Flows"},"content":{"rendered":"<h2>People<\/h2>\n<table style=\"height: 70px;\" width=\"100%\">\n<tbody>\n<tr>\n<td width=\"301\">Graduate student<\/td>\n<td width=\"301\">Zeng Zhang<\/td>\n<\/tr>\n<tr>\n<td width=\"301\">Project Supervisor<\/td>\n<td width=\"301\">Prof. Joseph Katz<\/td>\n<\/tr>\n<tr>\n<td width=\"301\">Project Collaborator<\/td>\n<td width=\"301\">Prof. Dan Choi (JHMI), Dr. Xun Zhou (JHMI)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h2>Introduction<\/h2>\n<div id=\"attachment_4599\" style=\"width: 360px\" class=\"wp-caption alignleft\"><a href=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/VAECMO1.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-4599\" class=\"wp-image-4599\" src=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/VAECMO1.jpg\" alt=\"\" width=\"350\" height=\"204\" srcset=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/VAECMO1.jpg 729w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/VAECMO1-300x175.jpg 300w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/VAECMO1-200x117.jpg 200w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/VAECMO1-150x87.jpg 150w\" sizes=\"auto, (max-width: 350px) 100vw, 350px\" \/><\/a><p id=\"caption-attachment-4599\" class=\"wp-caption-text\">Figure. 1 Sketch of V-A ECMO system<\/p><\/div>\n<p style=\"text-align: justify; text-indent: 36px;\">Veno-arterial extracorporeal membrane oxygenation (VA-ECMO) is a salvage therapy that provides patients with both respiratory and circulatory support by draining blood from the venous system, oxygenating it outside the body, and returning it retrogradely to the arterial system. The most commonly applied configuration is femoral-femoral VA-ECMO, in which the arterial flow to the patient is retrograde via the femoral artery. It has been widely applied to patients with cardiogenic shock, severe cardiac failure, and chronic cardiomyopathy. However, determining the optimal VA-ECMO flow rate (<em>Q<sub>E<\/sub><\/em>) is challenging. High <em>Q<sub>E<\/sub><\/em> is favorable for adequate end-organ perfusion. Nonetheless, it has been proposed that retrograde arterial flow may increase the afterload to the heart. Consequently, the metabolic work demand on the myocardium might increase, hindering myocardial tissue recovery. Clinical management relies on monitoring the hemodynamic states, but outcomes of the therapy are influenced by the patient- and treatment-related factors. Insights regarding the interactions between ECMO flows and native cardiac output at the admixing zone may lead to quantitative assessment of the impact of the afterload created by the retrograde arterial flow.<\/p>\n<p style=\"text-align: justify; text-indent: 36px;\">This project uses the optimized echo-PIV\/PTV to characterize the interactions between ECMO flow and native cardiac output in the aortic root of a Yorkshire pig with severe myocardial ischemia. The instantaneous and phase-averaged velocity distributions are analyzed to elucidate the effects of the ECMO flow rate on the flow patterns, as well as the duration and magnitude of cardiac outflow.<\/p>\n<h2>Results<\/h2>\n<div id=\"attachment_4609\" style=\"width: 510px\" class=\"wp-caption aligncenter\"><a href=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-scaled.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-4609\" class=\"wp-image-4609\" src=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-852x1024.jpg\" alt=\"\" width=\"500\" height=\"601\" srcset=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-852x1024.jpg 852w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-249x300.jpg 249w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-166x200.jpg 166w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-768x923.jpg 768w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-1277x1536.jpg 1277w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-1703x2048.jpg 1703w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_6-125x150.jpg 125w\" sizes=\"auto, (max-width: 500px) 100vw, 500px\" \/><\/a><p id=\"caption-attachment-4609\" class=\"wp-caption-text\">Figure. 2 Vectors and contour maps of the phase-averaged velocity magnitude (|V|) for varying ECMO flow rates (rows) and phases in the cardiac cycle (columns).<\/p><\/div>\n<p style=\"text-align: justify; text-indent: 36px;\">Figure 2 shows the phase-averaged velocity for five selected phases of the cardiac cycle for all the present values of <em>Q<sub>E<\/sub><\/em>. The selected phases (\u03a6) are specified as a percentage of the cardiac cycle, starting from the R wave peak of the ECG. As is evident, the jetting during systole (\u03a6~40%) strengthens as <em>Q<sub>E<\/sub><\/em> is decreased from 4.0 to 3.0L\/min, but then decreases with further reduction of the flow rate. During diastole, prominent secondary flows consist of a clockwise vortex in the sinus at <em>Q<sub>E<\/sub><\/em>\u22653.0L\/min, and a counterclockwise vortex above the sino-tubular junction at lower <em>Q<sub>E<\/sub><\/em>.