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Volumn 8, Issue 5 II, 2001, Pages 1916-1928

Experimental study of ion heating and acceleration during magnetic reconnection

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Indexed keywords


EID: 0035333446     PISSN: 1070664X     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.1356737     Document Type: Article
Times cited : (49)

References (39)
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    • note
    • Z.
  • 20
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    • note
    • TF/PF bank voltages = 13/11 kV; TF/PF bank capacitances = 120 μF, TF/PF trigger = 180/270 μs; TF/PF crowbar (w/reconnection) = 270/290 μs; TF/PF crowbar (w/o reconnection): 270/220 (null-helicity), 270/200 (co-helicity); initial He gas pressure = 6 mT.
  • 21
    • 33744674646 scopus 로고    scopus 로고
    • note
    • During plasma formation, coil current is increasing and private flux is reconnected into public flux, establishing a reconnection layer elongated in the R direction. This is push reconnection.
  • 22
    • 33744627418 scopus 로고    scopus 로고
    • note
    • θ after t = 270 μs is likely due to the plasma pinching off from one flux-core.
  • 24
    • 33744648346 scopus 로고    scopus 로고
    • note
    • High downstream pressure may arise due to pressure equalization along field lines which connect the reconnection region to the downstream regions near the flux cores. The thermal transit time of 15 eV electrons along this path is ∼ 1 μs, meaning that buildup of downstream pressure due to recirculating electrons over 20-30 μs is plausible.
  • 25
    • 33744657978 scopus 로고    scopus 로고
    • note
    • Z drift on the order of 30 km/s.
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    • edited by M. A. Leontovich (Consultants Bureau, New York)
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  • 29
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    • note
    • TF/PF bank voltages = 11/9, 12/10, 12.5/10.5, 13/11, 14/12 kV.
  • 35
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    • P. C. Stangeby, Phys. Fluids 27, 2699 (1984); K. S. Chung, J. Appl. Phys. 69, 3451 (1990); B. J. Peterson, J. N. Talmadge, D. T. Anderson, F. S. B. Anderson, and J. L. Shobet, Rev. Sci. Instrum. 65, 2599 (1994).
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    • Theory of Spherical and Cylindrical Probes in a Collisionless Maxwellian Plasma at Rest
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.