HYDROGEN PELLET ABLATION AND ACCELERATION BY CURRENT IN HIGH-TEMPERATURE PLASMAS

被引:52
作者
KUTEEV, BV
机构
关键词
D O I
10.1088/0029-5515/35/4/I05
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Hydrogen pellet ablation and acceleration by current in high temperature plasmas are analysed. The present state of ablation theory and experiment is discussed and an ablation model is formulated. This model takes into account the energy distribution of the particles (both electrons and ions) participating in the ablation process, electrostatic effects of the cloud charging and changes of the pellet form during ablation. Without charging the pellet form tends to a shape resembling a lentil while it remains almost spherical if charged. A new algorithm for ablation rate calculations that can be used for an arbitrary initial form of the pellet is described. The results of this kinetic two dimensional approach differ from those of the Parks ablation scaling used in the ITER design by not more than 30%. Plasma shielding effects are not significant in the ablation if strong turbulence in the cloud is taken into account. Acceleration analysis is based on the Braginskii corrected electron distribution function. For the lentil mode of ablation, acceleration is higher than those for the charged mode by a factor of 1.76. The ablation models are compared with the experiments on T-IO, JET, TFTR, Heliotron-E and Tore Supra. A sensitivity analysis shows that pellet size and electron temperature are the most significant factors for determination of the penetration length. The available database of penetration lengths is not sufficient for distinguishing between the models. Acceleration for the charged mode correlates with experimental data better than that for the lentil mode. The effect of the hot ions is seen on the ablation. Finally, ablation at reactor relevant plasma and pellet parameters is considered. This range of the plasma parameters needs a correction of the ablation scaling as follows: dN/dt similar to n(e)(0.453)T(e)(1.72)r(p)(1.443)M(i)(-0.283), where n(e) and T-e are the electron density and temperature, respectively, and r(p) and M(i) are the pellet radius and atomic mass.
引用
收藏
页码:431 / 453
页数:23
相关论文
共 39 条
  • [1] PELLET FUELING DEPOSITION MEASUREMENTS ON JET AND TFTR
    BAYLOR, LR
    SCHMIDT, GL
    HOULBERG, WA
    MILORA, SL
    GOWERS, CW
    BAILEY, WP
    GADEBERG, M
    KUPSCHUS, P
    TAGLE, JA
    OWENS, DK
    MANSFIELD, DK
    PARK, HK
    [J]. NUCLEAR FUSION, 1992, 32 (12) : 2177 - 2187
  • [2] Braginskii S., 1965, REV PLASMA PHYS, V1, P205, DOI DOI 10.1088/0741-3335/47/10/005
  • [3] BRAGINSKII SI, 1957, SOV PHYS JETP, V33, P459
  • [4] Chen F F, 1965, PLASMA DIAGNOSTIC TE, P113
  • [5] OPTICAL VISUALIZATION OF ELECTRIC AND MAGNETIC-FIELD PERTURBATIONS IN TOKAMAK DISCHARGES BY HYDROGEN PELLET INJECTION
    DRAWIN, HW
    DUBOIS, MA
    [J]. NUCLEAR FUSION, 1992, 32 (09) : 1615 - 1623
  • [6] DETERMINATION OF THE SAFETY FACTOR PROFILE IN TORE SUPRA FROM THE LARGEST STRIATIONS OBSERVED DURING PELLET ABLATION
    DUBOIS, MA
    SABOT, R
    PEGOURIE, B
    DRAWIN, HW
    GERAUD, A
    [J]. NUCLEAR FUSION, 1992, 32 (11) : 1935 - 1940
  • [7] TIME-DEPENDENT SIMULATION OF PELLET EVAPORATION IN TOKAMAK PLASMAS
    DUNNING, MJ
    MAYER, FJ
    KAMMASH, T
    [J]. NUCLEAR FUSION, 1990, 30 (05) : 919 - 924
  • [8] EXPERIMENTAL-OBSERVATIONS OF THE DYNAMICS OF PELLET ABLATION ON THE TEXAS EXPERIMENTAL TOKAMAK (TEXT)
    DURST, RD
    ROWAN, WL
    AUSTIN, ME
    COLLINS, RA
    GANDY, RF
    PHILLIPS, PE
    RICHARDS, B
    [J]. NUCLEAR FUSION, 1990, 30 (01) : 3 - 9
  • [9] CURRENT-DENSITY PROFILE AND ELECTRON-BEAM LOCALIZATION MEASUREMENTS USING CARBON PELLETS ON T-10
    EGOROV, SM
    KUTEEV, BV
    MIROSHNIKOV, IV
    MIKHAILENKO, AA
    SERGEEV, VY
    USHAKOV, SN
    BAGDASAROV, AA
    CHISTYAKOV, VV
    ELIZAVETIN, DY
    VASIN, NL
    [J]. NUCLEAR FUSION, 1992, 32 (11) : 2025 - 2028
  • [10] EGOROV SM, 1991, PLASMA PHYS CONTROLL, V1, P599