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Experimentally-based ExB drifts in the DIII-D divertor and SOL calculated from integration of Ohm's law using Thomson scattering measurements of T e and n e

机译:基于欧姆定律积分的DIII-D偏滤器和SOL中基于实验的ExB漂移,使用T e 和n e

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The 2D spatial distributions of cross field drift velocities are calculated from 2D Thomson scattering measurements of T e and n e in the divertor and SOL of DIII-D. In contrast with the method that has been used on DIII-D where the 2D distribution of plasma potential V plasma is obtained from measurements of the probe floating potential of reciprocating probes, the present method does not require insertion of a probe into the plasma and can therefore be used in high power discharges. The 2D spatial distribution of V plasma is calculated from Ohm's Law for the parallel electric field E || along each flux tube, E ∥ ( s ∥ ) = ? 1.71 d T e / d s ∥ ? ( T e / n e ) d n e / d s ∥ , where the Thomson scattering values of T e and n e are used. To within a constant of integration, V plasma is obtained by integrating E || along the flux-tubes (field lines); the constant is obtained for each flux tube using the sheath drop at the target calculated from the characteristic of Langmuir probes built into the divertor tiles. The 2D distributions of E radial = ? d V p / d s radial , E poloidal = ? d V p / d s poloidal , v ExB poloidal = E radial / B and v ExB radial = E poloidal / B are then calculated as well as the particle drift flux densities Γ ExB poloidal = nv ExB poloidal and Γ ExB radial = nv ExB radial for electrons, fuel ions and impurity ions, using the appropriate values of particle density, n.
机译:横场漂移速度的二维空间分布是根据DIII-D的分流器和SOL中T e和n e的二维Thomson散射测量值计算得出的。与DIII-D上使用的方法相反,在DIII-D上,通过测量往复式探针的探针浮动电势获得血浆电势Vplasma的2D分布,本方法不需要将探针插入血浆中并且可以因此可用于大功率放电。 V等离子体的二维空间分布是根据欧姆定律针对平行电场E ||计算的。沿每个通量管,E∥(s∥)=? 1.71 d T e / d s? (T e / n e)d n e / d s∥,其中使用了T e和n e的汤姆森散射值。通过积分E ||,可以在积分常数内获得V等离子体。沿通量管(磁力线);对于每个通量管,使用从内置在偏滤器瓦中的Langmuir探头的特性计算得出的目标处的护套压降即可获得该常数。 E径向的2D分布=? d V p / d s径向,E倍数=?然后计算d V p / ds极点,v ExB极点= E径向/ B和v ExB极点= E径向/ B以及粒子漂移通量密度ΓExB极点= nv ExB极点和ΓExB径向= nv ExB径向对于电子,燃料离子和杂质离子,使用适当的粒子密度值n。

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