Dynamical nature of inviscid power law for two-dimensional turbulences and self-consistent spectrum and transport of plasma filaments
Abstract
On the basis of equal-time correlation theory (a non-perturbative approach) inviscid power laws of 2D isotropic plasma turbulences with one Lagrangian inviscid constant of motion are unambiguously solved by determining the dynamical characteristics. Two distinct types of induced transport, according to the divergence of the inverse correlation length in the inviscid limit, are revealed. This analysis also suggests a physically reasonable closure. The self-consistent system (a set of integral equations) for plasma filaments is investigated in detail, and is found to be a nonlinear differential eigenvalue problem for the diffusion coefficient D, with the Dyson-like (integral) equation playing the role of a boundary condition. This new type of transport is non-Bohm-like, and shows quasilinear behavior even in the strong turbulence regime. Physically, this behavior arises from a synchronization of the shrinking squared correlation length with the decorrelation time, for which the ``mixing-length`` breaks down. The shrinkage of correlation length is a characteristic pertaining to the new type of turbulence; its relationship with the turbulence observed in supershot regime on TFTR is commented on.
- Authors:
-
- International Centre for Theoretical Physics, Trieste (Italy)
- Texas Univ., Austin, TX (United States). Inst. for Fusion Studies
- Publication Date:
- Research Org.:
- Texas Univ., Austin, TX (United States). Inst. for Fusion Studies
- Sponsoring Org.:
- USDOE, Washington, DC (United States)
- OSTI Identifier:
- 10139394
- Report Number(s):
- DOE/ET/53088-647; IFSR-647
ON: DE94009425; BR: 39KG01000/AT0520240; TRN: 94:007522
- DOE Contract Number:
- FG05-80ET53088
- Resource Type:
- Technical Report
- Resource Relation:
- Other Information: PBD: Feb 1994
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; PLASMA; TURBULENCE; TWO-DIMENSIONAL CALCULATIONS; LAGRANGE EQUATIONS; TRANSPORT THEORY; 700370; PLASMA FLUID AND MHD PROPERTIES
Citation Formats
Zhang, Y.Z., and Mahajan, S.M. Dynamical nature of inviscid power law for two-dimensional turbulences and self-consistent spectrum and transport of plasma filaments. United States: N. p., 1994.
Web. doi:10.2172/10139394.
Zhang, Y.Z., & Mahajan, S.M. Dynamical nature of inviscid power law for two-dimensional turbulences and self-consistent spectrum and transport of plasma filaments. United States. doi:10.2172/10139394.
Zhang, Y.Z., and Mahajan, S.M. Tue .
"Dynamical nature of inviscid power law for two-dimensional turbulences and self-consistent spectrum and transport of plasma filaments". United States.
doi:10.2172/10139394. https://www.osti.gov/servlets/purl/10139394.
@article{osti_10139394,
title = {Dynamical nature of inviscid power law for two-dimensional turbulences and self-consistent spectrum and transport of plasma filaments},
author = {Zhang, Y.Z. and Mahajan, S.M.},
abstractNote = {On the basis of equal-time correlation theory (a non-perturbative approach) inviscid power laws of 2D isotropic plasma turbulences with one Lagrangian inviscid constant of motion are unambiguously solved by determining the dynamical characteristics. Two distinct types of induced transport, according to the divergence of the inverse correlation length in the inviscid limit, are revealed. This analysis also suggests a physically reasonable closure. The self-consistent system (a set of integral equations) for plasma filaments is investigated in detail, and is found to be a nonlinear differential eigenvalue problem for the diffusion coefficient D, with the Dyson-like (integral) equation playing the role of a boundary condition. This new type of transport is non-Bohm-like, and shows quasilinear behavior even in the strong turbulence regime. Physically, this behavior arises from a synchronization of the shrinking squared correlation length with the decorrelation time, for which the ``mixing-length`` breaks down. The shrinkage of correlation length is a characteristic pertaining to the new type of turbulence; its relationship with the turbulence observed in supershot regime on TFTR is commented on.},
doi = {10.2172/10139394},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Tue Feb 01 00:00:00 EST 1994},
month = {Tue Feb 01 00:00:00 EST 1994}
}
-
It has long been recognized that if an EBT-confined plasma could be maintained in the collisionless-ion regime, characterized by positive ambipolar potential and positive radial electric field, the particle loss rates could be reduced by a large factor. The extent to which the loss rate of energy could be reduced has not been as clearly determined, and has been investigated recently using a one-dimensional, time-dependent transport code developed for this purpose. We find that the energy confinement can be improved by roughly an order of magnitude by maintaining a positive radial electric field that increases monotonically with radius, giving amore »
-
Possibility for a self-consistent treatment of transport processes in a turbulent plasma
All commonly used models of plasma dynamics share a common flaw in their a priori validity. In particular, a solid foundation of plasma modelling on microscopic dynamics, as exists for moderately dilute gases, is obscured because of the difficulties inherent in the treatment of the potentially very important interplay between plasma waves and collisional processes. The present report briefly discusses the nature of these difficulties and presents a possible approach towards the establishment of a plasma theory founded on the microscopic particle dynamics. The essence of this approach is the realization that only discrete particle interactions can create correlations. Thesemore » -
Self-consistent solutions of the plasma transport equations in an axisymmetric toroidal system
A numerical method is presented for solving a recently derived reduced set of equations describing two-dimensional transport in tokamak plasmas. The formulation exploits the different diffusion time scales by dividing each time advancement step into two parts. In the first part, the one-dimensional surface averaged partial differential equations are advanced implicitly. In the second part, the two-dimensional generalized differential equation for the toroidal flux surface velocity is inverted directly. Accurate efficient solutions are obtained with only explicit terms coupling these two steps. Solutions are presented illustrating the validity and the accuracy of this method.