Radial transport of toroidal angular momentum in tokamaks
The radial flux of toroidal angular momentum is needed to determine tokamak intrinsic rotation profiles. Its computation requires knowledge of the gyrokinetic distribution functions and turbulent electrostatic potential to second-order in $\epsilon = \rho/L$, where $\rho$ is the ion Larmor radius an...
| Asıl Yazarlar: | , |
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| Materyal Türü: | Journal article |
| Baskı/Yayın Bilgisi: |
2014
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| _version_ | 1826267263495307264 |
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| author | Calvo, I Parra, F |
| author_facet | Calvo, I Parra, F |
| author_sort | Calvo, I |
| collection | OXFORD |
| description | The radial flux of toroidal angular momentum is needed to determine tokamak intrinsic rotation profiles. Its computation requires knowledge of the gyrokinetic distribution functions and turbulent electrostatic potential to second-order in $\epsilon = \rho/L$, where $\rho$ is the ion Larmor radius and $L$ is the variation length of the magnetic field. In this article, a complete set of equations to calculate the radial transport of toroidal angular momentum in any tokamak is presented. In particular, the $O(\epsilon^2)$ equations for the turbulent components of the distribution functions and electrostatic potential are given for the first time without assuming that the poloidal magnetic field over the magnetic field strength is small. |
| first_indexed | 2024-03-06T20:51:31Z |
| format | Journal article |
| id | oxford-uuid:37be2610-c4fb-45c6-95f4-7a8a7d7f20c3 |
| institution | University of Oxford |
| last_indexed | 2024-03-06T20:51:31Z |
| publishDate | 2014 |
| record_format | dspace |
| spelling | oxford-uuid:37be2610-c4fb-45c6-95f4-7a8a7d7f20c32022-03-26T13:45:49ZRadial transport of toroidal angular momentum in tokamaksJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:37be2610-c4fb-45c6-95f4-7a8a7d7f20c3Symplectic Elements at Oxford2014Calvo, IParra, FThe radial flux of toroidal angular momentum is needed to determine tokamak intrinsic rotation profiles. Its computation requires knowledge of the gyrokinetic distribution functions and turbulent electrostatic potential to second-order in $\epsilon = \rho/L$, where $\rho$ is the ion Larmor radius and $L$ is the variation length of the magnetic field. In this article, a complete set of equations to calculate the radial transport of toroidal angular momentum in any tokamak is presented. In particular, the $O(\epsilon^2)$ equations for the turbulent components of the distribution functions and electrostatic potential are given for the first time without assuming that the poloidal magnetic field over the magnetic field strength is small. |
| spellingShingle | Calvo, I Parra, F Radial transport of toroidal angular momentum in tokamaks |
| title | Radial transport of toroidal angular momentum in tokamaks |
| title_full | Radial transport of toroidal angular momentum in tokamaks |
| title_fullStr | Radial transport of toroidal angular momentum in tokamaks |
| title_full_unstemmed | Radial transport of toroidal angular momentum in tokamaks |
| title_short | Radial transport of toroidal angular momentum in tokamaks |
| title_sort | radial transport of toroidal angular momentum in tokamaks |
| work_keys_str_mv | AT calvoi radialtransportoftoroidalangularmomentumintokamaks AT parraf radialtransportoftoroidalangularmomentumintokamaks |