{"id":140,"date":"2022-09-23T13:24:13","date_gmt":"2022-09-23T04:24:13","guid":{"rendered":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en2\/?post_type=case&#038;p=140"},"modified":"2022-09-23T11:46:53","modified_gmt":"2022-09-23T02:46:53","slug":"loop","status":"publish","type":"case","link":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/case\/loop\/","title":{"rendered":"Surface inflow current source in a closed loop (SUFCUR)"},"content":{"rendered":"<h3>Summary<\/h3>\n<p>When using SUFCUR as a bulk conductor surface inflow source, if there is a $B_n$=0 symmetry condition, defining a face element on one $B_n$=0 face makes that face the positive electrode and the other $B_n$=0 face the negative electrode and current flows out. When there is no such symmetry condition and current is induced by applying a voltage to the loop conductor, a gap element is used.  <\/p>\n<h3>Explanation<\/h3>\n<div class=\"img col2\">\n<div>\n        <a href=\"\/product\/EMSolution\/en\/wp-content\/uploads\/loop01.png\" class=\"modal\"><br \/>\n        <img decoding=\"async\" src=\"\/product\/EMSolution\/en\/wp-content\/uploads\/loop01.png\" alt=\"\" \/><\/a><br \/>\n<!--        \n\n<p class=\"text01\">Fig.1\u3000\u9589\u30eb\u30fc\u30d7\u30d0\u30eb\u30af\u5c0e\u4f53\u3078\u306e<br \/>\u9762\u96fb\u6d41\u6d41\u5165\u30bd\u30fc\u30b9<\/p>\n\n--><\/p>\n<p style=\"text-align:center\">Fig.1 Surface current inflow source in a closed loop bulk conductor<\/p>\n<\/p><\/div>\n<div>\n        <a href=\"\/product\/EMSolution\/en\/wp-content\/uploads\/loop02.png\" class=\"modal\"><br \/>\n        <img decoding=\"async\" src=\"\/product\/EMSolution\/en\/wp-content\/uploads\/loop02.png\" alt=\"\" \/><\/a><br \/>\n<!--        \n\n<p class=\"text01\">Fig.2\u3000\u767a\u71b1\u5bc6\u5ea6\u5206\u5e03<\/p>\n\n--><\/p>\n<p style=\"text-align:center\">Fig.2 Heat generation density distribution<\/p>\n<\/p><\/div>\n<\/div>\n<p>When a gap element is specified, electrical potentials are defined on both sides of it. If you define a SUFCUR surface to overlap that surface, a positive potential is defined on the positive side of the gap (in the right-hand thread direction of the element) and the negative side is set to zero.  <\/p>\n<p>Suppose we have a closed loop conductor as shown in Fig. 1. In this case we can use the symmetry condition, but we will solve for the entire upper half. Define a gap surface as shown in the figure. Gap surface elements can also be used as SUFCUR definition elements. First, create a mesh by extending in the z-direction from pre_geom2D.neu and 2D_to_3D, define the gap surface and SUFCUR surface with input, and perform an AC steady-state analysis. The loop current is induced as shown in Fig. 1, and the heat generation distribution is shown in Fig. 2.  <\/p>\n<p>Here we have shown the case where SUFCUR is defined on a symmetrical surface, but it can also be defined in an asymmetrical position. It can also be used in combination with a gap element on one end face, even when using rotational symmetry. $\\Rightarrow$ <a href=\"\/product\/EMSolution\/en\/case\/nonsym\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;SUFCUR at asymmetric locations or periodic boundaries&quot;<\/font><\/a>.  <\/p>\n<p><!--more--><\/p>\n<h3>How to use<\/h3>\n<p>Set the gap surface and SUFCUR definition surface to serve as a dual-use surface.  <\/p>\n<p class=\"slideText\"><font color=\"Red\">* SMAT_ID * TYPE *<\/font> SIGMA *   MU   * THICK *<br \/>\n<font color=\"Red\">         3              2<\/font>            0.0       1.0         0.0<br \/>\n* SOURCE *<br \/>\n   SOURCE<br \/>\n* SUFCUR * SERIES_NO * TIME_ID <font color=\"Red\">* SURFACE_MAT_ID *<\/font> CURRENT *<br \/>\n   SUFCUR             1                   0                        <font color=\"Red\">3<\/font>                          1.0\n<\/p>\n<h3>Download<\/h3>\n<p><button type=\"button\" class=\"btn btn-danger btn-lg\"><a href=\"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-content\/uploads\/gap-loop.zip\">Sample data DL<\/a><\/button>  <\/p>\n<p>\u30fb input2D<br \/>\n\u30fb pre_geom2D.neu<br \/>\n\u30fb 2D_to_3D  <\/p>\n","protected":false},"excerpt":{"rendered":"<p>Summary When using SUFCUR as a bulk conductor surface inflow source, if there is a $B_n$=0 symmetry condition, defining a face element on one $B_n$=0 face makes that face the positive electrode and the other $B_n$=0 face the negative electrode and current flows out. When there is no such symmetry condition and current is induced [&hellip;]<\/p>\n","protected":false},"featured_media":0,"template":"","tags":[],"case_cat":[8],"class_list":["post-140","case","type-case","status-publish","hentry","case_cat-gap"],"acf":[],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/140"}],"collection":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case"}],"about":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/types\/case"}],"version-history":[{"count":8,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/140\/revisions"}],"predecessor-version":[{"id":2950,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/140\/revisions\/2950"}],"wp:attachment":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/media?parent=140"}],"wp:term":[{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/tags?post=140"},{"taxonomy":"case_cat","embeddable":true,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case_cat?post=140"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}