Calculates the normal ( \(\cdot_n\)) or geodesic ( \(\cdot_g\)) components of the plasma perturbation \(\vec{\xi}\) or the magnetic perturbation \(\vec{Q} = \nabla \times \left(\vec{x} \times \vec{B}\right)\). More...
Public Member Functions | |
| integer function | calc_xuq_ind (mds_X, mds_sol, grid_eq, grid_X, grid_sol, eq_1, eq_2, X, sol, X_id, XUQ_style, time, XUQ, deriv) |
| (time) individual version More... | |
| integer function | calc_xuq_arr (mds_X, mds_sol, grid_eq, grid_X, grid_sol, eq_1, eq_2, X, sol, X_id, XUQ_style, time, XUQ, deriv) |
| (time) array version More... | |
Detailed Description
Calculates the normal ( \(\cdot_n\)) or geodesic ( \(\cdot_g\)) components of the plasma perturbation \(\vec{\xi}\) or the magnetic perturbation \(\vec{Q} = \nabla \times \left(\vec{x} \times \vec{B}\right)\).
Which variables are plot depends on XUQ_style [17] :
XUQ_style= 1: \(X\) (supports parallel derivative)XUQ_style= 2: \(U\) (supports parallel derivative)XUQ_style= 3: \(Q_n\)XUQ_style= 4: \(Q_g\)
\(X\) and \(U\) support the calculation of the parallel derivative.
For \(Q_n\) and \(Q_g\), the metric variables have to be provided as well.
The perturbation grid is assumed to have the same angular coordinates as the equilibrium grid, and the normal coordinates correspond to either the equilibrium grid (X_grid_style 1), the solution grid (X_grid_style 2) or the enriched equilibrium grid (X_grid_style 3).
The output grid, furthermore, has the angular part corresponding to the equilibrium grid, and the normal part to the solution grid.
- Returns
- ierr
Definition at line 56 of file sol_utilities.f90.
Member Function/Subroutine Documentation
◆ calc_xuq_arr()
| integer function sol_utilities::calc_xuq::calc_xuq_arr | ( | type(modes_type), intent(in), target | mds_X, |
| type(modes_type), intent(in), target | mds_sol, | ||
| type(grid_type), intent(in) | grid_eq, | ||
| type(grid_type), intent(in) | grid_X, | ||
| type(grid_type), intent(in) | grid_sol, | ||
| type(eq_1_type), intent(in) | eq_1, | ||
| type(eq_2_type), intent(in) | eq_2, | ||
| type(x_1_type), intent(in), target | X, | ||
| type(sol_type), intent(in) | sol, | ||
| integer, intent(in) | X_id, | ||
| integer, intent(in) | XUQ_style, | ||
| real(dp), dimension(:), intent(in) | time, | ||
| complex(dp), dimension(:,:,:,:), intent(inout) | XUQ, | ||
| logical, intent(in), optional | deriv | ||
| ) |
(time) array version
- Parameters
-
[in] mds_x general modes variables in perturbation grid [in] mds_sol general modes variables in solution grid [in] grid_eq equilibrium grid [in] grid_x perturbation grid [in] grid_sol solution grid [in] eq_1 flux equilibrium [in] eq_2 metric equilibrium [in] x perturbation variables [in] sol solution variables [in] x_id nr. of Eigenvalue [in] xuq_style whether to calculate \(X\), \(U\), \(Q_n\) or \(Q_g\) [in] time time range [in,out] xuq \(X\), \(U\), \(Q_n\) or \(Q_g\) [in] deriv return parallel derivative
Definition at line 67 of file sol_utilities.f90.
Here is the call graph for this function:◆ calc_xuq_ind()
| integer function sol_utilities::calc_xuq::calc_xuq_ind | ( | type(modes_type), intent(in) | mds_X, |
| type(modes_type), intent(in) | mds_sol, | ||
| type(grid_type), intent(in) | grid_eq, | ||
| type(grid_type), intent(in) | grid_X, | ||
| type(grid_type), intent(in) | grid_sol, | ||
| type(eq_1_type), intent(in) | eq_1, | ||
| type(eq_2_type), intent(in) | eq_2, | ||
| type(x_1_type), intent(in) | X, | ||
| type(sol_type), intent(in) | sol, | ||
| integer, intent(in) | X_id, | ||
| integer, intent(in) | XUQ_style, | ||
| real(dp), intent(in) | time, | ||
| complex(dp), dimension(:,:,:), intent(inout) | XUQ, | ||
| logical, intent(in), optional | deriv | ||
| ) |
(time) individual version
- Parameters
-
[in] mds_x general modes variables in perturbation grid [in] mds_sol general modes variables in solution grid [in] grid_eq equilibrium grid [in] grid_x perturbation grid [in] grid_sol solution grid [in] eq_1 flux equilibrium [in] eq_2 metric equilibrium [in] x perturbation variables [in] sol solution variables [in] x_id nr. of Eigenvalue [in] xuq_style whether to calculate X, U, Qn or Qg [in,out] xuq normal component of perturbation [in] deriv return parallel derivative
Definition at line 520 of file sol_utilities.f90.
The documentation for this interface was generated from the following file:
- /opt/PB3D/Modules/sol_utilities.f90