Abstract:This survey deals with research on plasma in toroidal systems with strong longitudinal fields (Tokamak devices).The author first of all considers the movement of single particles in these systems and then reviews the theoretical work on equilibrium, transport coefficients and plasma stability. The design of the various Tokamak devices is described, as are the methods of plasma diagnostics employed with them. The main experimental results are summarized and compared with theory. Possible methods of heating plas… Show more
“…It is a well-established fact that the dominant transport channel of the main ion species in the core region of tokamak devices is ion-temperature-gradient driven (ITG) turbulence. 1,2 Collisions in connection with the toroidal geometry of the magnetic guide field, however, provide another relevant channel: neoclassical transport. 3,4 In contrast to turbulent mechanisms, it does not possess a critical threshold for the driving pressure gradient and also provides a minimal flux level in transport barriers where turbulence is suppressed.…”
Neoclassical and turbulent transport in tokamaks have been studied extensively over the past decades, but their possible interaction remains largely an open question. The two are only truly independent if the length scales governing each of them are sufficiently separate, i.e. if the ratio ρ * between ion gyroradius and the pressure gradient scale length is small. This is not the case in particularly interesting regions such as transport barriers. Global simulations of collisional ion-temperature-gradient-driven microturbulence performed with the nonlinear global gyrokinetic code Gene are presented. In particular, comparisons are made between systems with and without neoclassical effects. In fixed-gradient simulations the modified radial electric field is shown to alter the zonal flow pattern such that a significant increase in turbulent transport is observed for ρ * 1/300. Furthermore, the dependency of the flux on the collisionality changes. In simulations with fixed power input we find that the presence of neoclassical effects decreases the frequency and amplitude of intermittent turbulent transport bursts (avalanches) and thus plays an important role for the self-organisation behaviour.
“…It is a well-established fact that the dominant transport channel of the main ion species in the core region of tokamak devices is ion-temperature-gradient driven (ITG) turbulence. 1,2 Collisions in connection with the toroidal geometry of the magnetic guide field, however, provide another relevant channel: neoclassical transport. 3,4 In contrast to turbulent mechanisms, it does not possess a critical threshold for the driving pressure gradient and also provides a minimal flux level in transport barriers where turbulence is suppressed.…”
Neoclassical and turbulent transport in tokamaks have been studied extensively over the past decades, but their possible interaction remains largely an open question. The two are only truly independent if the length scales governing each of them are sufficiently separate, i.e. if the ratio ρ * between ion gyroradius and the pressure gradient scale length is small. This is not the case in particularly interesting regions such as transport barriers. Global simulations of collisional ion-temperature-gradient-driven microturbulence performed with the nonlinear global gyrokinetic code Gene are presented. In particular, comparisons are made between systems with and without neoclassical effects. In fixed-gradient simulations the modified radial electric field is shown to alter the zonal flow pattern such that a significant increase in turbulent transport is observed for ρ * 1/300. Furthermore, the dependency of the flux on the collisionality changes. In simulations with fixed power input we find that the presence of neoclassical effects decreases the frequency and amplitude of intermittent turbulent transport bursts (avalanches) and thus plays an important role for the self-organisation behaviour.
“…The major emphasis in fusion research has been up to now on confining and heating a hydrogen plasma within closed nested magnetic sur faces in a toroidal vessel, such as in a tokamak ( Fig. 1) [8][9][10][11][12] or a stellarator ( Fig. 2) [13][14][15][16][17][18][19][20][21][22][23][24][25].…”
“…The atomic physics model we use i s t h e time-dependent corona model ,6 a1 though t h e code w i l l t r i v i a l l y generate steady-state corona model (corona equi 1 …”
Section: N Order T O Study T H E Temporal E V O L U T I O N O F I Mmentioning
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