CUTIE: Difference between revisions
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the electrostatic potential (Φ) and the parallel vector potential (Ψ). | the electrostatic potential (Φ) and the parallel vector potential (Ψ). | ||
The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time. | The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time. | ||
[[File:CUTIE.jpg|265px|thumb|right|Density | [[File:CUTIE.jpg|265px|thumb|right|Density fluctuations in a CUTIE simulation (from <ref name="cutie"/>)]] | ||
The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the [[Flux surface|flux surface]] averaged quantities and the turbulence in a self-consistent manner; | The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the [[Flux surface|flux surface]] averaged quantities and the turbulence in a self-consistent manner; |
Revision as of 13:15, 4 December 2009
CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma. [1] [2] [3] [4] The large aspect ratio tokamak ordering is used (R/a >> 1), and Bp << Btor, β << 1. The plasma modelled consists of electrons and a single ion species. Quasi-neutrality (ne ≈ ni) is assumed. The species are locally Maxwellian, but Te ≠ Ti . Particle and energy sources, and a radial profile of Zeff are imposed. Conservation equations for particles, energy, and momentum are solved to obtain the electron density (n), electron and ion temperatures (Te, Ti), the ion fluid velocty (v), the electrostatic potential (Φ) and the parallel vector potential (Ψ). The poloidal magnetic field (and consequently the safety factor, q) evolves in time.
The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the flux surface averaged quantities and the turbulence in a self-consistent manner; profile gradients interact non-linearly with the turbulence. Thus, the code is capable of modelling the following fluid-like modes: linear and non-linear shear Alfvén waves, slow magneto-acoustic modes, drift-tearing modes, ballooning modes (ideal and viscoresistive), and the fluid branch of the ion temperature gradient (ITG) instability. The code contains sufficient mechanisms for the generation of sheared flow by turbulence and produces a spontaneous confinement transition similar to the L-H transition in experimental devices.
Code history
Current installations
The code is being used at:
- Culham Centre for Fusion Energy, Culham, UK (code origin)
- Laboratorio Nacional de Fusión, CIEMAT, Madrid, Spain
References
- ↑ A. Thyagaraja, Plasma Phys. Control. Fusion 42 (2000) B255
- ↑ A. Thyagaraja, P.J. Knight, and N. Loureiro, Eur. Journal of Mech. B/Fluids 23 (2004) 475
- ↑ M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, Phys. Rev. Lett. 94 (2005) 035002
- ↑ 4.0 4.1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, Phys. Plasmas 12 (2005) 090907