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Residual Energy in Weak and Strong MHD Turbulence

机译:弱和强大的MHD湍流中的残余能量

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摘要

Recent numerical and observational studies revealed that spectra of magnetic and velocity fluctuations in MHD turbulence have different scaling indexes. This intriguing feature has been recently explained in the case of weak MHD turbulence, that is, turbulence consisting of weakly interacting Alfvén waves. However, astrophysical turbulence is strong in majority of cases. In the present work, we propose a unifying picture that allows one to address weak and strong MHD turbulence on the same footing. We argue that magnetic and kinetic energies are different in both weak and strong MHD turbulence. Their difference, the so-called residual energy, is spontaneously generated by turbulence, it has the Fourier spectrum E_r(k) = E_v(k) - E_b(k) ∝ - f_w(k_∥/k_⊥)k_⊥~(-2) in weak turbulence, and E_r(k) ∝ - f_s(k_∥/k_⊥) k_⊥~(-3) in strong turbulence. Here f_(w,s)(x) are functions declining fast for x > C_(w,s) and not significantly varying for x < C_(w,s) with some constants C_(w,s), and k_∥ and k_⊥ the field-parallel and field-perpendicular wave vectors with respect to the applied strong uniform magnetic field.
机译:近期数值和观测研究表明,MHD湍流中的磁性和速度波动的光谱具有不同的缩放指标。最近在MHD湍流的情况下最近已经解释了这种有趣特征,即由弱互动的Alfvén波组成的湍流。然而,在大多数情况下,天体物理湍流都很强烈。在目前的工作中,我们提出了一个统一的图片,允许一个人在相同的基础上解决弱和强大的MHD湍流。我们认为磁性和动力学在弱和强大的MHD湍流中不同。它们的差异是通过湍流自发地产生的所谓的残余能量,它具有傅里叶频谱E_R(k)= e_v(k) - e_b(k)α - f_w(k_∥/k_⊥)k_ə〜( - 2)在弱湍流中,E_R(k)α - f_s(k_∥/ k_m)k_⊥〜(-3)强的湍流。这里f_(w,s)(x)是x> c_(w,s)的函数,并且对于具有一些常量c_(w,s)和k_∈和k_∈和k_∈和k_∈和K_⊥相对于施加的强均匀磁场的场平行和场垂直波矢量。

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