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ImplicitSolveOperator.cpp
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Tue, Oct 8, 01:50
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rLAMMPS lammps
ImplicitSolveOperator.cpp
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// Header file for this class
#include "ImplicitSolveOperator.h"
// Other ATC includes
#include "ATC_Transfer.h"
#include "FE_Engine.h"
#include "PhysicsModel.h"
#include "PrescribedDataManager.h"
namespace
ATC
{
// --------------------------------------------------------------------
// --------------------------------------------------------------------
// ImplicitSolveOperator
// --------------------------------------------------------------------
// --------------------------------------------------------------------
ImplicitSolveOperator
::
ImplicitSolveOperator
(
ATC_Transfer
*
atcTransfer
,
/*const*/
FE_Engine
*
feEngine
,
const
PhysicsModel
*
physicsModel
)
:
atcTransfer_
(
atcTransfer
),
feEngine_
(
feEngine
),
physicsModel_
(
physicsModel
)
{
// Nothing else to do here
}
// --------------------------------------------------------------------
// --------------------------------------------------------------------
// FieldImplicitSolveOperator
// --------------------------------------------------------------------
// --------------------------------------------------------------------
FieldImplicitSolveOperator
::
FieldImplicitSolveOperator
(
ATC_Transfer
*
atcTransfer
,
/*const*/
FE_Engine
*
feEngine
,
FIELDS
&
fields
,
const
FieldName
fieldName
,
const
Array2D
<
bool
>
&
rhsMask
,
const
PhysicsModel
*
physicsModel
,
double
simTime
,
double
dt
,
double
alpha
)
:
ImplicitSolveOperator
(
atcTransfer
,
feEngine
,
physicsModel
),
fields_
(
fields
),
// ref to fields
fieldName_
(
fieldName
),
simTime_
(
simTime
),
dt_
(
dt
),
alpha_
(
alpha
),
epsilon0_
(
1.0e-8
)
{
// find field associated with ODE
rhsMask_
.
reset
(
NUM_FIELDS
,
NUM_FLUX
);
rhsMask_
=
false
;
for
(
int
i
=
0
;
i
<
rhsMask
.
nCols
();
i
++
)
{
rhsMask_
(
fieldName_
,
i
)
=
rhsMask
(
fieldName_
,
i
);
}
massMask_
.
reset
(
1
);
massMask_
(
0
)
=
fieldName_
;
// Save off current field
TnVect_
=
column
(
fields_
[
fieldName_
],
0
);
// NOTE assuming 1 dof ?
// Allocate vectors for fields and rhs
int
nNodes
=
atcTransfer_
->
get_nNodes
();
// copy fields
fieldsNp1_
=
fields_
;
// size rhs
int
dof
=
fields_
[
fieldName_
].
nCols
();
RnMap_
[
fieldName_
].
reset
(
nNodes
,
dof
);
RnpMap_
[
fieldName_
].
reset
(
nNodes
,
dof
);
// Compute the RHS vector R(T^n)
// Set BCs on Rn, multiply by inverse mass and then extract its vector
atcTransfer_
->
compute_rhs_vector
(
rhsMask_
,
fields_
,
RnMap_
,
atcTransfer_
->
FULL_DOMAIN
,
physicsModel_
);
DENS_MAT
&
Rn
=
RnMap_
[
fieldName_
];
atcTransfer_
->
get_prescribed_data_manager
()
->
set_fixed_dfield
(
simTime_
,
fieldName_
,
Rn
);
atcTransfer_
->
apply_inverse_mass_matrix
(
Rn
,
fieldName_
);
RnVect_
=
column
(
Rn
,
0
);
}
// --------------------------------------------------------------------
// operator *(Vector)
// --------------------------------------------------------------------
DENS_VEC
FieldImplicitSolveOperator
::
operator
*
(
DENS_VEC
x
)
const
{
// This method uses a matrix-free approach to approximate the
// multiplication by matrix A in the matrix equation Ax=b, where the
// matrix equation results from an implicit treatment of the
// fast field solve for the Two Temperature Model. In
// brief, if the ODE for the fast field can be written:
//
// dT/dt = R(T)
//
// A generalized discretization can be written:
//
// 1/dt * (T^n+1 - T^n) = alpha * R(T^n+1) + (1-alpha) * R(T^n)
//
// Taylor expanding the R(T^n+1) term and rearranging gives the
// equation to be solved for dT at each timestep:
//
// [1 - dt * alpha * dR/dT] * dT = dt * R(T^n)
//
// The operator defined in this method computes the left-hand side,
// given a vector dT. It uses a finite difference, matrix-free
// approximation of dR/dT * dT, giving:
//
// [1 - dt * alpha * dR/dT] * dT = dt * R(T^n)
// ~= dT - dt*alpha/epsilon * ( R(T^n + epsilon*dT) - R(T^n) )
//
// Compute epsilon
double
epsilon
=
(
x
.
norm
()
>
0.0
)
?
epsilon0_
*
TnVect_
.
norm
()
/
x
.
norm
()
:
epsilon0_
;
// Compute incremented vector = T + epsilon*dT
fieldsNp1_
[
fieldName_
]
=
TnVect_
+
epsilon
*
x
;
// Evaluate R(b)
atcTransfer_
->
compute_rhs_vector
(
rhsMask_
,
fieldsNp1_
,
RnpMap_
,
atcTransfer_
->
FULL_DOMAIN
,
physicsModel_
);
DENS_MAT
&
Rnp
=
RnpMap_
[
fieldName_
];
atcTransfer_
->
get_prescribed_data_manager
()
->
set_fixed_dfield
(
simTime_
,
fieldName_
,
Rnp
);
atcTransfer_
->
apply_inverse_mass_matrix
(
Rnp
,
fieldName_
);
RnpVect_
=
column
(
Rnp
,
0
);
// Compute full left hand side and return it
DENS_VEC
Ax
=
x
-
dt_
*
alpha_
/
epsilon
*
(
RnpVect_
-
RnVect_
);
return
Ax
;
}
// --------------------------------------------------------------------
// get_rhs
// --------------------------------------------------------------------
DENS_VEC
FieldImplicitSolveOperator
::
get_rhs
()
{
// Return dt * R(T^n)
return
dt_
*
RnVect_
;
}
// --------------------------------------------------------------------
// get_preconditioner
// --------------------------------------------------------------------
DIAG_MAT
FieldImplicitSolveOperator
::
get_preconditioner
(
FIELDS
&
fields
)
{
// Just create and return identity matrix
int
nNodes
=
atcTransfer_
->
get_nNodes
();
DENS_VEC
ones
(
nNodes
);
ones
=
1.0
;
DIAG_MAT
identity
(
ones
);
return
identity
;
}
}
// namespace ATC
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