The main objective of the Wendelstein 7-X (W7-X) stellarator is to demonstrate the integrated reactor potential of the optimized stellarator line. An important element of this mission is the achievement of high heating-power and high confinement in steady-state operation. Such an integrated plasma operation has not yet been demonstrated and represents the major scientific goal of W7-X. The way towards this goal is staged. In the first phase, called OP 1.1, December 2015-March 2016, a limiter configuration was used. In this paper, the preparation of the first operation phase as well as lessons learned during the first commissioning and the operation phase are discussed, while the physics results from OP 1.1 are reported elsewhere (Wolf et al 2017 Nucl. Fusion
57 102020).
In this work we describe the heating results in the LH frequency range (f = 2.45 GHz, Pw 5 250 kW, P < 6 k_W/cmz) both in the electron and ion regimes. Efficient electron heating was observes f o r n 5 5 ~1 0 ' ~ c w 3 . Increases of the peak electron temperature up to 700 eV were measured. At higher densities the interaction with electrons disappears. In the ion regime fast neutral tails and neutron enhancement were observed. The influence of plasma boundary conditions on the penetration of the wave is demonstrated. The principal physical problems are pointed out and some possible conclusions are given.
Abstract-Assembly of the superconducting stellarator Wendelstein 7-X is well advanced, and commissioning of the device is being prepared. A first draft of the commissioning tasks has been developed and will be discussed in this paper.
The energy confinement of plasma in FT (Frascati Tokamak) has been studied in a wide range of plasma currents (Ip up to 550 kA) and densities (n̄ up to 4.5 × 1014 cm−3). The Lawson parameter n̂τE has reached a value of 4 × 1013 cm−3 ·s. The main objective was to investigate the limits of validity of the linear relationship between confinement time and density. The ion heat flux has been found to be consistent with neoclassical ion transport. The electron heat diffusion coefficient has been found to increase with plasma current. Indeed, the electron thermal diffusion coefficient has been shown to be approximately proportional to the electron drift parameter (vD/vth). Thus the linear relationship of the electron energy confinement time with density holds only for discharges with the same current. – The deviation from a linear dependence of the totalenergy confinement time on density is due to ion transport and, therefore, appears to be a neoclassical effect.
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