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Pellet Ablation in Tokamak Refueling Process The purpose of this research is to develop novel mathematical models, numerical algorithms based on explicit tracking of interfaces, and computational software, and to perform large scale numerical simulations of complex physics processes associated with the injection of frozen deuterium-tritium fuel pellets in tokamaks. This research is being performed in collaboration with General Atomics and Princeton Plasma Physics Laboratory (PPPL).
We have developed a 2D axisymmetric model for the pellet ablation in
tokamaks based on the front tracking MHD code [1]. Since the method of front
tracking allows the study of multiphysics phenomena in multiphase systems
characterized by strong discontinuities in physical properties of the system
components, it is ideally suitable to the pellet ablation problem. In our
computational model, explicit interfaces separate the solid pellet from the
ablated gas, and the cold, dense, and weakly ionized ablation cloud from the
highly conducting fusion plasma. Realistic equations of state are employed
in different geometrical regions corresponding to different states of
matter. The code is capable of simulating the transition of deuterium in the
pellet from solid to liquid state under high ablation pressures. A surface
ablation model is used for on pellet surface. An electronic heat flux model
for the calculation of the thermal energy deposition in the ablation cloud
and on the pellet surface uses approximate analytical solutions of kinetic
equations. Atomic physics processes in the ablation cloud such as
dissociation, recombination, and ionization are taken into account by a
plasma equation of state. Using the developed model, we have performed
studies of the pellet ablation physics, pellet ablation rate and the
lifetime in the magnetic field, and compared with analytical predictions and
previous numerical simulations. The 1D version of the model is in excellent
agreement with the scaling laws and ablation rate predicted by the
theoretical neutral gas shielding model. The 2D axisymmetric simulations
agree with previously published numerical results. Our work goes beyond
these studies and calculates properties of the ablation channel in magnetic
fields and the reduction of the ablation rate. We showed that a common expectation of the nuclear fusion community
regarding the role of the anisotropic heating and magnetic field on the
pellet ablation rate was incorrect. The study of striation instabilities,
impossible without resolving the detailed physics in the ablation cloud,
will be the focus of our future research. These instabilities are not well
understood and have a significant impact on the pellet-plasma interaction
that will occur in the fueling of burning plasmas in ITER. In the future, we
will work with PPPL scientists on the coupling of the M3D code with
FronTier-MHD as a subgrid model for detailed pellet ablation physics, and
performing simulations on the BlueGene. Reference
Last Modified: April 23, 2009 |