{"id":154,"date":"2025-08-01T17:13:41","date_gmt":"2025-08-01T17:13:41","guid":{"rendered":"https:\/\/comphysics.com\/?p=154"},"modified":"2026-08-28T19:22:04","modified_gmt":"2026-08-28T10:22:04","slug":"introduction-of-e2m-a-1d-electro-magnetic-simulator-based-on-ios","status":"publish","type":"post","link":"https:\/\/comphysics.com\/index.php\/2025\/08\/01\/introduction-of-e2m-a-1d-electro-magnetic-simulator-based-on-ios\/","title":{"rendered":"Introducing E2M: A 1D Electromagnetic Simulator for iOS"},"content":{"rendered":"\n

E2M, short for \u201cEngineer with EM Waves,\u201d was scheduled for release on iOS in August 2025. It is an electromagnetic simulator for one-dimensional stacked (layered) structures composed of linear, homogeneous, isotropic (LHI) materials. The nine figures below summarize the original release features.<\/p>\n\n\n\n

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E2M makes these analysis functions available through a touch-based interface on iPhone and iPad. It is intended for electromagnetic problems that are inherently one-dimensional or can be represented accurately as one-dimensional layered structures.<\/p>\n","protected":false},"excerpt":{"rendered":"

An introduction to E2M, a native iOS simulator for one-dimensional electromagnetic analysis of layered LHI materials.<\/p>\n","protected":false},"author":1,"featured_media":130,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-154","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-e2m"],"_links":{"self":[{"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/posts\/154","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/comments?post=154"}],"version-history":[{"count":15,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/posts\/154\/revisions"}],"predecessor-version":[{"id":651,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/posts\/154\/revisions\/651"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/media\/130"}],"wp:attachment":[{"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/media?parent=154"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/categories?post=154"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/comphysics.com\/index.php\/wp-json\/wp\/v2\/tags?post=154"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}