2011 IEEE Pulsed Power Conference 2011
DOI: 10.1109/ppc.2011.6191527
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The flow dynamics along non-uniform self magnetically insulated transmission lines

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Cited by 5 publications
(3 citation statements)
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“…These results seem to conflict with the simulation results depicted in [15], which indicates for a conical transition with a large transition length and the same vacuum impedance as coaxial sections, the power flow condition is close to that of an uniform MITL, and the cathode current should not change a lot. This discrepancy might be due to the fact that the downstream coaxial MITL cathode current B-dot location is just in or very close to the loss front of self-limited flow, where many of electrons are launched from the cathode into the A-K gap, making the cathode current decrease remarkably.…”
Section: Resultscontrasting
confidence: 59%
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“…These results seem to conflict with the simulation results depicted in [15], which indicates for a conical transition with a large transition length and the same vacuum impedance as coaxial sections, the power flow condition is close to that of an uniform MITL, and the cathode current should not change a lot. This discrepancy might be due to the fact that the downstream coaxial MITL cathode current B-dot location is just in or very close to the loss front of self-limited flow, where many of electrons are launched from the cathode into the A-K gap, making the cathode current decrease remarkably.…”
Section: Resultscontrasting
confidence: 59%
“…The vacuum impedance is related to the canonical constant of motion in the direction of power flow and if the change in the vacuum impedance of transition between the geometrical shapes is small, regular flow could continue undisturbed. So the canonical momentum in this MITL configuration is conserved [15]. In the experiment hollow cathode diodes with different A-K distances were used as shown in Fig.…”
Section: Methodsmentioning
confidence: 99%
“…There is electron current loss to the walls along downstream cylindrical MITL prior to the edge where the entire current is shunted to the anode wall as anode current. 19,21,22 In addition, the electron loss front will cut down the pulse width. The cathode current amplitudes of the PIC simulation by probes P1, P2, P3, P4, P5 and P6 are 0.97 MA, 0.86 MA, 0.78 MA, 0.77 MA, 0.77 MA, 0.38 MA.…”
Section: A Downstream Mitl Work On Self-limited Flowmentioning
confidence: 99%