<\/p>\n<div id=\"attachment_4649\" style=\"width: 460px\" class=\"wp-caption alignleft\"><a href=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-scaled.jpg\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-4649\" class=\"wp-image-4649\" src=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-300x131.jpg\" alt=\"\" width=\"450\" height=\"197\" srcset=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-300x131.jpg 300w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-1024x449.jpg 1024w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-200x88.jpg 200w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-768x337.jpg 768w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-1536x673.jpg 1536w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-2048x898.jpg 2048w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_9-150x66.jpg 150w\" sizes=\"auto, (max-width: 450px) 100vw, 450px\" \/><\/a><p id=\"caption-attachment-4649\" class=\"wp-caption-text\">Figure. 3 Phase evolution of (a) the spatially averaged velocity and (b) acceleration<\/p><\/div>\n<div id=\"attachment_4651\" style=\"width: 460px\" class=\"wp-caption alignleft\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-4651\" class=\"wp-image-4651\" src=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-300x136.jpg\" alt=\"\" width=\"450\" height=\"204\" srcset=\"https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-300x136.jpg 300w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-1024x463.jpg 1024w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-200x90.jpg 200w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-768x347.jpg 768w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-1536x695.jpg 1536w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-2048x926.jpg 2048w, https:\/\/engineering.jhu.edu\/lefd\/wp-content\/uploads\/2020\/09\/BIO-20-1256_figure_10-150x68.jpg 150w\" sizes=\"auto, (max-width: 450px) 100vw, 450px\" \/><p id=\"caption-attachment-4651\" class=\"wp-caption-text\">Figure. 4 Variations of (a) maximum velocity, maximum deceleration magnitude, the phase interval between valve opening and closing (\u0394\u03a6open), phase of the maximum deceleration, and (b) velocity-time integral (VTI) over 1min calculated, and MAP during image acquisition with ECMO flowrate.<\/p><\/div>\n<p style=\"text-align: justify; text-indent: 36px;\">Two flow rate regimes are identified: For <em>Q<sub>E<\/sub><\/em>\u22653.0L\/min, the maximum velocity, phase of peak deceleration, duration with open valve, MAP and VTI increase with decreasing flow rate, peaking at <em>Q<sub>E<\/sub><\/em>=3.0L\/min, suggestive of sufficient ECMO support. Conversely, for <em>Q<sub>E<\/sub><\/em>\u22642.5L\/min, as the ECMO flow rate is reduced, the peak velocity, MAP and VTI decrease, while the phase of peak deceleration and duration with open valve plateau during systole. The deceleration during the transition to diastole is much milder in this range. Since the recommended optimal veno-arterial ECMO flow rate should be the lowest level that maintains adequate tissue perfusion, <em>Q<sub>E<\/sub><\/em>=3.0L\/min appears to be the optimal flow rate for the particular physiological condition for this study.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>People Graduate student Zeng Zhang Project Supervisor Prof. Joseph Katz Project Collaborator Prof. Dan Choi (JHMI), Dr. Xun Zhou (JHMI) Introduction Veno-arterial extracorporeal membrane oxygenation (VA-ECMO) is a salvage therapy that provides patients with both respiratory and circulatory support by &hellip; <a href=\"https:\/\/engineering.jhu.edu\/lefd\/cardiovascular-and-cerebrovascular-flows\/veno-arterial-ecmo-flows\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":5588,"featured_media":0,"parent":4688,"menu_order":3,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_exactmetrics_skip_tracking":false,"_exactmetrics_sitenote_active":false,"_exactmetrics_sitenote_note":"","_exactmetrics_sitenote_category":0,"footnotes":""},"class_list":["post-4596","page","type-page","status-publish","hentry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.9 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Veno-arterial ECMO Flows - Laboratory for Experimental Fluid Dynamics<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/engineering.jhu.edu\/lefd\/cardiovascular-and-cerebrovascular-flows\/veno-arterial-ecmo-flows\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Veno-arterial ECMO Flows - Laboratory for Experimental Fluid Dynamics\" \/>\n<meta property=\"og:description\" content=\"People Graduate student Zeng Zhang Project Supervisor Prof. Joseph Katz Project Collaborator Prof. Dan Choi (JHMI), Dr. Xun Zhou (JHMI) Introduction Veno-arterial extracorporeal membrane oxygenation (VA-ECMO) is a salvage therapy that provides patients with both respiratory and circulatory support by &hellip; 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