09.12.2012 Views

1 - Nuclear Sciences and Applications - IAEA

1 - Nuclear Sciences and Applications - IAEA

1 - Nuclear Sciences and Applications - IAEA

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

266 TSUJ1 et a).<br />

1. INTRODUCTION<br />

JT-6O is a large tokamak with powerful auxiliary heating systems. It was<br />

operated over a wide range of plasma parameters in 1987: 1 < Ip < 3.2 MA,<br />

0.65 < ap < 0.92 m, <strong>and</strong> 5 X 10' 8 :£ n,. < 1.2 x 10 20 nr 3 . A combined heating<br />

power of up to 30 MW was injected <strong>and</strong> the plasma stored energy was increased to<br />

3 MJ [1, 2].<br />

The improvements in confinement have been explored with beam heated hydrogen<br />

plasmas by several methods; by current profile modification with LHCD [3-5],<br />

by beam acceleration with ICRF [6, 7] <strong>and</strong> by H-mode transition with the outer<br />

X-point [1, 2, 8], A new divertor coil was installed to produce a lower X-point configuration<br />

at the beginning of 1988. Hence, JT-60 has become a unique device where<br />

the effect of configurations, limiter <strong>and</strong> outer or lower X-point on the plasma confinement<br />

can be examined with the same heating <strong>and</strong> diagnostic systems.<br />

NB heating experiments in the lower X-point configuration (ap « 0.65 m,<br />

K « 1.3) have been carried out with PMB up to 25 MW. A new regime of improved<br />

divertor confinement (IDC) appears in the lower X-point configuration when the<br />

heating power exceeds about 15 MW. The IDC regime is characterized by high particle<br />

recycling <strong>and</strong> remote radiative cooling in the divertor region, which is required<br />

to alleviate the heat load on the divertor plates of the fusion reactors.<br />

2. IMPROVED CONFINEMENT REGIME WITH LOWER X-POINT<br />

Discharge waveforms with <strong>and</strong> without improved divertor confinement are<br />

compared in Fig. 1. The thick lines in the figure are traces of an improved<br />

shot (E6950, Bt = 4.0 T) <strong>and</strong> the thin lines st<strong>and</strong> for an unimproved shot (E6956,<br />

Bt = 2.7 T). The stored plasma energy of the former shot begins to rise around<br />

6.1 s whereas that of the latter shots saturates early. Lowering the effective safety<br />

factor, qeff, leads to an excitation of edge localized modes (ELMs), which prevent<br />

the discharges from reaching the IDC regime. Frequent ELMs can be clearly seen<br />

in the H° w trace.<br />

The improvement is associated with an increase in the electron density <strong>and</strong> a<br />

decrease in the radiation power from the core plasma. The central electron temperature<br />

measured by ECE keeps rising with increasing density. Note that the Ha emission<br />

from the divertor region is significantly enhanced during the improved phase.<br />

Bolometric measurements indicate that radiation power both in the divertor <strong>and</strong> near<br />

the X-point regions increases at these moments. These observations suggest that high<br />

particle recycling takes place in the divertor region. Although the carbon impurity<br />

lines tend to rise, the oxygen impurity lines emitted from the main plasma drop<br />

during the improved phase. Visible bremsstrahlung measurement indicates that Zeff<br />

is kept nearly constant throughout the improved phase. The IDC regime is different<br />

from the H-mode since particle recycling never drops <strong>and</strong> there is no sharp transition.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!