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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

Prof Michael Barnes

Professor in Theoretical Physics

Sub department

  • Rudolf Peierls Centre for Theoretical Physics

Research groups

  • Theoretical astrophysics and plasma physics at RPC
michael.barnes@physics.ox.ac.uk
Telephone: 01865 (2)73960
Rudolf Peierls Centre for Theoretical Physics, room 50.10
  • About
  • Publications

Linearized Model Fokker-Planck Collision Operators for Gyrokinetic Simulations, II. Numerics

Phys. Plasmas 16 (2008) 072107

Authors:

M Barnes, IG Abel, T Tatsuno, AA Schekochihin, SC Cowley, W Dorland

Linearized model Fokker-Planck collision operators for gyrokinetic simulations. I. Theory

Physics of Plasmas 15 (2008) 122509

Authors:

IG Abel, M Barnes, SC Cowley, W Dorland, AA Schekochihin

Model Collision Operators for Numerical Gyrokinetics

THEORY OF FUSION PLASMAS 1069 (2008) 233-+

Authors:

IG Abel, M Barnes, SC Cowley, W Dorland, GW Hammett, AA Schekochihin, T Tatsuno

Gyrokinetic linear theory of the entropy mode in a Z pinch

Physics of Plasmas AIP Publishing 13:6 (2006) 062102

Authors:

Paolo Ricci, BN Rogers, W Dorland, M Barnes

Collisionality scaling of the electron heat flux in ETG turbulence

Plasma Physics and Controlled Fusion IOP Publishing: Hybrid Open Access

Authors:

GJ Colyer, AA Schekochihin, FI Parra, CM Roach, MA Barnes, Y-C Ghim, W Dorland

Abstract:

In electrostatic simulations of MAST plasma at electron-gyroradius scales, using the local flux-tube gyrokinetic code GS2 with adiabatic ions, we find that the long-time saturated electron heat flux (the level most relevant to energy transport) decreases as the electron collisionality decreases. At early simulation times, the heat flux "quasi-saturates" without any strong dependence on collisionality, and with the turbulence dominated by streamer-like radially elongated structures. However, the zonal fluctuation component continues to grow slowly until much later times, eventually leading to a new saturated state dominated by zonal modes and with the heat flux proportional to the collision rate, in approximate agreement with the experimentally observed collisionality scaling of the energy confinement in MAST. We outline an explanation of this effect based on a model of ETG turbulence dominated by zonal-nonzonal interactions and on an analytically derived scaling of the zonal-mode damping rate with the electron-ion collisionality. Improved energy confinement with decreasing collisionality is favourable towards the performance of future, hotter devices.

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