2010
DOI: 10.1109/tps.2009.2036730
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Effect of Wire Diameter and Addition of an Axial Magnetic Field on the Dynamics of Radial Wire Array $Z$-Pinches

Abstract: The operation of radial wire array Z-pinches driven by a 1-MA 250-ns current pulse was studied. Variation in the cathode diameter and wire diameter does not affect the overall plasma dynamics but controls the time of wire breakage and the time of pinch formation. The measured times of full wire ablation at the cathode were used to determine the ablation velocity (V abl ), and the results give a scaling V abl ∼ (wire diameter) −0.46 . Experiments with added axial magnetic field show an increase in the pinched p… Show more

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Cited by 27 publications
(11 citation statements)
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“…The inferred position of the ions is consistent with the location of the unstable, detached jet that develops on the axis of the cavity, which is shown from a timeresolved, dark-field Schlieren results presented in the right hand side of figure 6(b). The pinching and subsequent development of a kink-type MHD instability in the jet has been reported in previous experiments with radial wire arrays in Lebedev et al (2005), Suzuki-Vidal et al (2010b) and in radial foil Z-pinches, in which the wires are replaced by a continuous metallic foil ( Suzuki-Vidal et al 2007, Ciardi et al 2009, Gourdain et al 2009, 2013. The development of a kink instability in the latter leads to the formation of strong, tangled magnetic fields as studied from numerical simulations of radial foils Z-pinches using the code GORGON (Ciardi et al 2009).…”
Section: Fly-eye Camera and Magnetic Spectrometersupporting
confidence: 62%
See 1 more Smart Citation
“…The inferred position of the ions is consistent with the location of the unstable, detached jet that develops on the axis of the cavity, which is shown from a timeresolved, dark-field Schlieren results presented in the right hand side of figure 6(b). The pinching and subsequent development of a kink-type MHD instability in the jet has been reported in previous experiments with radial wire arrays in Lebedev et al (2005), Suzuki-Vidal et al (2010b) and in radial foil Z-pinches, in which the wires are replaced by a continuous metallic foil ( Suzuki-Vidal et al 2007, Ciardi et al 2009, Gourdain et al 2009, 2013. The development of a kink instability in the latter leads to the formation of strong, tangled magnetic fields as studied from numerical simulations of radial foils Z-pinches using the code GORGON (Ciardi et al 2009).…”
Section: Fly-eye Camera and Magnetic Spectrometersupporting
confidence: 62%
“…The toroidal magnetic field reaches ∼100 T at the electrode radius and decreases inversely proportional to the radial distance from the axis. The formation of magnetic-tower jets in radial wire arrays has been studied in detail both experimentally (Lebedev et al 2005, Suzuki-Vidal et al 2010b and numerically (e.g. Ciardi et al 2007) and are depicted schematically in figures 1(b)-(d).…”
Section: Magnetic Tower-jet Formation Using Radial Wire Arraysmentioning
confidence: 99%
“…This process is similar to the formation of radiatively cooled jets in conical wire array Z-pinches and during early stages of radial wire array Z-pinches. 18,[30][31][32][33][34][35] The first significant difference of this setup from our previous experiments 11 is the use of thicker foils and a cathode with a larger diameter. The corresponding increase of the foil mass and the decrease of the magnetic field pressure acting on the foil at the cathode radius allow to suppress the formation of magnetically dominated jets, studied in previous experiments.…”
Section: Experimental Setup Diagnostics and Numerical Setupmentioning
confidence: 91%
“…This assumption is based on the motion of different features along the jet, as seen also in the jets from single-episode magnetic cavities in radial wire arrays (Suzuki-Vidal et al 2010). The axial tip velocity of the first cavity was measured from time-resolved XUV emission images, resulting in V Ztip ≈ 128 km/s.…”
Section: Kinetic Energymentioning
confidence: 99%