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首页> 外文期刊>Physics of plasmas >Finite-temperature corrections to the time-domain equations of motion for perpendicular propagation in nonuniform magnetized plasmas
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Finite-temperature corrections to the time-domain equations of motion for perpendicular propagation in nonuniform magnetized plasmas

机译:在非均匀磁化等离子体中垂直传播时域运动方程的有限温度校正

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In this paper we extend the new techniques of W. Tierens and D. D. Zutter, J. Comput. Phys. 231, 5144 (2012) to include finite Larmor radius effects up to second order in the Larmor radius. We limit ourselves to the case of propagation perpendicular to the background magnetic field B→_0. We show that our time-domain technique is able to produce the lowest-order Bernstein wave (a wave believed to be useful for heating fusion devices [H. P. Laqua, Plasma Phys. Controlled Fusion 49, R1 (2007)]). The discrete equations retain many of the favourable properties described in W. Tierens and D. D. Zutter, J. Comput. Phys. 231, 5144 (2012), i.e., unconditional stability and a straightforward relation between the second-order accurate continuous dispersion relation and the dispersion relation of the discretized problem. The theory is illustrated by a place-independent and a place-dependent temperature numerical example.
机译:在本文中,我们扩展了W. Tierens和D. D. Zutter,J. Comput的新技术。物理231,5144(2012)包括有限的拉莫尔半径效应,直到拉莫尔半径为二阶。我们将自身限制为垂直于背景磁场B→_0传播的情况。我们证明了我们的时域技术能够产生最低阶的伯恩斯坦波(一种对加热聚变设备有用的波[H. P. Laqua,等离子物理控制聚变49,R1(2007)])。离散方程保留了W.Tierens和D.D.Zutter,J.Comput。物理231,5144(2012),即无条件稳定性和二阶精确连续色散关系与离散问题的色散关系之间的直接关系。通过与位置无关和与位置有关的温度数值示例来说明该理论。

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