1993
DOI: 10.1109/27.249653
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Plasma filamentation and upper pressure limit for neutron yield in a DPF device

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Cited by 14 publications
(13 citation statements)
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“…The empirically observed near-constancy of the drive parameter I a p [1] for well-optimized Mather type DPF devices over 8 decades of stored energy can be cited as an example. Since the energy required to ionize the volume of gas swept by the PCS must be supplied [20,23,24,25] by the electromechanical work represented by 35, there should exist an upper pressure limit for the operation of a Mather type DPF device; this conjecture, supported by experimental data [23], is another example of physics external to the snowplow effect.…”
Section: Nature Of the Device Optimization Problemmentioning
confidence: 99%
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“…The empirically observed near-constancy of the drive parameter I a p [1] for well-optimized Mather type DPF devices over 8 decades of stored energy can be cited as an example. Since the energy required to ionize the volume of gas swept by the PCS must be supplied [20,23,24,25] by the electromechanical work represented by 35, there should exist an upper pressure limit for the operation of a Mather type DPF device; this conjecture, supported by experimental data [23], is another example of physics external to the snowplow effect.…”
Section: Nature Of the Device Optimization Problemmentioning
confidence: 99%
“…All these aspects are probably reflections of the fact that their work was far ahead of its time: it arrived much before the spread of personal computers and internet. On the other hand, GV model has led to significant insights into limiting factors affecting DPF performance [23,24,25] and also to semi-empirical guidelines for design of DPF devices [26 ].…”
Section: Introductionmentioning
confidence: 99%
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“…This fact allows the verification that is necessary to get a complete ionization of the swept gas in order to obtain an efficient pinch. When the plasma focus is working beyond the UPL, the CS becomes filamented [12]. Drastic descent of the neutron yield under the detection level is verified in every discharge beyond the UPL.…”
Section: Introductionmentioning
confidence: 99%
“…Accordingly, this validates the idea that it is necessary to get a complete ionization of the swept gas in order to obtain an efficient pinch. When the plasma focus is working beyond the UPL, the sheath becomes filamented [11]. The 4 He specific ionization energy lies in the range 0.6 -1.9 MJ/g depending on how high is the fraction of complete ionizations over single ionizations.…”
Section: Pressure Optimizationmentioning
confidence: 99%