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arXiv 2011.03911physics.plasm-ph
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强迫磁重联从线性区向卢瑟福区转变的准线性理论

Quasi-linear theory of forced magnetic reconnection for the transition from linear to Rutherford regime

Wenlong Huang, Ping Zhu

摘要:

本文利用无粘双场简化MHD模型,发展了一种新的解析理论,将HKT线性解和Rutherford准线性区统一起来。采用准线性方法,我们得到了一个封闭的方程组的等离子体响应的静态等离子体板几何形状。得到了强迫磁重联的积分形式的解析解,从HKT线性解到卢瑟福准线性解,该解析解在整个区域内都是一致有效的.特别地,准线性效应可以通过单个系数$K_s\propto S^{8/5} ψ_c^2$来描述,其中$S=\frac{τ_R}{τ_A}$和$ψ_c$分别是外部磁扰动的伦奎斯特数和幅度。当指标$K_s\rightarrow 0$。另一方面,准线性效应在$K_s\sim1$时的岛生长中起关键作用。我们的新的解析解也进行了比较,减少MHD模拟协议。

英文摘要:

Using the in-viscid two-field reduced MHD model, a new analytical theory is developed to unify the Hahm-Kulsrud-Taylor (HKT) linear solution and the Rutherford quasi-linear regime. Adopting a quasi-linear approach, we obtain a closed system of equations for plasma response in a static plasma in slab geometry. An integral form of analytical solution is obtained for the forced magnetic reconnection, uniformly valid throughout the entire regimes from the HKT linear solution to the Rutherford quasi-linear solution. In particular, the quasi-linear effect can be described by a single coefficient $K_s\propto S^{8/5} ψ_c^2$, where $S=\frac{τ_R}{τ_A}$ and $ψ_c$ are the Lunquist number and amplitude of external magnetic perturbation, respectively. The HKT linear solution for response can be recovered when the index $K_s\rightarrow 0$. On the other hand, the quasi-linear effect plays a key role in the island growth when $K_s\sim1$. Our new analytical solution has also been compared with reduced MHD simulations with agreement.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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