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FORCE DE LAPLACE EN R ´ EGIME DIFFUSIF 183 et apr`es une transform´ee de Fourier,

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C.5. FORCE DE LAPLACE EN R ´ EGIME DIFFUSIF 183 et apr`es une transform´ee de Fourier,

− → b = i − → k .−→ B ηk2 − → v (C.20) La force de Laplace −→ J ×−→ B s’´ecrit alors : − → J ×−→ B ' −→ ∇∧B  ×B +−→ ∇∧b ×B (C.21)

et de C.20 on peut obtenir l’effet de la force de Laplace associ´ee aux courants de petite ´ echelle. −→ ∇∧b ×B = − −→ B .−→ k 2 ηk2 − → v + −→ B .−→ v  −→ B .−→ k  ηk2 − → k (C.22)

qui ne d´epend pas de l’´echelle ! Elle peut ˆetre vue comme une force de freinage magn´etique anisotrope −γ−→

u et une force de pression magn´etique. La force de freinage est exactement celle obtenue par Braginsky (1990). Cette expression montre que

– si −→

B est parall`ele `a −→

v (ce qui implique que −→

B est orthogonal `a −→

k ) il n’y a pas de friction ;

– pour −→

B orthogonal `a−→

v , la pression magn´etique est nulle ; – et pour −→

B orthogonal `a−→

k , la force de Laplace s’annule, mˆeme si−→

v croise des lignes de champ.

Comme nous travaillons avec l’´equation de vorticit´e, nous avons besoin du rotationnel de cette force, qui est simplement

− → ∇∧ −→ B .−→ ∇ −→ b = − −→ B .−→ k 2 ηk2 − → ω (C.23)

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