Boundary conditions for plasma fluid models at the magnetic presheath entrance J. Loizu, P. Ricci, F.D. Halpern, S. Jolliet, A. Mosetto ´ Ecole Polytecnique F´ ed´ erale de Lausanne Centre de Recherches en Physique des Plasmas Association Euratom-Conf´ ed´ eration Suisse CH-1015 Lausanne, Suisse

Marseille, December 19th, 2012

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Boundary conditions

The problem of fluid codes

I

Quasi-neutrality ne ' ni is assumed I

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A drift ordering is usually adopted, d/dt  ωci , leading to the 0 ion drift approximation : v⊥i = vExB + ωbci × ddt vExB I

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This is violated in the Debye sheath

This is violated in the Magnetic presheath

Need B.C. that supply the sheath physics to fluid codes I I

To describe the main plasma dynamics To predict the particle and energy fluxes at the solid surface

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Boundary conditions

Simulations of the plasma-wall transition with ODISEE (a)

4

CP

e φ / Te

3 2 1

Total potential drop

MP DS

0

I

12

1D3V

14

16

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20

22

20

22

(b) 2

B = B0

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Ti  Te

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ρe . λD  ρs  λmfp < L

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Absorbing walls

vs / cs

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1.5 1

vsi

0.5 0

12

14

16

18 (c)

2 vx / cs

1.5

vIDA

1 0.5 0

vxi 12

14

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22

(d)

2

v

1.5 vy / cs

20

IDA

1 0.5

v

yi

0

12

14

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22

18

20

22

(e)

0.6 (ni−ne) / nse

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0.4 0.2 0 12

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14

16 s / ρs

Boundary conditions

A theory to describe the magnetic presheath entrance A theoretical framework has been developed, from which one can derive a complete set of B.C. at the MP entrance « 2φ 1 θTe − θφ 2 Te „ « 2φ v||e = cs ± exp (Λ − ηm ) − θφ + 2(θn + θTe ) Te « „ 1 ∂s φ = −cs ±1 + θn ± θTe ∂s v||i 2 „ « 1 n ±1 + θn ± θTe ∂s v||i ∂s n = − cs 2 „

v||i = cs

±1 + θn ∓

∂s Te = κT ∂s φ h i ω = − cos2 α (1 + θTe ) (∂s v||i )2 + cs (±1 + θn ± θTe /2) ∂s2 v||i

Effect of radial gradients ∂x n, ∂x φ, ∂x Te :

θA =

cs ∂x A 2 tan α A

[Loizu et al., Physics of Plasmas, 2012]

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Boundary conditions

SOL simulations with self-consistent boundary conditions at the magnetic presheath entrance

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Boundary conditions

Parallel currents are drawn by the limiter plates

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Boundary conditions

Currently studying

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Equilibrium profiles in the SOL

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Spontaneous toroidal plasma rotation driven by the sheath

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Effect of the limter position on the SOL width

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Code validation (TORPEX)

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Boundary conditions

Boundary conditions for plasma fluid models at the ...

The problem of fluid codes. ▻ Quasi-neutrality ne ≃ ni ... Need B.C. that supply the sheath physics to fluid codes. ▻ To describe the main ... + cs (±1 + θn ± θTe /2) ∂2 s v||i i. Effect of radial gradients ∂x n, ∂x φ, ∂x Te : θA = cs. 2 tan α. ∂x A. A. [Loizu et al., Physics of Plasmas, 2012]. Loizu, Ricci, Halpern, Jolliet, Mosetto.

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