{"id":330497,"date":"2016-11-30T03:00:00","date_gmt":"2016-11-30T00:00:00","guid":{"rendered":"https:\/\/www.fyysika.ee\/?guid=12d2c370d7cbbdd05a21a95917ed8ee9"},"modified":"2016-11-30T03:00:00","modified_gmt":"2016-11-30T00:00:00","slug":"approximate-solution-of-a-thomas-fermi-model-equation-for-bulk-self-gravitating-stellar-objects-intwo-dimensions-2","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=330497","title":{"rendered":"Approximate solution of a Thomas\u2013Fermi model equation for bulk self-gravitating stellar objects in\r\ntwo dimensions"},"content":{"rendered":"<p>Direct variational methods are used to find simple approximate solutions of the Thomas\u2013Fermi<br \/>\nequations describing the properties of self-gravitating radially symmetric stellar objects both in<br \/>\nthe non-relativistic and ultra-relativistic cases. The approximate solutions are compared and shown<br \/>\nto be in good agreement with exact and numerically obtained solutions.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Direct variational methods are used to find simple approximate solutions of the Thomas\u2013Fermi<br \/>\nequations describing the properties of self-gravitating radially symmetric stellar objects both in<br \/>\nthe non-relativistic and ultra-relativistic cases. The a&#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-330497","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\/330497","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=330497"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/330497\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=330497"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=330497"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=330497"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}