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field_divB0.inp
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1 ipert ! 0=eq only, 1=vac, 2,3=vac+plas
1 iequil ! 0=pert. alone, 1=with equil.
0.00 ampl ! amplitude of perturbation, a.u.
81 ntor ! number of toroidal harmonics
0.99 cutoff ! inner cutoff in psi/psi_a units
4 icftype ! type of coil file
'../FIELD/17151.3800.AUGD.EQI.00.efit' gfile ! equilibrium file
'./DATA_ASDEX_MESH3D_30835/field.dat' pfile ! coil file
'../FIELD/convexwall.asdex' convexfile ! convex file for stretchcoords
'FROMQQ/FLUXDATA' fluxdatapath ! directory with data in flux coord.(not used now, 12.07.16)
0 nwindow_r ! window size for filtering of psi array over R
0 nwindow_z ! window size for filtering of psi array over Z
More detailed comments on switches.
Axisymmetric equilibrium is called in all cases. If some routines are not
called, their data is not required.
Perturbation switch "ipert":
0 - axisymmetric equilibrium is called alone (can be run withot coild data
and resonance plasma response data)
1 - cylindrical routine is called in addition to equilibrium (plasma response
data is not required
2 - both, cylindrical and flux coordinate routine modelling plasma response
are called, all data is required. Derivatives are not computed
3 - the same as 2 with computation of derivatives (7 times slower)
Equilibrium switch "iequil":
0 - equilibrium field is not added to the output (needed for computing the
perturbation field alone). The equilibrium routine is called - its
data is needed for plasma response field. For future: this call can be
disabled for stellarator modelling.
1 - normal mode, perturbation is added to the output field