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

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

HEATING OF PEAKED DENSITY PROFILES<br />

PRODUCED BY PELLET INJECTION IN JET<br />

JET TEAM*<br />

(Presented by G.L. Schmidt)<br />

JET Joint Undertaking,<br />

Abingdon, Oxfordshire,<br />

United Kingdom<br />

Abstract<br />

<strong>IAEA</strong>-CN-50/A-IV-l<br />

HEATING OF PEAKED DENSITY PROFILES PRODUCED BY PELLET INJECTION IN JET.<br />

A transient enhancement in performance of JET limiter discharges has been obtained when a<br />

peaked density profile formed by pellet injection is heated by using either ICRH alone or in combination<br />

with NBI. Pellet ftielling is applied during the current rise. Heating follows the fuelling sequence <strong>and</strong><br />

must be localized predominantly within the plasma core. Electron density profiles are strongly peaked<br />

immediately following the pellet injection sequence, ne(0)/vo| < 5, <strong>and</strong> retain a central peak while<br />

decaying during the period of enhancement. At a power level of 19 MW (Prr = 12.5 MW,<br />

Pnb = 5 MW <strong>and</strong> Poh = 1.5 MW) <strong>and</strong> a central density of 6 x 10 19 m~\ central ion <strong>and</strong> electron temperatures<br />

of 10.5 <strong>and</strong> 12 keV are obtained in 3 MA, 3.1 T discharges. Global energy confinement<br />

1.6 times the L-mode level has been obtained. Values of nd(0)Ti(0)TE(a) in the range from 1 to<br />

2 x 10 20 rn" 3 -keV-s are achieved. Peak neutron rates can exceed those in similar, non-enhanced shots<br />

by factors of three to five <strong>and</strong> increase strongly with heating power. Central ion <strong>and</strong> electron pressure<br />

can be enhanced by a factor of two to three. Electron pressure can be > 1 bar with a gradient of<br />

4 bar-m" 1 . Ballooning stability limits are approached within the plasma core. The period of enhanced<br />

performance has extended up to 1.2 s into the heating pulse, terminating spontaneously. The longest<br />

periods terminate with enhanced fluctuations <strong>and</strong> a strong <strong>and</strong> rapid decrease in central electron <strong>and</strong> ion<br />

temperatures. Although MHD activity can be present during this period, no sawtooth activity appears.<br />

1. Introduction<br />

The combination of peaked density profiles produced by pellet fueling with strong,<br />

central ICRF heating has been proposed as a means to enhance performance of limiter<br />

discharges! 1,2,3]. Such experiments have begun on JET using a pellet injector system<br />

jointly built as pan of the JET/USDOE collaboration on pellet fueling. The fueling<br />

source is a multi-barrel, multiple pellet, pneumatic launcher developed at Oak Ridge<br />

National Laboratory[4]. Initial results were reported previously[4,5,6,7]. Improved<br />

performance has been obtained with peaked density profiles in previous ohmic <strong>and</strong><br />

NBI heated experiments[2,8,9,10,llj <strong>and</strong> recently with RF heating in divertor configuration<br />

[12]. Experiments on TFTR[13] <strong>and</strong> JET[14], with high auxiliary heating<br />

power, have demonstrated improved performance in limiter configurations at high<br />

* See Appendix I to this paper.<br />

215

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

Saved successfully!

Ooh no, something went wrong!