Plasmadynamics Conference 1966
DOI: 10.2514/6.1966-152
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An experimental study of a neutral point in a plasma

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Cited by 7 publications
(10 citation statements)
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“…We can then introduce the isotropic ion and electron temperatures Tj and T e and write Uj = f kT { , U e = I kT e and p = p, + p e = nk (Tj + T e ) = f nU with good approximation. It is then also convenient to use expressions (26) and (27) in the balance equations (30) - (32), and to write div^ = Vp + divl and f: vv* = p divv* + % :VV\…”
Section: 2 the Plasma Fluid Equationsmentioning
confidence: 99%
“…We can then introduce the isotropic ion and electron temperatures Tj and T e and write Uj = f kT { , U e = I kT e and p = p, + p e = nk (Tj + T e ) = f nU with good approximation. It is then also convenient to use expressions (26) and (27) in the balance equations (30) - (32), and to write div^ = Vp + divl and f: vv* = p divv* + % :VV\…”
Section: 2 the Plasma Fluid Equationsmentioning
confidence: 99%
“…As noted previously, testing the validity of the field flattening assumption became a primary objective of the DIPD experiments, and according to preliminary reports (Bratenahl & Hirsch 1966; see also Hess 1968) the field flattening, neutral sheet and boundary layer concepts appeared to have been confirmed. However, with more complete information this earlier conclusion proved completely false (BY).…”
Section: Critique Of Traditional Approachmentioning
confidence: 72%
“…The first preliminary results of the DIPD program were reported in 1965 (Bratenahl and Hirsch, 1966). In 1969, the project was moved from JPL to UC Riverside and there the work continued until 1980.…”
Section: Reconnection Experimentsmentioning
confidence: 99%