{"id":1261,"date":"2013-07-01T18:01:21","date_gmt":"2013-07-01T18:01:21","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/07\/kwak_electrodialysis_02.jpg"},"modified":"2013-07-01T18:01:21","modified_gmt":"2013-07-01T18:01:21","slug":"kwak_electrodialysis_02","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/sheared-electroconvective-vortices-in-electrodialysis\/kwak_electrodialysis_02\/","title":{"rendered":"Figure 1"},"author":370,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"description":{"rendered":"

\"\"<\/a><\/p>\n"},"caption":{"rendered":"

Figure 1: Sheared ICP is visualized by showing local ion concentration profiles (Figures 1(a) and (c)) and EC vortices (Figures 1(b) and (d)) from experiment (at voltage V=10 V and average flow velocity UHP = 0.83 mm\/s (flow rate Q=10 \u00b5L\/min) (Figure 1(a-b)) and simulation (at V= 25V0 and UHP= 80U0, where V0 =25 mV and U0 =29.66 \u00b5m\/s) (Figure 1(c-d)). Cation exchange membrane (CEM) (anion exchange membrane (AEM)) is located at lower (upper) side of the channel, and ratio of channel width to length is 1:5 in both experiment and simulation. In the experiment, local ion concentration was tracked with 10-\u00b5M Rhodamine 6G (R6G), and circular depletion boundary layers dbl are observed as a dark region caused by depletion of R6G (Figure 2(a)); in simulation, ion depletion is represented as a blue region (Figure 2(c)). Fluid flows were visualized by stacking time-lapse images of 10-\u00b5m polystyrene (PS) beads (Figure 2(b)). Vortex evolution is clearly visualized at entrance region in experiment and simulation (yellow and white dotted lines). <\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/jpeg","media_details":{"width":502,"height":514,"file":"2013\/07\/kwak_electrodialysis_02.jpg","sizes":{"thumbnail":{"file":"kwak_electrodialysis_02-150x150.jpg","width":150,"height":150,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/kwak_electrodialysis_02-150x150.jpg"},"medium":{"file":"kwak_electrodialysis_02-292x300.jpg","width":292,"height":300,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/kwak_electrodialysis_02-292x300.jpg"},"post-thumbnail":{"file":"kwak_electrodialysis_02-150x150.jpg","width":150,"height":150,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/kwak_electrodialysis_02-150x150.jpg"},"abstract-thumb":{"file":"kwak_electrodialysis_02-214x220.jpg","width":214,"height":220,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/kwak_electrodialysis_02-214x220.jpg"},"full":{"file":"kwak_electrodialysis_02.jpg","width":502,"height":514,"mime_type":"image\/jpeg","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/kwak_electrodialysis_02.jpg"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":1260,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/07\/kwak_electrodialysis_02.jpg","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/1261"}],"collection":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media"}],"about":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/types\/attachment"}],"author":[{"embeddable":true,"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/users\/370"}],"replies":[{"embeddable":true,"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/comments?post=1261"}]}}