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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 6 (1999), S. 1397-1400 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A new type of toroidal condensation instability is found to dominate transport in the high-confinement-mode (H-mode) edge of tokamak plasmas when the temperature gradient is steeper than the density gradient. A particle pinch develops at the edge in agreement with experimental observations and the transport can be dominated by the ion or electron channel. © 1999 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 1 (1994), S. 809-814 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The threshold for parametric excitation of drift waves in a sheared slab geometry is calculated for a drift-wave pump which has a standing wave structure along the magnetic field, and the coupling is achieved by the Hasegawa–Mima vector product-type nonlinearity. The usual shear damping is counteracted by the parametric interaction which causes a reversal of the direction of the drift wave group velocity, and the nonlinear eigenvalue problem is solved analytically using Taylor's strong coupling approximation.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 9 (2002), S. 1217-1220 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The three-mode slab ion temperature gradient problem was considered. Starting from the drift kinetic equation with nonlinear term and diffusion, the hierarchy of fluid equations up to fourth moment was developed. As a closure, the nonlinear fluid closure by N. Mattor and S. Parker [Phys. Rev. Lett. 79, 3419 (1997)] was applied. Numerical solutions of the system of fluid equations have been obtained and analyzed. The time evolution of electrostatic potential shows that nonlinear fluid closure is able to capture particle trapping, which is important for fusion plasmas. Great attention was paid to studies of the role of diffusion. Diffusion here represents effects of background turbulence and can be described by a Fokker–Planck operator [A. Zagorodny and J. Weiland, Phys. Plasmas 6, 2359 (1999)]. The three wave system can be considered as a system of test waves in a turbulent background. This system can be used to study situations of varying partial coherence. © 2002 American Institute of Physics.
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  • 4
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The predictions of gyrokinetic and gyrofluid simulations of ion-temperature-gradient (ITG) instability and turbulence in tokamak plasmas as well as some tokamak plasma thermal transport models, which have been widely used for predicting the performance of the proposed International Thermonuclear Experimental Reactor (ITER) tokamak [Plasma Physics and Controlled Nuclear Fusion Research, 1996 (International Atomic Energy Agency, Vienna, 1997), Vol. 1, p. 3], are compared. These comparisons provide information on effects of differences in the physics content of the various models and on the fusion-relevant figures of merit of plasma performance predicted by the models. Many of the comparisons are undertaken for a simplified plasma model and geometry which is an idealization of the plasma conditions and geometry in a Doublet III-D [Plasma Physics and Controlled Nuclear Fusion Research, 1986 (International Atomic Energy Agency, Vienna, 1987), Vol. 1, p. 159] high confinement (H-mode) experiment. Most of the models show good agreements in their predictions and assumptions for the linear growth rates and frequencies. There are some differences associated with different equilibria. However, there are significant differences in the transport levels between the models. The causes of some of the differences are examined in some detail, with particular attention to numerical convergence in the turbulence simulations (with respect to simulation mesh size, system size and, for particle-based simulations, the particle number). The implications for predictions of fusion plasma performance are also discussed. © 2000 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 5 (1998), S. 3089-3100 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The influence of flow shear and curvature on toroidal drift modes has been studied for the case of strong inhomogeneity where the ballooning mode formalism does not apply. It has been found that flow curvature is often as important as the flow shear and may lead to complete cancellation of magnetic shear damping. The limit of validity of the ballooning mode formalism is explored. © 1998 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 5 (1998), S. 3669-3674 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Effects of ion temperature gradients on strong ballooning drift resistive edge modes are considered. The ion temperature perturbations are found to have a significant influence on the stability properties. In particular, the ion temperature gradient leads to a finite-Larmor radius stabilization of the strongest mode with an ideal growth rate for lower heating power than that required for stabilization due to the poloidal sheared rotation. © 1998 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 1 (1994), S. 1096-1097 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 8 (2001), S. 180-185 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Resistive edge modes in a shifted noncircular tokamak geometry are investigated in the electrostatic limit. The reduced Braghinskii equations are used as a model for the electrons and an advanced fluid model for the ions. An eigenvalue problem is derived from these equations which is solved numerically. It is found that the resistive ballooning modes are stabilized by plasma elongation for peaked density profiles. In addition, it is found that the resistive ηi-modes (ηi=Ln/LTi) may be either stabilized or destabilized by elongation depending on the collision frequency. © 2001 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 4 (1997), S. 690-695 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The influence of ion temperature fluctuations on the stability of resistive drift and ballooning modes is investigated using a two-fluid model. The eigenmode equations are derived and solved analytically in a low beta model equilibrium. Parameters relevant to low-confinement-mode (L-mode) edge plasmas from the Texas Experimental Tokamak (TEXT) [Phys. Fluids B 2, 2879 (1990)] are used. The resistive modes are found to be destabilized by ion temperature fluctuations over a broad range of mode numbers. The scaling of the growth rate with magnetic shear, ηi(Ln/LTi) and the mode number is elucidated. © 1997 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 777-780 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effect of a radially varying poloidal velocity field on the recently found radially extended toroidal drift waves [Connor et al., Phys. Rev. Lett. 70, 1803 (1993)] is investigated analytically. The role of velocity curvature (Vθ‘) is found to have robust effects on the radial mode structure of the mode. For a positive value of the curvature [usually found in the high-(H) mode edges] the radial mode envelope, similar to the sheared slab case, becomes fully outgoing. On the other hand, for a negative value of the curvature [usually observed in the low-(L) mode edges] the characteristics of conventional drift waves return back. The radial mode envelope reduces to a localized Gaussian shape and the mode can be unstable again for typical (magnetic) shear values in tokamaks. Velocity shear (Vθ') on the other hand is found to have a rather insignificant role both in determining the radial mode structure and the stability. © 1995 American Institute of Physics.
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