{"id":99,"date":"2022-08-26T10:07:49","date_gmt":"2022-08-26T01:07:49","guid":{"rendered":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en2\/?post_type=case&#038;p=99"},"modified":"2022-08-26T15:01:20","modified_gmt":"2022-08-26T06:01:20","slug":"phicoil_loop","status":"publish","type":"case","link":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/case\/phicoil_loop\/","title":{"rendered":"Loop current defined by Potential Current Source (PHICOIL)"},"content":{"rendered":"<h3>Summary<\/h3>\n<p>EMSolution has a <a href=\"\/product\/EMSolution\/en\/case\/phicoil\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;potential current source (PHICOIL)&quot;<\/font><\/a> expressed by an electric scalar potential. With this feature, coil currents flowing in and out of the Bn=0 surface and currents flowing in and out of periodically symmetric surfaces can be defined. We are pleased to report that PHICOIL can now be used to define coils that loop in the computational domain.  <\/p>\n<h3>Explanation<\/h3>\n<p>The representation of a looping coil by a surface inflow current source (SUFCUR) has already been described, but here it is represented by a gap element as well. As shown in Fig.1, the gap surface is defined in the form of a disconnection that is one or more layers out from the coil conductor. Current is defined in the direction of the gap surface (right-hand thread direction in nodal order). In Fig.1, the symmetry condition for the Ht=0 plane is used, but it is not necessary to define beyond the symmetry plane.   <\/p>\n<div class=\"img col1\">\n<div>\n        <a href=\"\/product\/EMSolution\/en\/wp-content\/uploads\/phicoil_loop01.png\" class=\"modal\"><br \/>\n        <img decoding=\"async\" src=\"\/product\/EMSolution\/en\/wp-content\/uploads\/phicoil_loop01.png\" alt=\"\" \/><\/a><br \/>\n<!--        \n\n<p class=\"text01\">Fig.1\u3000PHICOIL\u30e2\u30c7\u30eb\u3068\u96fb\u6d41\u5bc6\u5ea6\u5206\u5e03<\/p>\n\n--><\/p>\n<p style=\"text-align:center\">Fig.1 PHICOIL model and current density distribution<\/p>\n<\/p><\/div>\n<\/div>\n<p>The current density distribution defined by PHICOIL shows an inward current distribution where the coil bends, as shown in Fig. 1. In this model, the coil can also be defined by <a href=\"\/product\/EMSolution\/en\/case\/elmcur\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;internal current source (ELMCUR)&quot;<\/font><\/a> or <a href=\"\/product\/EMSolution\/en\/case\/sdefcoil\/\" target=\"_blank\" rel=\"noopener noreferrer\" style=\"display:inline\"><font color=\"Red\">&quot;surface defined current source (SDEFCOIL)&quot;<\/font><\/a>, but PHICOIL does not require a rectangular cross-section and is easier to define.\u3000SUFCUR can be used for AC steady-state calculations and transient analysis, but the current distribution is not fixed and corresponds to current flowing through a bulk conductor and cannot be used for static magnetic field analysis. PHICOIL has a fixed current distribution and can be used in DC analysis by giving the DC steady-state current distribution as a coil source. Fig. 2 shows the current distribution obtained by SUFCUR for the same model with a very long time period of 100 s. It is almost the same as in Fig. 1, and you can see that the current in PHICOIL corresponds to the DC steady-state current.<\/p>\n<div class=\"img col1\">\n<div>\n        <a href=\"\/product\/EMSolution\/en\/wp-content\/uploads\/phicoil_loop02.png\" class=\"modal\"><br \/>\n        <img decoding=\"async\" src=\"\/product\/EMSolution\/en\/wp-content\/uploads\/phicoil_loop02.png\" alt=\"\" \/><\/a><br \/>\n<!--        \n\n<p class=\"text01\">Fig.2\u3000SUFCUR\u306b\u3088\u3063\u3066\u6c42\u3081\u305f\u96fb\u6d41\u5206\u5e03(0.01Hz)<\/p>\n\n--><\/p>\n<p style=\"text-align:center\">Fig.2 Current distribution obtained by SUFCUR (0.01Hz)<\/p>\n<\/p><\/div>\n<\/div>\n<p><!--more--><\/p>\n<h3>How to use<\/h3>\n<p>Below is an example of a PHICOIL definition where the coil region property number is 2 and the gap element is represented by property number 3. The coil resistance is calculated using the electrical conductivity SIGMA of the coil conductor, which can be entered in PHICOIL.<br \/>\nThe coil resistance is calculated using the electrical conductivity SIGMA of the coil conductor, which can be entered in PHICOIL.  <\/p>\n<ul>\n<li>Coil region definition in Handbook &quot;16.1.1 Property of Volume Element\u201d<\/li>\n<\/ul>\n<p class=\"slideText\">* MAT_ID * POTENTIAL * B_H_CURVE_ID * SIGMA * MU * PACKING *<br \/>\n         2                  0                          0                  0.0        1.0        1.0\n<\/p>\n<ul>\n<li>Gap element definition in Handbook &quot;16.2 Surface Current Sources<\/li>\n<\/ul>\n<p class=\"slideText\">* SMAT_ID * TYPE * SIGMA * MU * IMP_TYPE or THICK *<br \/>\n         3              2          0.0       1.0                     0.0\n<\/p>\n<ul>\n<li>PHICOIL definition in Handbook &quot;17.4 Potential Current Sources<\/li>\n<\/ul>\n<p class=\"slideText\">* PHICOIL * SERIES_NO * NO_PARTS * IN_ROTOR *<br \/>\n   PHICOIL             1                     1                    0<br \/>\n* MAT_ID * SMAT_ID_IN * CURRENT * SIGMA *<br \/>\n         2                   3                  1.0            0.0\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\/phicoil_loop.zip\">Sample data DL<\/a><\/button>  <\/p>\n<p>\u30fb input.PHICOIL<br \/>\n\u30fb input.SUFCUR<br \/>\n\u30fb pre_geom2D.neu \uff1aMesh file<br \/>\n\u30fb 2D_to_3D \uff1a2D mesh extension file  <\/p>\n","protected":false},"excerpt":{"rendered":"<p>Summary EMSolution has a &quot;potential current source (PHICOIL)&quot; expressed by an electric scalar potential. With this feature, coil currents flowing in and out of the Bn=0 surface and currents flowing in and out of periodically symmetric surfaces can be defined. We are pleased to report that PHICOIL can now be used to define coils that [&hellip;]<\/p>\n","protected":false},"featured_media":0,"template":"","tags":[],"case_cat":[2],"class_list":["post-99","case","type-case","status-publish","hentry","case_cat-denjiba"],"acf":[],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/99"}],"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":9,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/99\/revisions"}],"predecessor-version":[{"id":3135,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case\/99\/revisions\/3135"}],"wp:attachment":[{"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/media?parent=99"}],"wp:term":[{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/tags?post=99"},{"taxonomy":"case_cat","embeddable":true,"href":"https:\/\/www.ssil.co.jp\/product\/EMSolution\/en\/wp-json\/wp\/v2\/case_cat?post=99"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}