Author/Authors :
Ghendrih، نويسنده , , Ph. and Bécoulet، نويسنده , , M. and Costanzo، نويسنده , , L. and Corre، نويسنده , , Y. and Grisolia، نويسنده , , C. and Grosman، نويسنده , , A. and Guirlet، نويسنده , , R. and Gunn، نويسنده , , J. and Loarer، نويسنده , , T. and Monier-Garbet، نويسنده , , P. and Mank، نويسنده , , G. and Reichle، نويسنده , , R. and Vallet، نويسنده , , Zabiego، M. نويسنده , , M. and Azéroual، نويسنده , , A. and Bucalossi، نويسنده ,
Abstract :
Experimental evidence of the location of the ergodic divertor separatrix is shown to agree with the predicted value given by codes. Variation of this position modifies the divertor tightness, defined as the ratio of the divertor to core density. This effect is governed by laminar transport, i.e., transport proportional to the magnitude of the perturbation. Operation with feedback control of the divertor temperature allows one to optimise the choice of injected impurity species. At 10 eV divertor temperature, nitrogen is shown to lead to the largest decrease in energy flux to the divertor at lowest contribution to Zeff. Parallel energy fluxes as low as 2 MW m−2 are thus achieved on the target plates. For this impurity, radiation is localised in the divertor volume thus leading to radiation compression close to 10. The ergodic divertor appears as a powerful tool to control plasma–wall interaction with no loss of core confinement or plasma current.
