TY - JOUR
T1 - Ion temperature profile simulation of JT-60 and TFTR plasmas with ion temperature gradient mode transport models
AU - Shirai, H.
AU - Hirayama, T.
AU - Koide, Y.
AU - Yoshida, H.
AU - Naito, O.
AU - Sato, M.
AU - Fukuda, T.
AU - Sugie, T.
AU - Azumi, M.
AU - Mikkelsen, D. R.
AU - Scott, S. D.
AU - Grek, B.
AU - Hill, K. W.
AU - Johnson, D. W.
AU - Mansfield, D. K.
AU - Park, H. K.
AU - Stratton, B. C.
AU - Synakowski, E. J.
AU - Taylor, G.
AU - Towner, H. H.
PY - 1994
Y1 - 1994
N2 - Ion temperature profiles of neutral beam heated plasmas in JT-60 and TFTR have been simulated using models of ion thermal diffusivity, χi, based on ion temperature gradient mode (ηi mode) turbulence and drift wave turbulence (trapped electron mode and circulating electron mode). The ion temperature profiles measured by charge exchange recombination spectroscopy are compared to predicted Ti profiles calculated from three theoretical models for ion heat transport by Dominguez and Waltz (1987), Lee and Diamond (1986), and Romanelli (1989). All three χi models can reproduce the measured Ti profile over a wide range of parameters in JT-60 L mode plasmas, except for two 1 MA limiter cases. With the use of transport models, which were adjusted to fit JT-60 plasmas, it was found that the Dominguez and Waltz and Romanelli models agree with measured Ti, profiles in TFTR L mode discharges in the region a/4 < r < a/2. The observed central peaking of Ti near the magnetic axis of TFTR L mode plasmas cannot be reproduced. It was found that the Lee and Diamond model does not fit me data as well. The χi models studied cannot consistently reproduce the measured Ti in the peripheral region of either JT-60 or TFTR plasmas. In the high ion temperature (high Ti) plasmas of JT-60 and supershot plasmas of TFTR, the predicted Ti profiles are much broader than the measured profile. In supershot plasmas, the measured central ion temperature greatly exceeds the predicted temperature, although there is reasonable agreement near the edge.
AB - Ion temperature profiles of neutral beam heated plasmas in JT-60 and TFTR have been simulated using models of ion thermal diffusivity, χi, based on ion temperature gradient mode (ηi mode) turbulence and drift wave turbulence (trapped electron mode and circulating electron mode). The ion temperature profiles measured by charge exchange recombination spectroscopy are compared to predicted Ti profiles calculated from three theoretical models for ion heat transport by Dominguez and Waltz (1987), Lee and Diamond (1986), and Romanelli (1989). All three χi models can reproduce the measured Ti profile over a wide range of parameters in JT-60 L mode plasmas, except for two 1 MA limiter cases. With the use of transport models, which were adjusted to fit JT-60 plasmas, it was found that the Dominguez and Waltz and Romanelli models agree with measured Ti, profiles in TFTR L mode discharges in the region a/4 < r < a/2. The observed central peaking of Ti near the magnetic axis of TFTR L mode plasmas cannot be reproduced. It was found that the Lee and Diamond model does not fit me data as well. The χi models studied cannot consistently reproduce the measured Ti in the peripheral region of either JT-60 or TFTR plasmas. In the high ion temperature (high Ti) plasmas of JT-60 and supershot plasmas of TFTR, the predicted Ti profiles are much broader than the measured profile. In supershot plasmas, the measured central ion temperature greatly exceeds the predicted temperature, although there is reasonable agreement near the edge.
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U2 - 10.1088/0029-5515/34/5/I09
DO - 10.1088/0029-5515/34/5/I09
M3 - Article
AN - SCOPUS:0028427414
SN - 0029-5515
VL - 34
SP - 703
EP - 727
JO - Nuclear Fusion
JF - Nuclear Fusion
IS - 5
M1 - I09
ER -