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Collisional stabilisation of trapped electron modes in tokamaks: pitch angle scattering vs energy scattering

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Collisional stabilisation of trapped electron modes in tokamaks: pitch angle scattering vs energy scattering

P. Manas

1

, Y. Camenen

1

, S. Benkadda

1

, W.A. Hornsby

2

, A.G. Peeters

2

1

Aix-Marseille Universit´e, CNRS, PIIM UMR7345, 13397 Marseille, France

2

Department of Physics, University of Bayreuth, 95440 Bayreuth, Germany

In tokamaks, trapped electron modes (TEM) are known for long to be stabilised by collisions.

Indeed, by de-trapping electrons, collisions prevent the resonance between the bouncing motion of the trapped electrons and the mode (see e.g. [1, 2]). Collisions are described by the Landau colli- sion operator [4] which satisfies the H-theorem, conservation of particle, momentum and energy.

The test particle part (collisions with a Maxwellian background), can be written as [5]:

C

ab

= (f

a

, f

b0

) = ν

Dab

L(f

a

) + 1 v

2

∂v

 v

3

 m

a

m

a

+ m

b

ν

sab

f

a

+ 1

2 ν

kab

v ∂f

a

∂v



(1) with ν

sab

the slowing down frequency, ν

Dab

the deflection frequency and ν

kab

the parallel velocity diffusion frequency.

Many turbulent transport studies are carried out with a simplified test particle collision opera- tor which only takes into account the pitch angle scattering (i.e ν

Dab

L) as it is sufficient to ob- tain TEM stabilisation by collisional detrapping. However, a full test particle operator includ- ing energy scattering can also play a non negligible role in the stabilisation of TEM. Simula- tions were performed with the gyrokinetic code GKW [3] which solves the gyro-averaged Vlasov equation including pitch angle scattering and energy scattering in the linearised Landau operator:

C

ab

(f

a

, f

b0

) + C

ab

(f

a0

, f

b

). The importance of conservation properties through a well defined field particle operator is emphasized. It is shown that energy scattering enhances the stabilisation of TEM, especially when the mode frequency is low. This impacts the ITG/TEM transition and the subsequent modifications of the particle, momentum and heat fluxes.

References

[1] M.A. Beer, Ph.D. thesis, Pinceton University (1995)

[2] F.Y. Gang and P.H. Diamond, Phys. Fluids B 2, 2976 (1990)

[3] A.G. Peeters, Y. Camenen, F.J. Casson, W.A. Hornsby, A.P. Snodin, D. Strintzi, G. Szepezi, Computer Physics Communications 180, 2650 (2009)

[4] L.D. Landau, Physikalische Zeitschrift der Sowjetunion 10, 154 (1936)

[5] P. Helander, D.J. Sigmar, Collisional transport in magnetized plasmas

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