Multiple timescale calculations of sawteeth and other global macroscopic dynamics of tokamak plasmas

S. Jardin, N. Ferraro, J. Breslau, J. Chen
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引用次数: 62

Abstract

The M3D-C1 (Breslau et al 2009 Phys. Plasmas 16 092503) code is designed for performing three-dimensional nonlinear magnetohydrodynamics (MHD) calculations of a tokamak plasma that span the timescales associated with ideal and resistive stability as well as parallel and perpendicular transport. This requires a scalable fully implicit time advance where the time step is not limited by a Courant condition based on the MHD wave velocities or plasma flow but is chosen instead to accurately and efficiently resolve the physics. In order to accomplish this, we make use of several techniques to improve the effective condition number of the implicit matrix equation that is solved every time step. The split time advance known as the differential approximation (Caramana 1991 J. Comput. Phys. 96 484) reduces the size of the matrix and improves its diagonal structure. A particular choice of velocity variables and annihilation operators approximately splits the large matrix into three sub-matrices, each with a much improved condition number. A final block-Jacobi preconditioner further dramatically improves the condition number of the final matrix, allowing it to converge in a Krylov solver (GMRES) with a small number of iterations. As an example, we have performed transport timescale simulations of a tokamak plasma that periodically undergoes sawtooth oscillations (Von Goeler et al 1974 Phys. Rev. Lett. 33 1201). We specify the transport coefficients and apply a 'current controller' that adjusts the boundary loop-voltage to keep the total plasma current fixed. The short-time plasma response depends on the initial conditions, but the long-time behavior depends only on the transport coefficients and the boundary conditions applied.
锯齿等托卡马克等离子体宏观动力学的多时间尺度计算
M3D-C1 (Breslau et al . 2009)等离子体16 092503)代码设计用于执行三维非线性磁流体动力学(MHD)计算托卡马克等离子体,该计算跨越与理想和电阻稳定性以及平行和垂直输运相关的时间尺度。这需要一个可扩展的完全隐式时间提前,其中时间步长不受基于MHD波速或等离子体流的Courant条件的限制,而是选择准确有效地解决物理问题。为了达到这一目的,我们利用了几种技术来提高隐式矩阵方程的有效条件数。被称为微分逼近的分裂时间推进(Caramana 1991 J. Comput)。物理学报。96 484)减小了矩阵的尺寸并改善了它的对角线结构。一个特定的速度变量和湮灭算子的选择近似地将大矩阵分成三个子矩阵,每个子矩阵都有一个改进的条件数。最终块- jacobi预调节器进一步显著提高了最终矩阵的条件数,使其能够在少量迭代的Krylov解算器(GMRES)中收敛。作为一个例子,我们已经对周期性经历锯齿振荡的托卡马克等离子体进行了输运时间尺度模拟(Von Goeler et al . 1974物理学)。Rev. Lett. 33 1201)。我们指定传输系数,并应用一个“电流控制器”来调整边界环电压,以保持总等离子体电流固定。等离子体的短时间响应取决于初始条件,而长时间行为仅取决于输运系数和所应用的边界条件。
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