Annual Report (MS-Word)
s
m-3 at JT-60. By the dynamic profile control and suppression of MHD instability of high beta-poloidal plasmas, notably large fusion product of 4 x 1020 m-3
s
keV ( equivalent QDT = 0.25 ) was sustained for 1.5 s in the quasi-steady-state ELMy H-mode discharge also at JT-60. In addition, JET has demonstrated the 20s steady-state H-mode as well as 7s high beta-poloidal discharge. The results from JT-60 and JET both indicate clearly the advantage of high beta-poloidal regime for the steady-state tokamak operation, which is accompanied by a large fraction of the bootstrap current. A number of scientists from JET and JT-60 participated in the TFTR D-T campaign, while TFTR proposed and conducted a part of high beta-poloidal runs at JT-60. Tritium transport was also intensively studied at TFTR, and the energetic ion loss in TFTR plasmas was investigated in collaboration with JT-60. Extensive joint work between JET and JT-60 was beneficial for ITER EDA. I. JET
After a commissioning procedure which started from the beginning of '94, JET resumed operation in mid-February with the new divertor configuration. Experimental programme started in early May, and the discharge optimization has been intensively carried out at Ip / BT = 2 MA / 2.8 T with ELMy H-mode phases reaching a duration of 20s. The additional heating system has also been successfully commissioned, and the non-inductive current drive of 2 MA was achieved. The combined heating power has thereby reached 26 MW.
The heat load capability was improved by an order of magnitude, and 140 MJ has been injected into the plasma whereas in the previous configuration a carbon bloom occurred after 15 MJ. However, the ELM-free periods are shorter and the ELM frequency is higher due to the increased recycling and reduced triangularity, even so ELM-free durations of 2s have been achieved. In the transient peak performance regimes, the fusion product has reached 85% and QDD 75% of previous best values despite the now smaller plasma volume.
Operating regimes have been established at 4 and 5 MA. The divertor cryopump is operating successfully and is being used for divertor pumping and helium exhaust studies. Detached plasmas with radiative transfer in the divertor have been obtained using nitrogen puffing. This work is directly relevant to ITER.
High values of
~ 2% have been maintained for 7s (
= 3,
= 1.5 at Ip / BT = 1.5 MA / 1.4 T). Collaboration with JT-60 and with TFTR have suggested important operating regimes and experimental investigations. Important experiments for the near future are experiments with variable toroidal ripple and a comparison of the present operation using CFC divertor target plates with operation on beryllium target plates.
II. JT-60
During the 1994 campaign, major experimental efforts have been devoted to further enhancement of the integrated fusion performance at JT-60, focusing on the attainment of steady-state improved confinement regimes. As a result of the dynamic control of heat deposition and current density profile as well as the suppression of
-collapse, a large fusion product of 4 x 1020 m-3
s
keV ( equivalent QDT = 0.25 ) was sustained for 1.5 s in the ELMy H-mode discharge, while the highest performance achieved was 1.2 x 1021 m-3
s
keV ( equivalent QDT = 0.46 ). Termination of the steady-state high performance was caused by the carbon influx from the divertor plates. It was also documented that Helium accumulation was subtle in the ELMy H-mode, in spite of the deteriorated Helium exhausting capability relative to the L-mode.
Non-inductive current drive experiment with substantial bootstrap and NB driven current fraction have also been intensively carried out. Production of the reversed shear was found to have influences on the achieved values of normalized and poloidal beta both around 3 and the H-factor of 2.2 for 1 s. The full current drive condition was sustained for 0.65 s. Production of the internal transport barrier is the key factor for the attainment of high-
mode. The influence of the heat deposition and momentum input profile on the transport barrier formation was investigated in collaboration with TFTR group.
In addition, recent turbulent transport studies prevailed that the long-wavelength mode can possibly be responsible for the deteriorated confinement in the L-mode discharges. This is consistent with the TFTR results.
III. TFTR
The TFTR device continued to optimize the D-T plasma performance with the increased toroidal field capability and beam power, and number of scientists from JET and JT-60 participated. A maximum fusion power of 10.7 MW was obtained, and it was sustained above 10 MW for approximately 0.1 s. The highest fusion product obtained hereby reached 5 x 1020 m-3
s
keV. Lithium pellet injection allowed the supershot conditions to be obtained at the high plasma current of 2.7 MA.
The observed neutron flux was in good agreement with calculated value based on the electron and ion temperature and density profiles. The loss of alpha particles can be attributed to the classical first orbit loss. In these high power D-T experiments, collective instabilities induced by the presence of alpha particles have not been documented. The stored plasma energy, electron and ion temperature increased in deuterium-tritium plasmas compared with similar deuterium plasmas, corresponding to an increase in
from 160 ms to 210 ms.
Tritium transport has also been intensively carried out with multi-channel neutron collimator, and it has been documented that tritium diffusivity is similar to that of He and the thermal diffusivity of deuterium, which is consistent with the E x B drift theory. For r / a < 0.5, the deduced ion thermal diffusivity is a factor of 1.5 lower in the D-T plasma compared to the D-D plasma. This suggests a strong sensitivity of ion heat conduction to isotopic composition in supershots plasmas.
in these supershot discharges increases with the mass of the Hydrogenic species.
H-mode features also differs from the D-D discharges i.e., larger Da drop and ELM amplitude, smaller ELM frequency, and
/
ITER-89P > 4.3 was achieved in D-T limiter H-mode discharges. The amount of reduction in
i is also significant in D-T discharges.
Second harmonic tritium heating with 5.5 MW of ICRF power superimposed on the 23 MW of NB power has resulted in increasing the ion temperature from 26 to 36 keV. Te increased from 8 to 10.5 keV due to direct electron damping as well as 3He minority heating.