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Weak Form Modeling and Multiphysics Coupling in RF Module
Posted 2013年4月15日 GMT-4 15:21 RF & Microwave Engineering, Modeling Tools & Definitions, Parameters, Variables, & Functions Version 4.3 11 Replies
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I have some problems when using user-defined weak form PDEs and multiphysics coupling for 3D nano particles scattering in the RF module. Please find the attachment for the detailed information. Any comments would be highly appreciated. Thanks in advance.
Cordially,
Tony
Attachments:
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As for your first question, I think the whole matrix equation system solved at last comes from both weak forms of Maxwell's equation and boundary conditions. As you may have noted the original weak form of Maxwell's equation corresponds to the one with negative sign, so if the one without negative sign is used, it's not consistent with the weak form of boundary conditions. I'm not sure, but this could be the reason.
The second one, you said the problem doesn't appear for 2D case, but I don't know how you introduce the coupling for 2D case. I suppose 3D case is the same.
Best
--
Pu, ZHANG ??
Departamento de Física Teórica de la Materia Condensada,
Universidad Autónoma de Madrid,
Madrid, Spain.
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Cordially,
Tony
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--
Pu, ZHANG ??
Departamento de Física Teórica de la Materia Condensada,
Universidad Autónoma de Madrid,
Madrid, Spain.
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beta^2*Jh1x+Jh2y)*test(Jh1x)-(omega0^2-1i*omega0*gamma)*Jh1*test(Jh1)-1i*omega0*epsilon0_const*omegap^2*emw.Ex*test(Jh1)
beta^2*Jh1x+Jh2y)*test(Jh2y)-(omega0^2-1i*omega0*gamma)*Jh2*test(Jh2)-1i*omega0*epsilon0_const*omegap^2*emw.Ey*test(Jh2)
and the boundary condition reduces to
nx*Jh1+ny*Jh2=0
And, for the Electric field, the user-defined weak form reduces to
-emw.curlEz*test(curlEz)+epsinf*emw.k0)^2*emw.Ex*test(emw.relEx)+emw.Ey*test(emw.relEy))-emw.iomega*mu0_const*(Jh1*test(emw.relEx)+Jh2*test(emw.relEy))
It works good for me.
Cordially,
Tony
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Cordially,
Tony
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