Turbulent transport of impurities in 3D devices

Nuclear Fusion IOP Publishing 61:11 (2021) 116019

Authors:

Jm Garcia-Regana, M Barnes, I Calvo, A Gonzalez-Jerez, H Thienpondt, E Sanchez, Fi Parra, Da St-Onge

Abstract:

The evidence of a large diffusive turbulent contribution to the radial impurity transport in Wendelstein 7-X (W7-X) plasmas has been experimentally inferred during the first campaigns and numerically confirmed by means of gyrokinetic simulations with the code stella. In general, the absence of strong impurity accumulation during the initial W7-X campaigns is attributed to this diffusive term. Given the large variety of possible stellarator configurations, in the present work the diffusive contribution is also calculated in other stellarator plasmas. In particular, a numerical cross-device comparison is presented, where the diffusion (D) and convection (V) coefficients of carbon and iron impurities produced by ion-temperature-gradient (ITG) turbulence are obtained. The simulations have been performed for the helias W7-X, the heliotron LHD, the heliac TJ-II and the quasi-axisymmetric stellarator NCSX at the radial position r/a = 0.75. The results show that, although the size of D and V can differ across the four devices, inward convection is found for all of them. For W7-X, TJ-II and NCSX the two coefficients are comparable and the turbulent peaking factor is surprisingly similar. In LHD, appreciably weaker diffusive and convective impurity transport and significantly larger turbulent peaking factor, in comparison with the other three stellarators, are predicted. All this suggests that ITG turbulence, although not strongly, would lead to negative impurity density gradients in stellarators. Then, considering mixed ITG/trapped electron mode (TEM) turbulence for the specific case of W7-X, it has been quantitatively assessed to what degree pellet fueled reduced turbulence scenarios feature reduced turbulent transport of impurities as well. The results for trace iron impurities show that, although their turbulent transport is not entirely suppressed, a significant reduction of the convection and a stronger decrease of the diffusion term are found. Although the diffusion is still above neoclassical levels, the neoclassical convection would gain under such conditions a greater specific weight on the dynamics of impurities in comparison with standard ECRH scenarios without pellet fueling.

Binaries are softer than they seem: effects of an external potential on the scattering dynamics of binaries

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 508:1 (2021) 190-194

Authors:

Yonadav Barry Ginat, Hagai B Perets

Modes of a stellar system II: non-ergodic systems

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 507:2 (2021) 2562-2567

Authors:

Jun Yan Lau, James Binney

Modes of a stellar system I: Ergodic systems

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 507:2 (2021) 2241-2252

Authors:

Jun Yan Lau, James Binney

Stellar dynamics in the periodic cube

Monthly Notices of the Royal Astronomical Society Oxford University Press 507:4 (2021) 4840-4851

Abstract:

We use the problem of dynamical friction within the periodic cube to illustrate the application of perturbation theory in stellar dynamics, testing its predictions against measurements from N-body simulations. Our development is based on the explicitly time-dependent Volterra integral equation for the cube’s linear response, which avoids the subtleties encountered in analyses based on complex frequency. We obtain an expression for the self-consistent response of the cube to steady stirring by an external perturber. From this, we show how to obtain the familiar Chandrasekhar dynamical friction formula and construct an elementary derivation of the Lenard–Balescu equation for the secular quasi-linear evolution of an isolated cube composed of N equal-mass stars. We present an alternative expression for the (real-frequency) van Kampen modes of the cube and show explicitly how to decompose any linear perturbation of the cube into a superposition of such modes.