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Interplay between toroidal rotation and flow shear in turbulence stabilisation
The interplay between toroidal rotation u, parallel flow shear u′, and perpendicular flow shear γE in the stabilisation of tokamak turbulence is investigated in non-linear flux-tube gyrokinetic simulations. The simulations are performed for a reference L-mode DIII-D plasma (the so-called shortfall c...
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Published in: | Physics of plasmas 2016-02, Vol.23 (2) |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The interplay between toroidal rotation u, parallel flow shear u′, and perpendicular flow shear γE
in the stabilisation of tokamak turbulence is investigated in non-linear flux-tube gyrokinetic simulations. The simulations are performed for a reference L-mode DIII-D plasma (the so-called shortfall case) at
r
/
a
=
0.8
, varying the flow parameters around their nominal values. Depending on the respective signs of u, u′, and γE
, turbulence is found to be enhanced, reduced, or unchanged. When the coupling is favorable, the overall effect on the non-linear heat fluxes can be very large, even at moderate flow values. The ion heat flux is, for instance, decreased by a factor of 3 when the direction of the parallel flow shear is reversed with respect to its nominal value. Even more surprising, keeping u′ and γE
at their nominal values, the ion heat flux decreases by more than 50% when the toroidal flow is reversed. The relevance of this mechanism in the experiments which depends on the ability to decouple u, u′, and γE
is discussed. The interplay between u and u′ observed in the non-linear simulations qualitatively follows the linear stability results and is interpreted in the frame of a simple fluid model. |
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ISSN: | 1070-664X 1089-7674 |
DOI: | 10.1063/1.4942422 |