Abstract:With a given density profile of plasma,the temperature profiles of the plasma operating in the negative central magnetic shear mode,the H-mode and L-mode of conventional magnetic shear,are calculated respectively by applying the energy equation of electrons and ions,according to the thermal conductivity in different operational regimes.And then the electron cyclotron current drive and wave power deposition in the above modes are investigated with the relativistic Fokker-Planck equation incorporated into a ray … Show more
“…[3] ECCD is one of the main means of controlling MHD activity in ITER. [4] Stabilization of MHD by ECCD has been observed in HL-2A, [5,6] DIII-D, [7] JT-60U, [8] etc.…”
韦 维) a)b) , Ding Bo-Jiang(丁伯江) a) † , Zhang Xin-Jun(张新军) a) , Wang Xiao-Jie(王晓洁) a) , Li Miao-Hui(李妙辉) a) , Kong Er-Hua(孔二华) a) , and Zhang Lei(张 磊) a) a)
“…[3] ECCD is one of the main means of controlling MHD activity in ITER. [4] Stabilization of MHD by ECCD has been observed in HL-2A, [5,6] DIII-D, [7] JT-60U, [8] etc.…”
韦 维) a)b) , Ding Bo-Jiang(丁伯江) a) † , Zhang Xin-Jun(张新军) a) , Wang Xiao-Jie(王晓洁) a) , Li Miao-Hui(李妙辉) a) , Kong Er-Hua(孔二华) a) , and Zhang Lei(张 磊) a) a)
“…Electron-cyclotron current drive (ECCD) has become a widely used way to drive current and stabilize magnetohydrodynamic (MHD) instabilities in toroidal magnetic confinement devices, since the electron-cyclotron (EC)-driven current profiles are spatially localized and the EC current drive efficiency is competitive with other approaches, such as neutral beam. [1][2][3][4] The HL-2M project is the up-grade of the HL-2A tokamak with plasma elongation up to 1.8. The goal of the HL-2M is to illuminate important research issues such as the physics of plasma confinement, transport, high energy particles, MHD stability, and the interaction between the first wall and plasma for fusion study.…”
The capabilities of current drive, neoclassical tearing mode (NTM) stabilization, and sawtooth control are analyzed for the electron-cyclotron wave (ECW) system in a HL-2M tokamak. Better performance of the upper launcher is demonstrated in comparison with that of a dropped upper launcher, in terms of J EC /J bs for NTM stabilization and I ECCD /(∆ρ tor ) 2 for sawtooth control. 1-MW ECW power is enough for the 3/2 NTM stabilization, and 1.8-MW ECW power is required to suppress 2/1 NTM in a single null divertor equilibrium with 1.2-MA toroidal current with the upper launcher. Optimization simulation of electron-cyclotron current drive (ECCD) is carried out for three mirrors in an equatorial port, indicating that the middle mirror has a good performance compared with the top and bottom mirrors. The results for balanced co-and counter-ECCD in an equatorial port are also presented.
“…[1] The plane mirrors of ECRH antenna can be rotated in the toroidal and poloidal directions, [2] thereby it can provide on/off-axis heating, and ECCD experiment. [3] Time evolution of soft x-ray spectra is measured by SDD system, the thermal and superthermal electron temperatures are derived according to energy spectra. Because of the ratio of peak counts to background counts is very high in the measurements of energy spectra for the mono-energy x-ray reference sources such as M nkα (5.894 keV), M okα,kβ (17.44, 19.63 keV), p/b ≥ 400-3000, these spectra also can be regarded as the electron velocity distributions roughly.…”
Two high performance silicon drift detectors (SDD) are installed at the equatorial port with z = 0 and z = −16.4 cm on HL-2A tokamak, respectively. These SDDs combine with the new and non-conventional software pulse height analyser (SPHA) successfully developed more recently by us to measure the time evolution of soft x-rays spectra, the thermal and superthermal electron temperatures. The high-quality three-dimensional figure of time evolution for soft x-rays energy spectra is easily obtained by combination of a new SPHA and computer. Therefore, the measurement accuracies and the time resolutions of thermal and superthermal electron temperatures are also improved. The enhancement phenomenon of superthermal electron during electron cyclotron resonance heating (ECRH) can be explained by the combination of superthermal electron avalanche theory and experimental parameters.
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