Alpha Particle Destabilization of the Toroidicity-induced Alfven Eigenmodes

Alpha Particle Destabilization of the Toroidicity-induced Alfven Eigenmodes PDF Author: C. Z. Cheng
Publisher:
ISBN:
Category :
Languages : en
Pages : 28

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Alpha Particle Destabilization of the Toroidicity-induced Alfven Eigenmodes

Alpha Particle Destabilization of the Toroidicity-induced Alfven Eigenmodes PDF Author: C. Z. Cheng
Publisher:
ISBN:
Category :
Languages : en
Pages : 28

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Alpha Particle Destabilization of the Toroidicity-induced Alfven Eigenmodes

Alpha Particle Destabilization of the Toroidicity-induced Alfven Eigenmodes PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 28

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Book Description
The high frequency, low mode number toroidicity-induced Alfven eigenmodes (TAE) are shown to be driven unstable by the circulating and/or trapped?-particles through the wave-particle resonances. Satisfying the resonance condition requires that the?-particle birth speed v{sub?} ≥ v{sub A}/2{vert bar}m-nq{vert bar}, where v{sub A} is the Alfven speed, m is the poloidal model number, and n is the toroidal mode number. To destabilize the TAE modes, the inverse Landau damping associated with the?-particle pressure gradient free energy must overcome the velocity space Landau damping due to both the?-particles and the core electrons and ions. The growth rate was studied analytically with a perturbative formula derived from the quadratic dispersion relation, and numerically with the aid of the NOVA-K code. Stability criteria in terms of the?-particle beta?{sub?},?-particle pressure gradient parameter (?{sub {asterisk}}/?{sub A}) (?{sub {asterisk}} is the?-particle diamagnetic drift frequency), and (v{sub {alpha}}/v{sub A}) parameters will be presented for TFTR, CIT, and ITER tokamaks. The volume averaged {alpha}-particle beta threshold for TAE instability also depends sensitively on the core electron and ion temperature. Typically the volume averaged {alpha}-particle beta threshold is in the order of 10−4. Typical growth rates of the n=1 TAE mode can be in the order of 10−2?{sub A}, where?{sub A}=v{sub A}/qR. Other types of global Alfven waves are stable in D-T tokamaks due to toroidal coupling effects.

Alpha Particle Losses from Toroidicity Induced Alfvén Eigenmodes

Alpha Particle Losses from Toroidicity Induced Alfvén Eigenmodes PDF Author: D. J. Sigmar
Publisher:
ISBN:
Category :
Languages : en
Pages : 43

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Nonlinear Evolution of the Alpha Particle Driven Toroidicity-induced Alfven Eigenmode

Nonlinear Evolution of the Alpha Particle Driven Toroidicity-induced Alfven Eigenmode PDF Author: Yanlin Wu
Publisher:
ISBN:
Category : Computer simulation
Languages : en
Pages : 34

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Evolution of the Alpha Particle Driven Toroidicity Induced Alfven Mode

Evolution of the Alpha Particle Driven Toroidicity Induced Alfven Mode PDF Author: C.Z. Cheng
Publisher:
ISBN:
Category : Alpha rays
Languages : en
Pages : 10

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Evolution of the Alpha Particle Driven Toroidicity Induced Alfven Mode

Evolution of the Alpha Particle Driven Toroidicity Induced Alfven Mode PDF Author: C. Z. Cheng
Publisher:
ISBN:
Category : Alpha rays
Languages : en
Pages : 10

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Energy Research Abstracts

Energy Research Abstracts PDF Author:
Publisher:
ISBN:
Category : Power resources
Languages : en
Pages : 464

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Experimental Aspects of Effects of High-energy Particles on Alfven Modes

Experimental Aspects of Effects of High-energy Particles on Alfven Modes PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 16

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Global Alfven modes are observed in a number of tokamaks, including DIII-D and TFTR. Instabilities occur during neutral-beam injection and during fast-wave ICRF heating, and may recently have been observed during alpha-particle heating. Identification of toroidicity-induced Alfven eigenmodes (TAE) is based primarily on the scaling of the real frequency of the mode. Other modes, including the beta-induced Alfven eigenmode (BAE), are also observed. The stability threshold of TAE modes agree (to within a factor of two) with theoretical predictions. Toroidal mode numbers of n = 2-6 are usually most unstable, as theoretically expected. Measurements of the poloidal and radial mode structure are consistent with theoretical predictions, but the uncertainties are large. Both TAE and BAE modes can cause large, concentrated losses of fast ions. Phenomenologically, beam-driven Alfven modes usually {open_quotes}saturate{close_quotes} through bursts that expel beam ions, while modes observed during ICPF heating approach a steady saturation amplitude.

Advanced Magnetohydrodynamics

Advanced Magnetohydrodynamics PDF Author: J. P. Goedbloed
Publisher: Cambridge University Press
ISBN: 1139487280
Category : Science
Languages : en
Pages : 651

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Book Description
Following on from the companion volume Principles of Magnetohydrodynamics, this textbook analyzes the applications of plasma physics to thermonuclear fusion and plasma astrophysics from the single viewpoint of MHD. This approach turns out to be ever more powerful when applied to streaming plasmas (the vast majority of visible matter in the Universe), toroidal plasmas (the most promising approach to fusion energy), and nonlinear dynamics (where it all comes together with modern computational techniques and extreme transonic and relativistic plasma flows). The textbook interweaves theory and explicit calculations of waves and instabilities of streaming plasmas in complex magnetic geometries. It is ideally suited to advanced undergraduate and graduate courses in plasma physics and astrophysics.

Destabilization of Tokamak Pressure-gradient Driven Instabilities by Energetic Alpha Populations

Destabilization of Tokamak Pressure-gradient Driven Instabilities by Energetic Alpha Populations PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 22

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Alpha particle populations can significantly alter existing MHD in stabilities in tokamaks through kinetic effects and coupling to otherwise stable shear Alfven waves. Here we consider resonances of the trapped alpha precessional drift with both the usual ballooning mode diamagnetic frequency ([omega]{sub *i}/2) and the toroidicity induced Alfven eigenmode (TAE). This is examined for noncircular tokamaks in the high-n ballooning limit using an isotropic alpha slowing down distribution and retaining the full energy and pitch angle dispersion in the alpha drift frequency. Applying this to CIT and ITER indicates that ballooning instabilities can persist at [Beta]'s below the ideal MHD threshold. These are especially dominated by the destabilization of the TAE mode. In addition, a hybrid fluid-particle approach for simulating alpha effects on pressure-gradient driven instabilities is described. 13 refs., 6 figs.