Dear David,


I tried what you suggested and I have the following error when solving the Laplace equation:

ufl.log.UFLException: Integral of type cell cannot contain a ReferenceNormal.


I defined:
V_d = FunctionSpace(mesh, "CG", 1)  

V_p = FunctionSpace(mesh, "CG", 1)  

W = V_d*V_p


trial_d, trial_p = TrialFunction(W)

v_d, v_p = TestFunction(W)


result_mixed = Function(W)

u_d, u_p = split(result_mixed)


I define the normal pointing outward the disk interface as:

n_vec = FacetNormal(mesh)

n_int = I_d("+") * n_vec("+") + I_d("-") * n_vec("-")


where I_d (and I_p) are the discontinuous (DG0) indicators defined as in Tomasz code. Then I define my weak forms as follows:

A_u_d = sigma_d*dot(grad(trial_d),grad(v_d))*avg(I_d)*dx # Laplace in V_d

A_u_p = sigma_p*dot(grad(trial_p),grad(v_p))*avg(I_p)*dx # Laplace in V_p


L_u_d = sigma_d*v_d*dot(grad(tmp_d),n_int)*4*avg(I_d)*avg(I_p)*dx # interface 

L_u_p = -sigma_p*v_p*E*ds(domaine_bc_r) -   sigma_p*v_p*dot(grad(tmp_p),n_int)*4*avg(I_d)*avg(I_p)*dx  # right BC and interface 


A_u = A_u_d + A_u_p

L_u = L_u_d + L_u_p


cell_pb = LinearVariationalProblem(A_u, L_u, result_mixed)

cell_solver = LinearVariationalSolver(cell_pb)


cell_solver.solve()


The full error is pasted below. Do you know where it comes from ?
Thank you,
Floriane

UFL:ERROR Integral of type cell cannot contain a ReferenceNormal.

Traceback (most recent call last):

  File "lin_cell.py", line 196, in <module>

    cell_solver = LinearVariationalSolver(cell_pb)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/variational_solver.py", line 286, in __init__

    super(LinearVariationalSolver, self).__init__(*args, **kwargs)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/variational_solver.py", line 156, in __init__

    pre_function_callback=pre_f_callback)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/solving_utils.py", line 333, in __init__

    form_compiler_parameters=fcp)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/assemble.py", line 143, in create_assembly_callable

    collect_loops=True)

  File "<decorator-gen-280>", line 2, in _assemble

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/utils.py", line 62, in wrapper

    return f(*args, **kwargs)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/assemble.py", line 192, in _assemble

    kernels = tsfc_interface.compile_form(f, "form", parameters=form_compiler_parameters, inverse=inverse)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/tsfc_interface.py", line 193, in compile_form

    number_map).kernels

  File "/Users/mmfg/firedrake/src/PyOP2/pyop2/caching.py", line 200, in __new__

    obj = make_obj()

  File "/Users/mmfg/firedrake/src/PyOP2/pyop2/caching.py", line 190, in make_obj

    obj.__init__(*args, **kwargs)

  File "/Users/mmfg/firedrake/src/firedrake/firedrake/tsfc_interface.py", line 112, in __init__

    tree = tsfc_compile_form(form, prefix=name, parameters=parameters)

  File "/Users/mmfg/firedrake/src/tsfc/tsfc/driver.py", line 46, in compile_form

    fd = ufl_utils.compute_form_data(form)

  File "/Users/mmfg/firedrake/src/tsfc/tsfc/ufl_utils.py", line 56, in compute_form_data

    do_estimate_degrees=do_estimate_degrees,

  File "/Users/mmfg/firedrake/src/ufl/ufl/algorithms/compute_form_data.py", line 382, in compute_form_data

    _check_facet_geometry(self.integral_data)

  File "/Users/mmfg/firedrake/src/ufl/ufl/algorithms/compute_form_data.py", line 168, in _check_facet_geometry

    error("Integral of type %s cannot contain a %s." % (it, cls.__name__))

  File "/Users/mmfg/firedrake/src/ufl/ufl/log.py", line 172, in error

    raise self._exception_type(self._format_raw(*message))

ufl.log.UFLException: Integral of type cell cannot contain a ReferenceNormal.



De : firedrake-bounces@imperial.ac.uk <firedrake-bounces@imperial.ac.uk> de la part de Ham, David A <david.ham@imperial.ac.uk>
Envoyé : vendredi 5 octobre 2018 15:56
À : firedrake
Objet : Re: [firedrake] local discontinuity
 

Dear Floriane,

 

I think you can do this in a manner analogous to the way that Thomasz did fluid-structure interaction.

 

We define a mixed function space with two continuous components: (V_d, V_p). We’re going to use the first component for the solution in the disk and the second component for the solution outside the disk.

 

We further define two DG0 functions I_d and I_p such that I_d is 1 inside the disk and 0 outside, and I_p = 1 – I_d.

 

You can now write the Laplace equation for the two parts using essentially normal Firedrake code except that you multiply the test function by the appropriate indicator function. This ensures that you only actually assemble integral contributions on the correct part of the domain.

 

Now we just need the surface integral over the facets on the edge of the disk. Observe that this is the only place in the domain where both indicator functions are positive. You can write your jump integrals using the  *dS measure. You can restrict the intervals to the relevant edges by multiplying the integrand by 4*avg(I_p)*avg(I_d).

 

If

W = V_d * V_p

and

u_d, u_p = TrialFunctions(W)

 

then you can write the jump as:

 

avg(u_d) – avg(u_p)

 

The avg is mathematically unnecessary and does nothing, however in UFL all terminals that appear in dS integrals have to be restricted (you could just as well write u_d(‘+’) – u_p(‘+’)).

 

Finally, when you come to the solve, you need to ensure that all the V_d nodes outside the disk are eliminated, and all the V_p nodes inside the disk too. You do this using the same DirichletBC subclassing trick which is in https://www.firedrakeproject.org/demos/linear_fluid_structure_interaction.py.html


 

I realise that is slightly involved, but it should work and the syntax will be fairly clean once you have done it. Feel free to ask for clarifications.

 

Regards,

 

David

 

 

From: <firedrake-bounces@imperial.ac.uk> on behalf of "Floriane Gidel [RPG]" <mmfg@leeds.ac.uk>
Reply-To: firedrake <firedrake@imperial.ac.uk>
Date: Friday, 5 October 2018 at 15:33
To: firedrake <firedrake@imperial.ac.uk>
Subject: [firedrake] local discontinuity

 

Dear Firedrakers,

 

I would like to solve equations in a domain made of two subdomains:

- a disk, inside which test functions are continuous (Omega_d)

- a plane around the disk, in which test functions are continuous (Omega_p)

However, I would like the test functions to be discontinuous across the interface Gamma between the disk and the surrounding plane.

This is to solve Laplace equation in each domain, augmented by a dynamic boundary condition on the jump between the two domains, that is

Delta u = 0 in Omega_d

Delta u = 0 in Omega_p

partial_t [u] = ...   on Gamma, where [u]= u(+)-u(-) is the jump

 

Is there a way to define a functionspace on the full mesh, with continuous basis functions in each subdomain but discontinuous across the interface ? Or is there any better way to solve this kind of system ?

 

Thank you for your help,

 

Floriane