{"id":176,"date":"2022-09-23T10:51:04","date_gmt":"2022-09-23T01:51:04","guid":{"rendered":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en2\/?post_type=case&#038;p=176"},"modified":"2022-09-23T10:45:59","modified_gmt":"2022-09-23T01:45:59","slug":"current_through_surface","status":"publish","type":"case","link":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/case\/current_through_surface\/","title":{"rendered":"Current passing through an arbitrary conductor cross-section"},"content":{"rendered":"<h3>summary<\/h3>\n<p>EMSolution has conventionally provided the CUR_FLUX option as a function for outputting the amount of current passing through an arbitrary cross section. However, no examples were available so far. The following is an introduction of the CUR_FLUX option using a model of <a href=\"\/product\/EMSolution\/en\/case\/bulk-steady-current\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;DC current field analysis of bulk conductors&quot;<\/font><\/a>. This option can also be used in AC steady-state and transient analyses.  <\/p>\n<h3>Explanation<\/h3>\n<p>The function of the CUR_FLUX option is explained using the models shown in Fig. 1(a) and (b), which simulate a conductor with two branches. Fig. 1(a) shows the same half model as in the <a href=\"\/product\/EMSolution\/en\/case\/bulk-steady-current\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;DC current field analysis of bulk conductors&quot;<\/font><\/a> and (b) shows the full model with a mirror copy of the mesh in the Y direction. The analytical conditions for both models are the same as in the <a href=\"\/product\/EMSolution\/en\/case\/bulk-steady-current\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;DC current field analysis of bulk conductors&quot;<\/font><\/a>, and the geometry of the two branches is the same, but the conductivity of one side is halved. This is equivalent to doubling the resistance. The analysis is performed by applying a DC current of 90 A to the underside of the branch as the input current. Calculating the amount of current passing through the branch using the &quot;Surfaces for current flux computation(11.3)&quot; function, we can confirm that the current passes through at a ratio of approximately 1:2 (Table 1). Naturally, the amount of current passing through the Half model and the Full model are identical.  <\/p>\n<div class=\"img col2\">\n<div>\n        <a href=\"\/product\/EMSolution\/en\/wp-content\/uploads\/current_through_surface01.png\" class=\"modal\"><br \/>\n        <img decoding=\"async\" src=\"\/product\/EMSolution\/en\/wp-content\/uploads\/current_through_surface01.png\" alt=\"\" \/><\/a><br \/>\n<!--        \n\n<p class=\"text01\">(a) Half\u30e2\u30c7\u30eb<\/p>\n\n--><\/p>\n<p style=\"text-align:center\">(a) Half model<\/p>\n<\/p><\/div>\n<div>\n        <a href=\"\/product\/EMSolution\/en\/wp-content\/uploads\/current_through_surface02.png\" class=\"modal\"><br \/>\n        <img decoding=\"async\" src=\"\/product\/EMSolution\/en\/wp-content\/uploads\/current_through_surface02.png\" alt=\"\" \/><\/a><br \/>\n<!--        \n\n<p class=\"text01\">(b) Full\u30e2\u30c7\u30eb<\/p>\n\n--><\/p>\n<p style=\"text-align:center\">(b) Full model<\/p>\n<\/p><\/div>\n<p class=\"caption\">Fig.1 Bifurcated conductor model (excluding air region)<\/p>\n<\/div>\n<h2 id=\"tablepress-20-name\" class=\"tablepress-table-name tablepress-table-name-id-20\">Table 1 Amount of Pass Through Current<\/h2>\n\n<table id=\"tablepress-20\" class=\"tablepress tablepress-id-20\" aria-labelledby=\"tablepress-20-name\">\n<thead>\n<tr class=\"row-1\">\n\t<th class=\"column-1\"><\/th><th colspan=\"2\" class=\"column-2\">Right Branch<\/th><th colspan=\"2\" class=\"column-4\">Left radical<\/th>\n<\/tr>\n<\/thead>\n<tbody class=\"row-hover\">\n<tr class=\"row-2\">\n\t<td class=\"column-1\">Model<\/td><td class=\"column-2\">Half<\/td><td class=\"column-3\">Full<\/td><td class=\"column-4\">Half<\/td><td class=\"column-5\">Full<\/td>\n<\/tr>\n<tr class=\"row-3\">\n\t<td class=\"column-1\">Amount of Pass Through Current<\/td><td class=\"column-2\">30.66A<\/td><td class=\"column-3\">30.66A<\/td><td class=\"column-4\">59.34A<\/td><td class=\"column-5\">59.34A<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n\n<p>This is a brief introduction to the function for outputting the amount of current passing through an arbitrary cross section. We hope you will use this function to output the amount of current passing through, for example, in a bulk conductor analysis or rotor bars and end rings of a three-dimensional induction machine analysis.  <\/p>\n<p><!--more--><\/p>\n<h3>How to use<\/h3>\n<p>Use CUR_FLUX in &quot;11. Printed Output&quot;. Use the surface element for output of the amount of current passing through.  <\/p>\n<p>The following items must be set  <\/p>\n<ul>\n<li>NO_SURFACES : Number of surface element properties that output the amount of passing current  <\/li>\n<li>MAT_ID_NOS : Property number of the face element\n<ul>\n<li>The face element must match the face of the conductor volume element.  <\/li>\n<li>The orientation of the face element (right-hand thread direction) is outward with respect to the volume element. Negative property numbers reverse the orientation of the face element (useful for two-dimensional analysis).  <\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p class=\"slideText\"><span>* Q_AVERAGE * HEAT * MAG_FLUX <font color=\"Red\">* CUR_FLUX *<\/font><\/span><br \/>\n<span>             0                0               0                    <font color=\"Red\">1<\/font><\/span><br \/>\n<span>* FORCE_J_B * FORCE_NODAL * MAGNETIC_ENERGY * IRON_LOSS *<\/span><br \/>\n<span>            0                       0                                 0                                 0<\/span><br \/>\n<font color=\"Red\"><span>* NO_SURFACES *<\/span><br \/>\n<span>              2<\/span><br \/>\n<span>* MAT_ID_NOS *<\/span><br \/>\n<span>       12     13<\/span><\/font>\n<\/p>\n<p>The calculation results are output to an output file.  <\/p>\n<p class=\"slideText\"><span>*************************************************<\/span><br \/>\n<span>*            Current fluxes Thhrough surfaces              *<\/span><br \/>\n<span>*************************************************<\/span><br \/>\n<span>   Surface Mat id      Current flux (A)<\/span><br \/>\n<span>              12             :      3.06607e+01<\/span><br \/>\n<span>              13             :      5.93393e+01<\/span>\n<\/p>\n<h3>Download<\/h3>\n<h4>Analysis Model<\/h4>\n<p><button type=\"button\" class=\"btn btn-danger btn-lg\"><a href=\"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-content\/uploads\/current_through_surface_data.zip\">Sample data DL<\/a><\/button>  <\/p>\n<p>\u30fb inputAC3D_DCCURR.ems : Input condition file<br \/>\n\u30fb pre_geom2D.neu : Mesh file<br \/>\n\u30fb 2D_to_3D : 2D mesh stacking file  <\/p>\n","protected":false},"excerpt":{"rendered":"<p>summary EMSolution has conventionally provided the CUR_FLUX option as a function for outputting the amount of current passing through an arbitrary cross section. However, no examples were available so far. The following is an introduction of the CUR_FLUX option using a model of &quot;DC current field analysis of bulk conductors&quot;. This option can also be [&hellip;]<\/p>\n","protected":false},"featured_media":0,"template":"","tags":[],"case_cat":[12],"class_list":["post-176","case","type-case","status-publish","hentry","case_cat-ninidanmen"],"acf":[],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/176"}],"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":5,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/176\/revisions"}],"predecessor-version":[{"id":2846,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/176\/revisions\/2846"}],"wp:attachment":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/media?parent=176"}],"wp:term":[{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/tags?post=176"},{"taxonomy":"case_cat","embeddable":true,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case_cat?post=176"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}