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Low Z Impurity Transport in Tokamaks. [Neoclassical Transport Theory].

Low Z Impurity Transport in Tokamaks. [Neoclassical Transport Theory]. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
Low Z impurity transport in tokamaks was simulated with a one-dimensional impurity transport model including both neoclassical and anomalous transport. The neoclassical fluxes are due to collisions between the background plasma and impurity ions as well as collisions between the various ionization states. The evaluation of the neoclassical fluxes takes into account the different collisionality regimes of the background plasma and the impurity ions. A limiter scrapeoff model is used to define the boundary conditions for the impurity ions in the plasma periphery. In order to account for the spectroscopic measurements of power radiated by the lower ionization states, fluxes due to anomalous transport are included. The sensitivity of the results to uncertainties in rate coefficients and plasma parameters in the periphery are investigated. The implications of the transport model for spectroscopic evaluation of impurity concentrations, impurity fluxes, and radiated power from line emission measurements are discussed.

Low Z Impurity Transport in Tokamaks. [Neoclassical Transport Theory].

Low Z Impurity Transport in Tokamaks. [Neoclassical Transport Theory]. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
Low Z impurity transport in tokamaks was simulated with a one-dimensional impurity transport model including both neoclassical and anomalous transport. The neoclassical fluxes are due to collisions between the background plasma and impurity ions as well as collisions between the various ionization states. The evaluation of the neoclassical fluxes takes into account the different collisionality regimes of the background plasma and the impurity ions. A limiter scrapeoff model is used to define the boundary conditions for the impurity ions in the plasma periphery. In order to account for the spectroscopic measurements of power radiated by the lower ionization states, fluxes due to anomalous transport are included. The sensitivity of the results to uncertainties in rate coefficients and plasma parameters in the periphery are investigated. The implications of the transport model for spectroscopic evaluation of impurity concentrations, impurity fluxes, and radiated power from line emission measurements are discussed.

Impurity Transport in Tokamaks

Impurity Transport in Tokamaks PDF Author: Paul Harding Rutherford
Publisher:
ISBN:
Category : Tokamaks
Languages : en
Pages : 19

Book Description


Low Z Impurity Transport in Tokamaks

Low Z Impurity Transport in Tokamaks PDF Author: R. J. Hawryluk
Publisher:
ISBN:
Category :
Languages : en
Pages : 79

Book Description


Impurity Transport in Tokamak Plasmas

Impurity Transport in Tokamak Plasmas PDF Author: Peter Donnel
Publisher:
ISBN:
Category :
Languages : en
Pages : 0

Book Description
Impurity transport is an issue of utmost importance for tokamaks. Indeed high-Z materials are only partially ionized in the plasma core, so that they can lead to prohibitive radiative losses even at low concentrations, and impact dramatically plasma performance and stability. On-axis accumulation of tungsten has been widely observed in tokamaks.While the very core impurity peaking is generally attributed to neoclassical effects, turbulent transport could well dominate in the gradient region at ITER relevant collisionality. Up to recently, first principles simulations of corresponding fluxes were performed with different dedicated codes, implicitly assuming that both transport channels are separable and therefore additive. The validity of this assumption is questionned. Simulations obtained with the gyrokinetic code GYSELA have shown clear evidences of a neoclassical-turbulence synergy for impurity transport and allowed the identification of a mechanism that underly this synergy.An analytical work allows to compute the level and the structure of the axisymmetric part of the electric potential knowing the turbulence intensity. Two mechanisms are found for the generation of poloidal asymmetries of the electric potential: flow compressibility and the ballooning of the turbulence. A new prediction for the neoclassical impurity flux in presence of large poloidal asymmetries and pressure anisotropies has been derived. A fair agreement has been found between the new theoretical prediction for neoclassical impurity flux and the results of a GYSELA simulation displaying large poloidal asymmetries and pressure anisotropies induced by the presence of turbulence.

Observation of Neoclassical-like Impurity Transport in the Q Less Than Or Equal to 1 Region of the PBX Tokamak

Observation of Neoclassical-like Impurity Transport in the Q Less Than Or Equal to 1 Region of the PBX Tokamak PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
Charge-dependent convective impurity transport is observed in the central core of PBX H-mode discharges by measuring radial profiles for both low- and high-Z intrinsic impurities in the presence of strong sawtooth activity. Transport coefficients are derived by simulating the data with a diffusive/convective transport model which includes an internal disruption model. The time evolving Z/sub eff/ profile and central metallic densities are fitted during the quiescent phase between internal disruptions to yield a diffusion coefficient of D = 1 x 103 cm2/s for all species and an inward convective speed of v = 2.2 x 102 (r/a) cm/s for oxygen and carbon and v = 1.1 x 103 (r/a) cm/s for metals. These transport coefficients are in quantitative agreement with simple cylindrical neoclassical estimates for the region within q less than or equal to 1. 17 refs., 4 figs.

Source Effects on Impurity and Heat Transport in a Tokamak

Source Effects on Impurity and Heat Transport in a Tokamak PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
A recently developed generalization of neoclassical theory is extended here to study heat flux contributions to impurity transport, as well as the heat fluxes themselves. The theory accounts for the first four source moments, with external drags, which has been studied previously with either fewer moments or restricted to a collisional plasma. Conditions are established for which a momentum source may be used to modify the particle and heat transport. In the course of this work, the particle and heat transport is evaluated for a two species plasma with arbitrary plasma geometry, beta, and collisionality.

Test of Local Transport Theory and Reduced Wall Impurity Influx with Highly Radiative Plasmas in the Tokamak Fusion Test Reactor

Test of Local Transport Theory and Reduced Wall Impurity Influx with Highly Radiative Plasmas in the Tokamak Fusion Test Reactor PDF Author: K. W. Hill
Publisher:
ISBN:
Category : Transport theory
Languages : en
Pages : 23

Book Description


Energy Research Abstracts

Energy Research Abstracts PDF Author:
Publisher:
ISBN:
Category : Power resources
Languages : en
Pages : 782

Book Description


Impurity Transport Theory for Text and ASDEX Tokamak. Final Report, September 25, 1989--November 24, 1990

Impurity Transport Theory for Text and ASDEX Tokamak. Final Report, September 25, 1989--November 24, 1990 PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 24

Book Description
Progress is reported in the following areas of plasma research: impurity and transport, neoclassical losses of fusion-produced energetic particles, and plasma turbulence.

Moment-equation Approach to Impurity Transport in Tokamaks

Moment-equation Approach to Impurity Transport in Tokamaks PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

Book Description
The purpose of this report is to overview neoclassical impurity transport through a fluid theory description, and experiments relevant to the topic. Three theoretical forms for particle transport are discussed here. The distinctions among these are mainly historical, as all can be included within the same framework, although the resulting transport effects differ greatly. The three, in order of historical development, are classical, Pfirsch-Schlueter, which introduced geometric effects, and neoclassical, which included long mean free path effects.