A tutorial introduction to the statistical theory of turbulent plasmas, a half-century after Kadomtsev’s Plasma Turbulence and the resonance-broadening theory of Dupree and&nbsp;Weinstock

Krommes, John A.

doi:10.1017/s0022377815000756

A tutorial introduction to the statistical theory of turbulent plasmas, a half-century after Kadomtsev’s Plasma Turbulence and the resonance-broadening theory of Dupree and Weinstock

Journal Article · Mon Sep 21 04:00:00 EDT 2015 · Journal of Plasma Physics

DOI:https://doi.org/10.1017/s0022377815000756· OSTI ID:1256594

Krommes, John A. ^[1]

Princeton Plasma Physics Lab. (PPPL), Princeton, NJ (United States)

In honour of the 50th anniversary of the influential review/monograph on plasma turbulence by B. B. Kadomtsev as well as the seminal works of T. H. Dupree and J. Weinstock on resonance-broadening theory, an introductory tutorial is given about some highlights of the statistical–dynamical description of turbulent plasmas and fluids, including the ideas of nonlinear incoherent noise, coherent damping, and self-consistent dielectric response. The statistical closure problem is introduced. Incoherent noise and coherent damping are illustrated with a solvable model of passive advection. Self-consistency introduces turbulent polarization effects that are described by the dielectric function$${\mathcal{D}}$$. Dupree’s method of using$${\mathcal{D}}$$to estimate the saturation level of turbulence is described; then it is explained why a more complete theory that includes nonlinear noise is required. The general theory is best formulated in terms of Dyson equations for the covariance$$C$$and an infinitesimal response function$$R$$, which subsumes$${\mathcal{D}}$$. An important example is the direct-interaction approximation (DIA). It is shown how to use Novikov’s theorem to develop an$$\boldsymbol{x}$$-space approach to the DIA that is complementary to the original$$\boldsymbol{k}$$-space approach of Kraichnan. A dielectric function is defined for arbitrary quadratically nonlinear systems, including the Navier–Stokes equation, and an algorithm for determining the form of$${\mathcal{D}}$$in the DIA is sketched. The independent insights of Kadomtsev and Kraichnan about the problem of the DIA with random Galilean invariance are described. The mixing-length formula for drift-wave saturation is discussed in the context of closures that include nonlinear noise (shielded by$${\mathcal{D}}$$). The role of$$R$$in the calculation of the symmetry-breaking (zonostrophic) instability of homogeneous turbulence to the generation of inhomogeneous mean flows is addressed. The second-order cumulant expansion and the stochastic structural stability theory are also discussed in that context. In conclusion, various historical research threads are mentioned and representative entry points to the literature are given. In addition, some outstanding conceptual issues are enumerated.

View Accepted Manuscript (DOE)

Research Organization:: Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)

Sponsoring Organization:: USDOE

OSTI ID:: 1256594

Report Number(s):: PPPL--5178; PII: S0022377815000756

Journal Information:: Journal of Plasma Physics, Journal Name: Journal of Plasma Physics Journal Issue: 06 Vol. 81; ISSN 0022-3778; ISSN applab

Publisher:: Cambridge University PressCopyright Statement

Country of Publication:: United States

Language:: English

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S3T stability of the homogeneous state of barotropic beta-plane turbulence Bakas, Nikolaos A.; Constantinou, Navid C.; Ioannou, Petros J. arXiv https://doi.org/10.48550/arxiv.1407.3354	text	January 2014
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Projection-operator methods for classical transport in magnetized plasmas. Part 2. Nonlinear response and the Burnett equations Krommes, John A. Journal of Plasma Physics, Vol. 84, Issue 6 https://doi.org/10.1017/s0022377818000892	journal	November 2018
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