{"id":2337,"date":"2013-08-05T16:03:32","date_gmt":"2013-08-05T16:03:32","guid":{"rendered":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/files\/2013\/06\/farnoosh_scattering01b.gif"},"modified":"2013-08-05T16:03:32","modified_gmt":"2013-08-05T16:03:32","slug":"farnoosh_scattering01b","status":"inherit","type":"attachment","link":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/partial-differential-equation-integral-equation-pde-ie-solvers-for-electromagnetic-scattering\/farnoosh_scattering01b\/","title":{"rendered":"Figure 1"},"author":370,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"description":{"rendered":"<p class=\"attachment\"><a href='https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b.gif' rel=\"lightbox[2337]\"><img width=\"300\" height=\"203\" src=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-300x203.gif\" class=\"attachment-medium size-medium\" alt=\"\" loading=\"lazy\" srcset=\"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-300x203.gif 300w, https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-220x149.gif 220w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n"},"caption":{"rendered":"<p>Figure 1: FEM-BEM domain decomposition and cement variables.<\/p>\n"},"alt_text":"","media_type":"image","mime_type":"image\/gif","media_details":{"width":840,"height":570,"file":"2013\/06\/farnoosh_scattering01b.gif","sizes":{"thumbnail":{"file":"farnoosh_scattering01b-150x150.gif","width":150,"height":150,"mime_type":"image\/gif","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-150x150.gif"},"medium":{"file":"farnoosh_scattering01b-300x203.gif","width":300,"height":203,"mime_type":"image\/gif","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-300x203.gif"},"post-thumbnail":{"file":"farnoosh_scattering01b-150x150.gif","width":150,"height":150,"mime_type":"image\/gif","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-150x150.gif"},"abstract-thumb":{"file":"farnoosh_scattering01b-220x149.gif","width":220,"height":149,"mime_type":"image\/gif","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b-220x149.gif"},"full":{"file":"farnoosh_scattering01b.gif","width":840,"height":570,"mime_type":"image\/gif","source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b.gif"}},"image_meta":{"aperture":0,"credit":"","camera":"","caption":"","created_timestamp":0,"copyright":"","focal_length":0,"iso":0,"shutter_speed":0,"title":""}},"post":912,"source_url":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-content\/blogs.dir\/22\/files\/2013\/06\/farnoosh_scattering01b.gif","_links":{"self":[{"href":"https:\/\/mtlsites.mit.edu\/annual_reports\/2013\/wp-json\/wp\/v2\/media\/2337"}],"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=2337"}]}}