Note: This discussion is about an older version of the COMSOL Multiphysics® software. The information provided may be out of date.
Discussion Closed This discussion was created more than 6 months ago and has been closed. To start a new discussion with a link back to this one, click here.
Superconducting wire
Posted 05.06.2012, 08:32 GMT-4 Low-Frequency Electromagnetics, Studies & Solvers Version 4.2a 7 Replies
Please login with a confirmed email address before reporting spam
Hi,
I was trying to model a tape of superconducting material; its conductivity is dependent on the current going through it.
This creates circular variable dependency, and thus cannot be modeled as easily as I'd like. In the knowledge database there is a model that sort-of deals with that problem:
www.comsol.com/showroom/gallery/689/
Model 689.
In this model, the PDE is solved for the H-field instead of going around with the conductivity.
I have tried to create this model in three dimensions, and I think I succeeded in copying; but I have a few questions about that, and a problem I will add later.
my questions:
1.
How did the equation described in the .PDF file related to the file become in the form of the General Form PDE? where did the Curl go and why is there a div(GAMMA) there?
2.
why is GAMMA defined as it is? if I change one of the values there so that they're both positive/negative, the solution doesn't converge. however if I switch both signs, the solution doesn't change. and in 3D, the third part of gamma doesn't seem to matter at all; if it is 0,0,Ez_sc it's the same as 0,0,234234234.
And now the problem:
I want to have this model eventually coupled with another physics - since I want to add a time dependent magnetic field on the tape. How will I be able to tell the program to do that? to treat my domain with properties that are defined via the PDEs?
I know I'm asking a lot,
Thank you very much for your time,
Shoval
I was trying to model a tape of superconducting material; its conductivity is dependent on the current going through it.
This creates circular variable dependency, and thus cannot be modeled as easily as I'd like. In the knowledge database there is a model that sort-of deals with that problem:
www.comsol.com/showroom/gallery/689/
Model 689.
In this model, the PDE is solved for the H-field instead of going around with the conductivity.
I have tried to create this model in three dimensions, and I think I succeeded in copying; but I have a few questions about that, and a problem I will add later.
my questions:
1.
How did the equation described in the .PDF file related to the file become in the form of the General Form PDE? where did the Curl go and why is there a div(GAMMA) there?
2.
why is GAMMA defined as it is? if I change one of the values there so that they're both positive/negative, the solution doesn't converge. however if I switch both signs, the solution doesn't change. and in 3D, the third part of gamma doesn't seem to matter at all; if it is 0,0,Ez_sc it's the same as 0,0,234234234.
And now the problem:
I want to have this model eventually coupled with another physics - since I want to add a time dependent magnetic field on the tape. How will I be able to tell the program to do that? to treat my domain with properties that are defined via the PDEs?
I know I'm asking a lot,
Thank you very much for your time,
Shoval
7 Replies Last Post 11.06.2012, 10:50 GMT-4