From 0e2b97d637233efd31ac33af568bfc7d6b8377f0 Mon Sep 17 00:00:00 2001
From: Ruth Sabariego <ruth.sabariego@kuleuven.be>
Date: Mon, 25 Jun 2018 11:09:27 +0200
Subject: [PATCH] Update electromagnet.pro
---
Magnetodynamics/electromagnet.pro | 10 ++++++----
1 file changed, 6 insertions(+), 4 deletions(-)
diff --git a/Magnetodynamics/electromagnet.pro b/Magnetodynamics/electromagnet.pro
index b5e7138..a381e59 100644
--- a/Magnetodynamics/electromagnet.pro
+++ b/Magnetodynamics/electromagnet.pro
@@ -14,6 +14,8 @@
To compute the solution interactively from the Gmsh GUI:
File > Open > electromagnet.pro
+ You may choose the Resolution in the left panel:
+ Magnetodynamics2D_av (default) or Magnetostatics2D_a
Run (button at the bottom of the left panel)
------------------------------------------------------------------- */
@@ -32,8 +34,8 @@ Group {
Vol_Mag = Region[{Air, Core, Ind, AirInf}]; // full magnetic domain
Vol_C_Mag = Region[Core]; // massive conductors
Vol_S_Mag = Region[Ind]; // stranded conductors (coils)
- Vol_Inf_Mag = Region[AirInf]; // annulus for infinite shell transformation
- Val_Rint = rInt; Val_Rext = rExt; // interior and exterior radii of annulus
+ Vol_Inf_Mag = Region[AirInf]; // ring-shaped shell for infinite transformation
+ Val_Rint = rInt; Val_Rext = rExt; // interior and exterior radii of ring
}
Function {
@@ -50,7 +52,7 @@ Function {
sigma[ Ind ] = 5e7;
Ns[ Ind ] = 1000 ; // number of turns in coil
- Sc[ Ind ] = SurfaceArea[] ; // surface (cross section) of coil
+ Sc[ Ind ] = SurfaceArea[] ; // area of coil cross section
// Current density in each coil portion for a unit current (will be multiplied
// by the actual total current in the coil)
js0[ Ind ] = Ns[]/Sc[] * Vector[0,0,-1];
@@ -66,7 +68,7 @@ Constraint {
}
{ Name Current_2D;
Case {
- // represents the phasor amplitude for a dynamic analysis
+ // represents the phasor amplitude (peak to peak value) for a dynamic analysis
{ Region Ind; Value Current; }
}
}
--
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