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Overview of DT results from TFTR

  • Author(s): Bell, MG
  • McGuire, KM
  • Arunasalam, V
  • Barnes, CW
  • Batha, SH
  • Bateman, G
  • Beer, MA
  • Bell, RE
  • Bitter, M
  • Bretz, NL
  • Budny, RV
  • Bush, CE
  • Cauffman, SR
  • Chang, Z
  • Chang, C-S
  • Cheng, CZ
  • Darrow, DS
  • Dendy, RO
  • Dorland, W
  • Duong, HH
  • Durst, RD
  • Efthimion, PC
  • Ernst, D
  • Evenson, H
  • Fisch, NJ
  • Fisher, RK
  • Fonck, RJ
  • Fredrickson, ED
  • Fu, GY
  • Furth, HP
  • Gorelenkov, NN
  • Grek, B
  • Grisham, LR
  • Hammett, GW
  • Hanson, GR
  • Hawryluk, RJ
  • Heidbrink, WW
  • Herrmann, HW
  • Hill, KW
  • Hosea, JC
  • Hsuan, H
  • Hughes, MH
  • Hulse, RA
  • Janos, AC
  • Jassby, DL
  • Jobes, FC
  • Johnson, DW
  • Johnson, LC
  • Kesner, J
  • Kugel, HW
  • Lam, NT
  • Leblanc, B
  • Levinton, FM
  • Machuzak, J
  • Majeski, R
  • Mansfield, DK
  • Mazzucato, E
  • Mauel, ME
  • McChesney, JM
  • McCune, DC
  • McKee, G
  • Meade, DM
  • Medley, SS
  • Mikkelsen, DR
  • Mirnov, SV
  • Mueller, D
  • Navratil, GA
  • Nazikian, R
  • Owens, DK
  • Park, HK
  • Park, W
  • Parks, PB
  • Paul, SF
  • Petrov, MP
  • Phillips, CK
  • Phillips, MW
  • Pitcher, CS
  • Ramsey, AT
  • Redi, MH
  • Rewoldt, G
  • Roberts, DR
  • Rogers, JH
  • Ruskov, E
  • Sabbagh, SA
  • Sasao, M
  • Schilling, G
  • Schivell, JF
  • Schmidt, GL
  • Scott, SD
  • Semenov, I
  • Sesnic, S
  • Skinner, CH
  • Stratton, BC
  • Strachan, JD
  • Stodiek, W
  • Synakowski, EJ
  • Takahashi, H
  • Tang, WM
  • Taylor, G
  • Terry, JL
  • Thompson, ME
  • Tighe, W
  • Goeler, S Von
  • White, RB
  • Wieland, RM
  • Wilson, JR
  • Wong, K-L
  • Woskov, P
  • Wurden, GA
  • Yamada, M
  • Young, KM
  • Zarnstorff, MC
  • Zweben, SJ
  • et al.
Abstract

Experiments with plasmas having nearly equal concentrations of deuterium and tritium have been carried out on TFTR. To date (September 1995), the maximum fusion power has been 10.7 MW, using 39.5 MW of neutral beam heating, in a supershot discharge and 6.7 MW in a high beta P discharge following a current ramp-down. The fusion power density in the core of the plasma has reached 2.8 MW/m3, exceeding that expected in the International Thermonuclear Experimental Reactor (ITER). The energy confinement time tau E is observed to increase in DT, relative to D plasmas, by 20% and the n1(0).T1(0). tau E product by 55%. The improvement in thermal confinement is caused primarily by a decrease in ion heat conductivity in both supershot and limiter H mode discharges. Extensive lithium pellet injection increased the confinement time to 0.27 s and enabled higher current operation in both supershot and high beta P discharges. First measurements of the confined alpha particles have been performed and found to be in good agreement with TRANSP simulations assuming classical confinement. Measurements of the alpha ash profile have been compared with simulations using particle transport coefficients from helium gas puffing experiments. The loss of energetic alpha particles to a detector at the bottom of the vessel is well described by the first-orbit loss mechanism. No loss due to alpha particle driven instabilities has yet been observed. ICRF heating of a DT plasma, using the second harmonic of tritium, has been demonstrated. DT experiments on TFTR will continue both to explore the physics underlying the ITER design and to examine some of the physics issues associated with an advanced tokamak reactor.

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