## 抄録

A new theoretical method is presented to analyse turbulence and associated transport in far-non-equilibrium fluids and plasmas. First, direct nonlinear interactions with background turbulence are renormalized into nonlinear dielectric form. The relation between the turbulent intensity spectra of energy and temperature, E(k) and E_{θ}(k), and the nonlinear transfer rates (dielectric) of momentum and energy, ν_{N} and κ_{N}, are obtained as recurrent formulae of integral equations. Second, nonlinear marginal stability conditions are examined by introduction of dressed test mode analysis. Solutions have a power law which are analogous to critical exponents in renormalization group theory. The same paradigm is first applied to neutral fluids to recover conventional results. For two-dimensional (2D) buoyancy-driven turbulence, where a supercritical turbulence appears, spectral forms of E(k), E_{θ}(k) ∝ |g·∇T|k^{-3} and ν_{N}(k), κ_{N}(k) ∝ (|g·∇T|)^{1/2}k^{-2} are obtained in the energy containing range (or subrange). (∇T is the temperature gradient and g is the gravity.) The relation between global turbulent transport coefficients, such as ν_{T} and κ_{T}, and nonlinear transfer rates ν_{N} and κ_{N} is obtained. A global spatial structure of the turbulent fluid, which is consistent with the spectrum, is solved. The Nusselt number is obtained as Nu ≃ 0.4(R_{a}/R_{ac})^{1/3} and the relations κ_{T} ∝ (R_{a}/R_{ac})^{4/9} and ν_{T} ∝ (R_{a}/R_{ac})^{4/9} are obtained. (R_{a} is the Rayleigh number and R_{ac} is the critical Rayleigh number.) To turbulence in the magnetized plasma, where a subcritical turbulence appears, this paradigm is applied. The combination of the pressure gradient (∇p) and magnetic field gradient (Ω′), G_{0} = ∇p·Ω′, characterizes the non-equilibrium form of the plasma. The spectral intensity of the fluctuating fields forthe potential, current and pressure E(k), E_{J}(k), Eθ(k) ∝ G_{0}k^{-3} and the nonlinear transfer rates μ_{N}(k), λ_{N}(k), χ_{N}(k) ∝ (G_{0})^{1/2}k^{-2} are first obtained (symbols μ, λ and χ correspond to the ion viscosity, current diffusivity and heat diffusivity, respectively) in the energy containing range. The turbulence level, W, and the transport coefficients, χ_{T}, are derived as W ∝ G_{0}^{2}, and χ_{T} ∝ G_{0}^{3/2}. The dissipation balance is also examined. These analyses demonstrate that this method is applicable to both the supercritical and subcritical turbulences in neutral fluid and plasma turbulences, i.e. in systems which are far from the thermal equilibrium.

本文言語 | 英語 |
---|---|

ページ（範囲） | 1729-1766 |

ページ数 | 38 |

ジャーナル | Plasma Physics and Controlled Fusion |

巻 | 40 |

号 | 10 |

DOI | |

出版ステータス | 出版済み - 12月 1 1998 |

## !!!All Science Journal Classification (ASJC) codes

- 原子力エネルギーおよび原子力工学
- 凝縮系物理学