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首页> 外文期刊>The Open Plasma Physics Journal >Current Density Equation in Turbulent Magnetized Plasmas
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Current Density Equation in Turbulent Magnetized Plasmas

机译:湍流磁化等离子体中的电流密度方程

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摘要

A turbulent extension of Ohm's law, derived from the self-consistent action-angle transport theory, ispresented. The equation describes the steady-state profile of the current density in axisymmetric magnetized plasmas inthe presence of magnetic turbulence. The hyper-resistive, helicity-conserving contribution, usually derived in theframework of magneto-hydro-dynamics, is recovered, and the hyper-resistivity is defined. Additionally, the generalizedOhm's law contains an anomalous resistivity term, and a term proportional to the current density derivative. For giventhermodynamic profiles, the numerical solution of the equation shows that turbulent contributions, besides regularizingthe current density profile in the central region, lead to an increase of the total plasma current. This ”turbulent bootstrap“effect provides a possible explanation to discrepancies recently observed between experimental current profiles andneoclassical predictions.
机译:提出了欧姆定律的湍流扩展,它源自自洽的动作角传输理论。该方程描述了在存在磁湍流的情况下轴对称磁化等离子体中电流密度的稳态分布。通常在磁流体动力学框架中得出的超电阻,保螺旋性贡献得到恢复,并定义了超电阻。另外,广义欧姆定律包含反常的电阻率项和与电流密度导数成比例的项。对于给定的热力学曲线,该方程的数值解表明,除了调节中心区域的电流密度曲线以外,湍流贡献还导致总等离子体电流增加。这种“湍流自举”效应为最近在实验电流曲线和新古典预测之间观察到的差异提供了可能的解释。

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