2011
DOI: 10.1088/1009-0630/13/4/22
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Calculation of Beam Intensity Distribution for the Neutral Beam Injection in EAST

Abstract: Theoretical beam intensity distribution is derived for the neutral-beam-injection ion source with a multi-slot extraction in EAST. The beam intensity profile, both along and perpendicular to the injecting direction and the beam power deposition to the inner elements in the neutral beam injector (NBI) are evaluated. The results indicate that the transverse beam intensity is much higher than the longitudinal one. This study could provide information for the design of vacuum system, structure of inner elements an… Show more

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Cited by 12 publications
(4 citation statements)
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“…The prediction and expansion of divertor power footprint widths are the main tasks for SOL physics research. Experimental studies on the SOL heat flux width have been carried out on most of the current tokamaks [5][6][7][8][9][10][11][12][13][14][15]. The basic finding is the negative dependence of λ q on I p [11][12][13][14][15], which is consistent with the heuristic drift-based model proposed by Goldston [16], indicating that λ q would narrow to about 1 mm when extrapolated to ITER [11].…”
Section: Introductionsupporting
confidence: 71%
“…The prediction and expansion of divertor power footprint widths are the main tasks for SOL physics research. Experimental studies on the SOL heat flux width have been carried out on most of the current tokamaks [5][6][7][8][9][10][11][12][13][14][15]. The basic finding is the negative dependence of λ q on I p [11][12][13][14][15], which is consistent with the heuristic drift-based model proposed by Goldston [16], indicating that λ q would narrow to about 1 mm when extrapolated to ITER [11].…”
Section: Introductionsupporting
confidence: 71%
“…As mentioned in section-2, the grid set in the ROBIN device is segmented and tilted with an angle θ = 0.873 • with the vertical(y-axis) towards the beam(z-axis) axis. Individual grid segments are treated as tilted axes with respect to the lab frame and center of the GG as the origin [11]. The transformed axes for both top and bottom grid half were obtained and used as inputs for the equation-2.…”
Section: Beam Modelmentioning
confidence: 99%
“…Then, using the random number, the location of one simulation particle is determined. Through this method, the distribution of simulated particle will meet the beam intensity distribution formula [16]. The validity of the simulation is determined by judging the simulated particle within the beam cross section.…”
Section: D Dsmc Modelingmentioning
confidence: 99%