The DistributedPower kernel computes the kinetic energy contribution of the body force due to total energy in an element. More...
#include <DistributedPower.h>
Public Member Functions | |
DistributedPower (const InputParameters ¶meters) | |
Protected Member Functions | |
virtual Real | computeQpResidual () |
virtual Real | computeQpJacobian () |
virtual Real | computeQpOffDiagJacobian (unsigned int jvar) |
Protected Attributes | |
RealVectorValue | _acceleration |
unsigned int | _rhou_var_number |
unsigned int | _rhov_var_number |
unsigned int | _rhow_var_number |
const VariableValue & | _rho_u |
const VariableValue & | _rho_v |
const VariableValue & | _rho_w |
The DistributedPower kernel computes the kinetic energy contribution of the body force due to total energy in an element.
In this kernel, the acceleration of the body force is assumed to be a constant defined by up to three dimensional components as input. This kinetic energy component is the acceleration vector dotted into the momentum vector components, yielding a scalar kinetic contribution.
Definition at line 26 of file DistributedPower.h.
DistributedPower::DistributedPower | ( | const InputParameters & | parameters | ) |
Definition at line 34 of file DistributedPower.C.
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Definition at line 58 of file DistributedPower.C.
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Definition at line 64 of file DistributedPower.C.
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Definition at line 50 of file DistributedPower.C.
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Definition at line 36 of file DistributedPower.h.
Referenced by computeQpOffDiagJacobian(), and computeQpResidual().
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Definition at line 40 of file DistributedPower.h.
Referenced by computeQpResidual().
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Definition at line 41 of file DistributedPower.h.
Referenced by computeQpResidual().
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Definition at line 42 of file DistributedPower.h.
Referenced by computeQpResidual().
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Definition at line 37 of file DistributedPower.h.
Referenced by computeQpOffDiagJacobian().
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Definition at line 38 of file DistributedPower.h.
Referenced by computeQpOffDiagJacobian().
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Definition at line 39 of file DistributedPower.h.
Referenced by computeQpOffDiagJacobian().