134 research outputs found

    Improvements in the CHERS system for DT experiments on TFTR

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    Improvements in the charge exchange recombination spectroscopy (CHERS) system have resulted in accurate measurements of T{sub i} and V{sub {phi}} profiles during DT experiments. These include moving the spectrometer detector array and electronics farther away from the tokamak to a low neutron flux location. This relocation has also improved access to all components of the system. Also, a nonplasma-viewing calibration fiber system was added to monitor the change in fiber transmission due to the high flux DT neutrons. Narrowband filtered light transmitted through the calibration fiber is now used as a reference for the VO measurement. At the highest neutron flux of {approximately} 2.5 {times} 10{sup 18} neutrons/see (fusion power {approximately} 6.2 MW) a modest 5% decrease in fiber transmission was observed. Corrections for transmission loss are made and T{sub i} (r,t) and absolute V{sub phi} (r,t) profiles are automatically calculated within four minutes of every shot

    TRANSPORT PHYSICS IN REVERSED SHEAR PLASMAS

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    Abstract TRANSPORT PHYSICS IN REVERSED SHEAR PLASMAS. Rcversed magnetic shear is considered a good candidate for improving the tokamak c m q t because it has the potcntial to stabilize MHD instabilities and reduce panicle and energy transport. With reduced transpon. the high ptessun gradient would generate a strong off-axis bootstrap current and could sustain a hollow current density profile. Such a conlbination of favorable conditions cwld lead to an attractive steady-state tokamak configuntion. Indeed, a new tokamak confinement regime with reversed magnetic shear has been cbserved on the Tokamak Fusion Test Reactor (TFTR) where the panicle. mOnienNm. &,ion thermal diffusiviticr drop precipitously, by Over an order of magnitude. ?he panicle diffusivity drops to the neoclassical level and the ion thermal diffisivity drops to much less than the neoclassical value in the region with mend shear. This enhanced reversed shear CERS) confinement mode is characterized by an abmpt tmsition with P large rate of rise of the density in the reversed shear region dur!ng neutral beam injection. resulting in nearly a factor of three increase in the ccntral density to -1.2 x 10" ni-'. At thc smie time thc density fluctuation levfl in the reversed shcar region dramatically decreases. The ion and clcctron temperatures, which are about 20 keV and 7 keV respectively, change little during the ERS mode. Thc transport and transition into and out of the ERS mode have been studied on TFTR with plasma currcnts in the range 0.9-2.2 MA, with a toroidal magnetic field of 2.7-4.6 T. and the radius of thc q(r) mininium. qmb, has been varied from do = 0.35 to 0.55. Toroidal field and co/counter neutral beam injection toroidal rotation variations have been used to elucidate the underlying physics of the transition mcchanism and power threshold of the ERS mode. 19980330 097 31
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