共 1 条
A pulsed high-current plasma beam under external and self-induced magnetic confinement in a linear device
被引:2
|作者:
Zheng, X. J.
[1
,2
]
Gou, F. J.
[3
]
Zhou, Y.
[4
]
Wang, H. X.
[4
]
Wallace, A. C.
[2
]
Wang, H. B.
[1
]
Huang, Z. H.
[4
]
Ji, X. Q.
[4
]
Liang, S. Y.
[4
]
Liu, W.
[2
]
Feng, Y. T.
[1
]
Deng, B. Q.
[4
]
机构:
[1] Hope Innovat Shanghai Inc, Shanghai, Peoples R China
[2] Hope Innovat Inc, Mississauga, ON L4W 0A5, Canada
[3] Sichuan Univ, Chengdu 610064, Sichuan, Peoples R China
[4] Southwestern Inst Phys, Chengdu 610041, Sichuan, Peoples R China
基金:
中国国家自然科学基金;
关键词:
experimental verification;
self-induced magnetic confinement;
linear device;
magnetic inertial confinement fusion;
MICF;
astrophysics;
RADIATION;
FUSION;
D O I:
10.1088/1361-6587/ab3618
中图分类号:
O35 [流体力学];
O53 [等离子体物理学];
学科分类号:
070204 ;
080103 ;
080704 ;
摘要:
The previously developed governing equations for Magnetic Inertial Confinement Fusion, which combines the advantages of both magnetic and inertial confinement approaches, are improved to analyse a plasma beam in a linear device assisted by an external magnetic field. The equations are applied to simulate a steady state plasma beam sustained by a DC power supply as well as a transient beam generated by a separate pulsed discharge superimposed on the steady-state plasma. The calculated increase of plasma density during the pulse from the steady-state condition is compared with measurements using a laser interferometer at a relatively low voltage supply of 150 V for the pulses. The numerical and test results are found to agree within 20%. When the voltage rises, plasma instability is observed. This issue is inherent due to the use of a solid positive target electrode that blocks the plasma flow in the axial direction. As a remedy, additional tests were carried out using a hollow target electrode in a two-circuit design (to permit free gas flow in the axial direction) by replacing the DC power with transient, pulsed, high-voltage sources for plasma initiation and beam formation. These enhancements were successful in suppressing the instabilities. The peak plasma density was calculated at similar to 10(22) m(-3) for confinement times of the order of 1 ms. These results lie between the extremes for the current leading approaches yet are achieved for a more compact and inexpensive linear device.
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