{"id":395934,"date":"2017-04-12T02:00:00","date_gmt":"2017-04-11T23:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=97274239939775090ff4695a1b89ad08"},"modified":"2017-04-12T02:00:00","modified_gmt":"2017-04-11T23:00:00","slug":"electromagnetic-angular-momentum-in-quasi-static-conditions","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=395934","title":{"rendered":"Electromagnetic angular momentum in quasi-static conditions"},"content":{"rendered":"<p>The correct definition of electromagnetic momentum in matter, either Abraham\u2019s g A\u00a0=\u00a0(1\/4 \u03c0 c) (<br \/>\nE\u00a0\u00d7\u00a0H ), or Minkowski\u2019s g M\u00a0=\u00a0(1\/4 \u03c0 c) ( D\u00a0\u00d7\u00a0B ) has been a theme of controversy for a century.<br \/>\nTherefore, we can find those who favor one or the other of these proposals. We present here an<br \/>\nalternative view, considering that both of the aforementioned equations are equivalent since they<br \/>\npertain to different balance equations derived from the macroscopic Maxwell equations. This is done<br \/>\nthrough their application to a device proposed by Lai in 1980, and recovering his results. Advanced<br \/>\nundergraduate and graduate students can find in this work an introduction to a controversial issue<br \/>\nand an alternative point of view about it.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The correct definition of electromagnetic momentum in matter, either Abraham\u2019s g A\u00a0=\u00a0(1\/4 \u03c0 c) (<br \/>\nE\u00a0\u00d7\u00a0H ), or Minkowski\u2019s g M\u00a0=\u00a0(1\/4 \u03c0 c) ( D\u00a0\u00d7\u00a0B ) has been a theme of controversy for a century.<br \/>\nTherefore, we can find those who favor o&#8230;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[178],"tags":[],"class_list":{"0":"post-395934","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-fuusikaharidus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/395934","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=395934"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/395934\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=395934"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=395934"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=395934"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}