NUMERICAL MODELING AND EXPERIMENTAL SIMULATION OF VAPOR SHIELD FORMATION AND DIVERTOR MATERIAL EROSION FOR ITER TYPICAL PLASMA DISRUPTIONS

Citation
H. Wurz et al., NUMERICAL MODELING AND EXPERIMENTAL SIMULATION OF VAPOR SHIELD FORMATION AND DIVERTOR MATERIAL EROSION FOR ITER TYPICAL PLASMA DISRUPTIONS, Journal of nuclear materials, 215, 1994, pp. 1349-1352
Citations number
7
Categorie Soggetti
Nuclear Sciences & Tecnology","Metallurgy & Mining","Material Science
ISSN journal
00223115
Volume
215
Year of publication
1994
Part
B
Pages
1349 - 1352
Database
ISI
SICI code
0022-3115(1994)215:<1349:NMAESO>2.0.ZU;2-A
Abstract
The high divertor heat load during a tokamak plasma disruption results in sudden evaporation of a thin layer of divertor plate material, whi ch acts as vapor shield and protects the target from further excessive evaporation. Formation and effectiveness of the vapor shield are theo retically modeled and experimentally investigated at the 2MK-200 facil ity under conditions simulating the thermal quench phase of ITER tokam ak plasma disruptions. In the optical wavelength range C II, C III, C IV emission lines for graphite, Cu I, Cu II lines for copper and conti nuum radiation for tungsten samples are observed in the target plasma. The plasma expands along the magnetic field lines with velocities of (4 +/- 1) X 10(6) cm/s for graphite and 10(5) cm/s for copper. Modelin g was done with a radiation hydrodynamics code in one-dimensional plan ar geometry. The multifrequency radiation transport is treated in flux limited diffusion and in forward reverse transport approximation. In these first modeling studies the overall shielding efficiency for carb on and tungsten defined as ratio of the incident energy and the vapori zation energy for power densities of 10 MW/cm(2) exceeds a factor of 3 0. The vapor shield is established within 2 mu s, the power fraction t o the target after 10 mu s is below 3% and reaches in the stationary s tate after about 20 mu s a value of around 1.5%.