XGC-221: series of single particle simulations

Several single particle simulation has been run with different time step. The energy is preserved within 2% in the simulation for 200 ion transient times only when the time step is about 1e-3 of ion transient time (sml_dt=1.d-3). Figures below show energy as function of time

sml_dt=0.02

sml_dt=0.005

sml_dt=0.002

sml_dt=0.001

In these single particle simulations, the computation time with the FMCFM interface (fm_use=1)

real    20m15.682s
user    19m57.207s
sys     0m6.028s

is compared with the corresponding simulation without the FMCFM interface (fm_use=0)

real    2m0.557s
user    1m55.979s
sys     0m3.632s


Case XGC-223: test for new radiation and new sheath potential models

Updated version of the XGC-0 code that includes recent additions from Gunyoung Park is used for this simulation. The new version of XGC- inludes:

  1. New simple radiation model is based on ADPAK radiation data. The model assumes constant impurity density in the region where radiation cooling is applied;
  2. Improved sheath potential model;
  3. Diffusivities in the SOL region is set by tbl_ parameters rather than FMCFM models.

The electron temperature is slightly lower in the SOL region comparing to the electron temperature in the case XGC-222.


Case XGC-222: Use of MMM95 modules is delayed by 1000 time steps

In order to give time for the radial electric field to develop, the use of MMM95 module through the FMCFM interface is delayed by 1000 time steps. Particle and thermal diffusivities from tbl namelist were used during the first 1000 time steps.

There are relatively small changes for the plasma density profile; electron temperature profile looks more realist.

Overall summary: There is insufficient flow shear stabilization for the particle transport in the inner pedestal region. The next thing to try is the updated sheath potential and radiation models provided by Gunyoung Park.