Steady-state Fully Non-inductive Operation with Electron Cyclotron Current Drive and Current Profile Control in the Tokamak À Configuration Variable TCV

Steady-state Fully Non-inductive Operation with Electron Cyclotron Current Drive and Current Profile Control in the Tokamak À Configuration Variable TCV PDF Author: APS Division of Plasma Physics. Annual Meeting
Publisher:
ISBN:
Category :
Languages : en
Pages : 15

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Steady-state Fully Non-inductive Operation with Electron Cyclotron Current Drive and Current Profile Control in the Tokamak À Configuration Variable TCV

Steady-state Fully Non-inductive Operation with Electron Cyclotron Current Drive and Current Profile Control in the Tokamak À Configuration Variable TCV PDF Author: APS Division of Plasma Physics. Annual Meeting
Publisher:
ISBN:
Category :
Languages : en
Pages : 15

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أفحكم الجاهلية يبغون

أفحكم الجاهلية يبغون PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Quasi-steady-state Improved Central Confinement in the TCV Tokamak with Electron Cyclotron Heating and Current Drive

Quasi-steady-state Improved Central Confinement in the TCV Tokamak with Electron Cyclotron Heating and Current Drive PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 7

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HIGH PERFORMANCE ADVANCED TOKAMAK REGIMES FOR NEXT-STEP EXPERIMENTS.

HIGH PERFORMANCE ADVANCED TOKAMAK REGIMES FOR NEXT-STEP EXPERIMENTS. PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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OAK-B135 Advanced Tokamak (AT) research in DIII-D seeks to provide a scientific basis for steady-state high performance operation in future devices. These regimes require high toroidal beta to maximize fusion output and poloidal beta to maximize the self-driven bootstrap current. Achieving these conditions requires integrated, simultaneous control of the current and pressure profiles, and active magnetohydrodynamic (MHD) stability control. The building blocks for AT operation are in hand. Resistive wall mode stabilization via plasma rotation and active feedback with non-axisymmetric coils allows routine operation above the no-wall beta limit. Neoclassical tearing modes are stabilized by active feedback control of localized electron cyclotron current drive (ECCD). Plasma shaping and profile control provide further improvements. Under these conditions, bootstrap supplies most of the current. Steady-state operation requires replacing the remaining Ohmic current, mostly located near the half-radius, with noninductive external sources. In DIII-D this current is provided by ECCD, and nearly stationary AT discharges have been sustained with little remaining Ohmic current. Fast wave current drive is being developed to control the central magnetic shear. Density control, with divertor cryopumps, of AT discharges with edge localized moding (ELMing) H-mode edges facilitates high current drive efficiency at reactor relevant collisionalities. A sophisticated plasma control system allows integrated control of these elements. Close coupling between modeling and experiment is key to understanding the separate elements, their complex nonlinear interactions, and their integration into self-consistent high performance scenarios. Progress on this development, and its implications for next-step devices, will be illustrated by results of recent experiment and simulation efforts.

Steady-state Current Drive in Tokamaks Workshop Summary

Steady-state Current Drive in Tokamaks Workshop Summary PDF Author: United States. Department of Energy. Division of Magnetic Confinement Systems
Publisher:
ISBN:
Category : Fusion reactors
Languages : en
Pages : 124

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A Non-inductively Driven Steady State Tokamak Reactor

A Non-inductively Driven Steady State Tokamak Reactor PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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The physics and engineering guidelines for the ITER device are shown to lead to viable and attractive operating points for a steady state tokamak power reactor. Non-inductive current drive is provided in steady state by high energy neutral beam injection in the plasma core, lower hybrid slow waves in the outer regions of the plasma and bootstrap current. Plasma gain Q (/equivalent to/fusion power/input power) in excess of 20 and average neutron wall loading, GAMMA approx. 2.0 MW/m2 are predicted in a device with major radius, R0 = 7.5 m and minor radius, a = 2.8 m. 15 refs., 3 figs., 3 tabs.

Magnetic Fusion Technology

Magnetic Fusion Technology PDF Author: Thomas J. Dolan
Publisher: Springer Science & Business Media
ISBN: 1447155564
Category : Technology & Engineering
Languages : en
Pages : 816

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Book Description
Magnetic Fusion Technology describes the technologies that are required for successful development of nuclear fusion power plants using strong magnetic fields. These technologies include: • magnet systems, • plasma heating systems, • control systems, • energy conversion systems, • advanced materials development, • vacuum systems, • cryogenic systems, • plasma diagnostics, • safety systems, and • power plant design studies. Magnetic Fusion Technology will be useful to students and to specialists working in energy research.

Electron Cyclotron Current Drive and Suprathermal Electron Dynamics in the TCV Tokamak

Electron Cyclotron Current Drive and Suprathermal Electron Dynamics in the TCV Tokamak PDF Author: S. Coda
Publisher:
ISBN:
Category :
Languages : en
Pages : 19

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A Non-inductively Driven Tokamak Reactor Based on ITER.

A Non-inductively Driven Tokamak Reactor Based on ITER. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages :

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Book Description
The physics and engineering guidelines for the ITER device are shown to lead to viable physics operating points for a steady state tokamak power reactor. Non-inductive current drive is provided in steady state by high energy neutral beam injection in the plasma core, lower hybrid slow waves in the outer regions of the plasma and bootstrap current. Plasma gain Q(/equivalent to/fusion power/input power) in excess of 20 and average neutron wall loading, GAMMA approx. 2.0 MW/m2 are predicted in a device with major radius, R0 = 7.5 m and minor radius, a = 2.8 m. 15 refs., 3 figs., 3 tabs.

ELECTRON CYCLOTRON CURRENT DRIVE EFFICIENCY IN GENERAL TOKAMAK GEOMETRY.

ELECTRON CYCLOTRON CURRENT DRIVE EFFICIENCY IN GENERAL TOKAMAK GEOMETRY. PDF Author:
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ISBN:
Category :
Languages : en
Pages :

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Green's-function techniques are used to calculate electron cyclotron current drive (ECCD) efficiency in general tokamak geometry in the low-collisionality regime. Fully relativistic electron dynamics is employed in the theoretical formulation. The high-velocity collision model is used to model Coulomb collisions and a simplified quasi-linear rf diffusion operator describes wave-particle interactions. The approximate analytic solutions which are benchmarked with a widely used ECCD model, facilitate time-dependent simulations of tokamak operational scenarios using the non-inductive current drive of electron cyclotron waves.