| On Plasma Rotation Induced by Traveling Fast Alfvin Waves | |
| Perkins, F.W. ; White, R.B. ; Chan, and V.S. | |
| Princeton University. Plasma Physics Laboratory. | |
| 关键词: Ion Cyclotron-Resonance; Wavelengths; 70 Plasma Physics And Fusion Technology; Travelling Waves; Tokamak Devices; | |
| DOI : 10.2172/788205 RP-ID : PPPL-3605 RP-ID : AC02-76CH03073 RP-ID : 788205 |
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| 美国|英语 | |
| 来源: UNT Digital Library | |
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【 摘 要 】
Absorption of fast Alfven waves by the minority fundamental ion-cyclotron resonance, coupled with finite banana width physics, generates torque distributions and ultimately rotational shear layers in the bulk plasma, even when the toroidal wavenumber k(subscript ''phi'') = n/R of the fast wave vanishes (n=0) and cyclotron absorption introduces no angular momentum nor canonical angular momentum [F.W. Perkins, R.B. White, P.T. Bonoli, and V.S. Chan, Phys. Plasmas 8 (2001) 2181]. The present work extends these results to travelling waves with non-zero n where heating directly introduces angular momentum. Since tokamak fast-wave antennas have approximately one wavelength per toroidal field coil, the toroidal mode number n lies in the range n = 10-20, independent of machine size. A zero-dimensional analysis shows that the rotation rate arising from direct torque is comparable to that of the rotational shear layer and has the same scaling. Nondimensional rotation profiles for n = (-10, 10) show modest changes from the n = 0 case in the expected direction. For a balanced antenna spectrum, the nondimensional rotational profile (averaged over n = -10, 10) lies quite close to the n = 0 profile.
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| Files | Size | Format | View |
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| 788205.pdf | 265KB |
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