2018
DOI: 10.1002/ctpp.201700168
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Turbulent heat transport in TOKAM3X edge plasma simulations

Abstract: The recent version of the 3D fluid code TOKAM3X, including self‐consistent variation of both electron and ion temperature, is used to investigate the properties of energy turbulent structures and heat transport. We also make a comparison with the results of the isothermal equivalent simulation. The studied regime is an L‐mode‐like regime where both particle and heat transport are dominated by turbulence with Γturb/Γtot > 80% and the turbulence features are found to be similar in isothermal and anisothermal mod… Show more

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Cited by 10 publications
(20 citation statements)
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“…The code is run here in its isothermal version and in a circular limited geometry. A non-isothermal version of the code exists as seen in [23] and is able to run into complex and realistic geometries [21]. This allows us in this first work to exclude geometrical and non isothermal effects for a step-by-step approach.…”
Section: The Tokam3x Modelmentioning
confidence: 99%
“…The code is run here in its isothermal version and in a circular limited geometry. A non-isothermal version of the code exists as seen in [23] and is able to run into complex and realistic geometries [21]. This allows us in this first work to exclude geometrical and non isothermal effects for a step-by-step approach.…”
Section: The Tokam3x Modelmentioning
confidence: 99%
“…[19]. Neumann conditions are applied at the radial inner and outer boundaries, and Bohm-Chodura boundary conditions are applied at the target plates [23].…”
Section: The Tokam3x Code For Fluid Turbulence Simulationsmentioning
confidence: 99%
“…In addition, the plasma collisionality is set to ν * ≡ ρ s /(c s τ e ) = 0.072, where τ e is the electron collision time. The choice of this value, approximately a factor of 5 larger than the typical experimental one, is driven by the need to keep computational costs reasonable [23], since small collisionality leads to smaller turbulent structures and requires grid with higher resolution. The impact of this parameter on blob dynamics will be further discussed in section 5.…”
Section: The Tokam3x Code For Fluid Turbulence Simulationsmentioning
confidence: 99%
“…We also remark that the terms of higher order in 1/Ω cD + 2 𝑑/𝑑𝑡 in the perpendicular velocity of D + 2 ions are neglected when writing ∇ • v D + 2 in the temperature equations, Eqs. ( 26) and (27), which is a necessary assumption in order to avoid explicit time derivatives arising from the polarization drift velocity, v pol,D + 2 . Nevertheless, all terms are considered in the divergence of the perpendicular velocity of D + ions in Eq.…”
Section: The Three-fluid Drift-reduced Braginskii Equationsmentioning
confidence: 99%
“…We note that dimensionless units are used in Eqs. (19)(20)(21)(22)(23)(24)(25)(26)(27) and in the rest of the paper. The densities, 𝑛 e , 𝑛 D + and 𝑛 D + 2 , are normalized to the reference value 𝑛 0 , while temperatures, 𝑇 e , 𝑇 D + and 𝑇 D + 2 , are normalized to the respective reference values, 𝑇 e0 , 𝑇 D + 0 and 𝑇 D + 2 0 = 𝑇 D + 0 , which are related by the dimensionless quantity 𝜏 = 𝑇 D + 0 /𝑇 𝑒0 .…”
Section: The Three-fluid Drift-reduced Braginskii Equationsmentioning
confidence: 99%