Dimension independent Maxwell`s equations

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Konstantin Ladutenko

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Dec 26, 2016, 7:00:22 AM12/26/16
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Dear all,

Any ideas, what is the best way to go when implementing Maxwell equations to make them dimension independent? Or at least to have the same code for 2d and 3d cases?

Simply using dim template parameter doesn`t work by definition - when switching from 3D to 2D  you need to specify, should it be TE or TM mode (which field, electric of magnetic, should be normal to the 2D plane). Introducing some boolean variable  `isTEmode` to be True or False can help, but this will lead to many if\then codes... As soon as it is still the same Maxwell equation I hope there is a better way to do this. Any ideas?

From the code point of view it does not work either at the moment. Using

     fe (FE_RaviartThomas<dim> (degree), 1, FE_Nedelec<dim> (degree), 1),

where Raviart-Thomas face element is needed for magnetic field, Nedelec edge element is needed for electric field and

    const FEValuesExtractors::Vector B_field (0);
    const FEValuesExtractors::Vector E_field (dim);
    const auto &curl_W_j = fe_values[E_field].curl  (j, q);
    const auto &F_i      = fe_values[B_field].value (i, q);

works fine for 3D (some wave is traveling in free space) and breaks down in 2D during compilation of a weak-form integral local component.

/home/tig/symlink/dealii/examples/step-maxwell-nonliner/step-maxwell-linear.cc: In instantiation of ‘void Maxwell::MaxwellTD<dim>::assemble_system() [with int dim = 2]’:
/home/tig/symlink/dealii/examples/step-maxwell-nonliner/step-maxwell-linear.cc:549:20:   required from ‘void Maxwell::MaxwellTD<dim>::run() [with int dim = 2]’
/home/tig/symlink/dealii/examples/step-maxwell-nonliner/step-maxwell-linear.cc:648:32:   required from here
/home/tig/symlink/dealii/examples/step-maxwell-nonliner/step-maxwell-linear.cc:394:51: error: no match for ‘operator*’ (operand types are ‘const dealii::Tensor<1, 1, double>’ and ‘const dealii::Tensor<1, 2, double>’)
                   local_rhs_KT (i, j) += curl_W_j * F_i * fe_values.JxW (q)

Full example is available online at GitHub


Best regards,
Konstantin Ladutenko



Timo Heister

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Dec 26, 2016, 3:44:49 PM12/26/16
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The problem is that .curl returns a scalar in 2d and a tensor in 3d. A
typical definition of maxwell curl notation is to treat the 2d case as
a 3d solution that is constant in the (implicit) 3rd dimension, right?
Maybe you can do something like

Tensor<1,3> make_3d_curl(double curl_2d)
{
Tensor<1,3> r; r[2] = curl_2d; return r;
}

Tensor<1,3> make_3d_curl(Tensor<1,3> curl_3d)
{
return curl_3d;
}

and then do all the math in 3d:

Tensor<1,dim> curl_W_j = make_3d_curl(fe_values[E_field].curl (j, q));

local_rhs_KT (i, j) += curl_W_j * ...

etc.
> https://urldefense.proofpoint.com/v2/url?u=https-3A__github.com_kostyfisik_dealii_blob_0188064ee4dd0cdd53d515f33932732b0a2d5d66_examples_step-2Dmaxwell-2Dnonliner_step-2Dmaxwell-2Dlinear.cc&d=CwIFaQ&c=Ngd-ta5yRYsqeUsEDgxhcqsYYY1Xs5ogLxWPA_2Wlc4&r=4k7iKXbjGC8LfYxVJJXiaYVu6FRWmEjX38S7JmlS9Vw&m=DjvKZYOEy46NTfpFc92OVXJsfNl6mHgZuzQYoA80LvQ&s=3pcGss3gRopgWpsIOGUaJCr3t5KJooO1atsssf2KC4w&e=
>
> Best regards,
> Konstantin Ladutenko
>
>
>
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--
Timo Heister
http://www.math.clemson.edu/~heister/

Konstantin Ladutenko

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Dec 30, 2016, 9:31:45 AM12/30/16
to deal.II User Group
Thank you a lot! I`ve tried to play around and my conclusion is trivial and exactly what you have said - we do really need to solve a full 3d equation for 2D geometry too, it comes from physics, not from coding or math. Just imagine a typical 1D (or 2D) problem - an infinite subwavelength plate made from uniaxial crystal, with a wave passing it at normal incidence. Such a 1D setup (geometrically) we need all field components to describe a phenomenon, an extraordinary ray for sure will move away form initial 1D line and in general will move  out of 2D plane of consideration.

I am still a bit confused. E.g. to simulate  Fresnel equation in 1D should I need to consider a 1D stack of hexahedral? I do actually need only 2 components for field out of six (one normal for electric field, and one normal for magnetic for 1D case). However, to keep compatibility with 3D case I need to evaluate all six components, so it will be easy to move to a 2D as a plane of hexahedra or to a 3d case with a volume.  Probably I should simply put a constraint for components that I am sure are not needed to be equal zero. This way the number of DoF per element should be reduced...




понедельник, 26 декабря 2016 г., 23:44:49 UTC+3 пользователь Timo Heister написал:
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