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Published on: February 27, 2016
Thermodynamic potential in local turbulence simulations
1Centre for Interdisciplinary Plasma Science, Max-Planck Institut für Plasmaphysik, EURATOM-IPP Association, D-85748 Garching, Germany.
Energy conservation is maintained in reduced tokamak turbulence models. However, new constraints on velocity and field fluctuations can be found using the generalized grand canonical potential, applicable to Boltzmann, gyrokinetic, and fluid equations.
Area of Science:
- Plasma Physics
- Computational Fluid Dynamics
- Thermodynamics
Background:
- Reduced local equations are common in tokamak turbulence computations.
- In these models, kinetic and magnetic energy are often neglected in the energy functional.
- This leads to a lack of constraints on velocity and field fluctuations.
Purpose of the Study:
- To identify conserved quantities beyond the standard energy functional in reduced plasma models.
- To derive new constraints on velocity and magnetic field fluctuations.
- To demonstrate the applicability of these constraints across different kinetic and fluid models.
Main Methods:
- Utilized the generalized grand canonical potential as a conserved quantity.
- Applied this potential to reduced local equations relevant to tokamak turbulence.
- Examined the conservation properties for Boltzmann, gyrokinetic, and fluid equations.
Main Results:
- The generalized grand canonical potential is conserved in reversible processes within these reduced models.
- This conserved potential provides constraints on velocity and field fluctuations that are not captured by the energy functional alone.
- The method is shown to be effective for Boltzmann, gyrokinetic, and fluid descriptions.
Conclusions:
- The generalized grand canonical potential offers a valuable tool for analyzing fluctuations in reduced plasma physics models.
- It provides a more complete set of conserved quantities, enhancing the accuracy of turbulence simulations.
- This approach is broadly applicable to various kinetic and fluid plasma models.
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