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11 mars 2014
New insight on the transition to high confinement regimes in metallic wall fusion devices

The observation that the transition to high confinement regime (the so-called L-H transition) has a lower power threshold in metallic than in carbon wall devices receives an original explanation invoking the potential role of resistive instability at the edge of the plasma

 
New insight on the transition to high confinement regimes in metallic wall fusion devices

Growth rate of the most unstable mode versus the temperature for edge parameters with Zeff=1.3, blue asterisks, Zeff=1, green squares and Zeff=2.2, red circles.The resistive modes are more unstable for larger Zeff (see vertical lines) which is consistent with a larger input power needed to enter into H mode.

Recent observations of the impact of the metallic ITER-like Wall (ILW) in European tokamak JET (UK) show that the transition to high confinement mode  (L-H threshold)  is reduced by 40% with respect to similar experiments in the carbon wall. In the german tokamak ASDEX Upgrade, a similar reduction of the threshold when comparing carbon wall to metallic wall was also observed despite quite different divertor configurations, geometries and wall materials. A common feature of both JET-ILW and ASDEX Upgrade is a significant reduction of the plasma effective charge from C walls to metallic ones.

 

The nature of the primary instability present in the region of the plasma where the confinement is enhanced (pedestal region) prior to the L-H transition is analyzed using a so-called gyro-kinetic code on JET-ILW using temperature and density profile measurements. The linear analysis shows that the primary instability is of resistive nature and can be stabilized when the temperature is increased, hence when the power is increased. The unstable modes are identified as being Resistive Ballooning Modes (RBM). Their growth rates decrease for temperatures increasing towards the experimentally measured temperature at the L-H transition. As the temperature raises further Ion temperature Gradient (ITG) and Trapped Electron Modes (TEM) are destabilized. The low temperature RBM have lower growth rates for lower effective charge Zeff as illustrated by the figure below. This dependence is shown to be in qualitative agreement with recent and past experimental observations of reduced Zeff associated with lower L-H power thresholds.

 

Clarisse Bourdelle, et al, Letter in Nucl. Fusion 54 (2014) 022001

 

Maj : 11/03/2014 (373)

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