2012
DOI: 10.1063/1.4725423
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Numerical investigation on the implosion dynamics of wire-array Z-pinches in (r, θ) geometry

Abstract: The implosion dynamics of wire-array Z-pinches are investigated numerically in 2D (r, θ) geometry by using a resistive MHD code. It is assumed that the wires have expanded to plasmas with diameter d0, which is used as the initial condition for the consequent implosion process. In fact, the explosion process of individual wires is not included. By changing d0, the effects of the wire expansion degree on the implosion dynamics are analyzed. When d0 is larger, the current density is more concentrated at the outer… Show more

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Cited by 12 publications
(5 citation statements)
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“…We studied the influence of the wire number of outer array on the implosion mode of nested wire array by using a 2D (r, θ) resistive MHD code [82] which has been used to simulate the implosion process of single wire array [19]. Since the current distribution inside the wire array depends not only on the inductance, but also on the diffusion and M A N U S C R I P T…”
Section: Nested Wire Arraysmentioning
confidence: 99%
“…We studied the influence of the wire number of outer array on the implosion mode of nested wire array by using a 2D (r, θ) resistive MHD code [82] which has been used to simulate the implosion process of single wire array [19]. Since the current distribution inside the wire array depends not only on the inductance, but also on the diffusion and M A N U S C R I P T…”
Section: Nested Wire Arraysmentioning
confidence: 99%
“…where η ⊥ is the transverse Spitzer resistivity, ρ vac is the initial low-density background which is considered to be 10 −6 g cm −3 , ρ is the plasma density and k is the resistivity coefficient of the low-density background [32]. The optimal value of k was calculated to be 24 allowing for a smooth transition to the high resistivity background as well as for an accepted timestep value.…”
Section: Set Of Equationsmentioning
confidence: 99%
“…Purely Eulerian grid codes like GORGON [15][16][17][18][19][20][21][22], purely Lagrangian like MULTI-2D [23][24][25] or arbitrary Lagrangian Eulerian (ALE) codes like ALEGRA [26][27][28][29] and MACH2 [30,31], are capable to describe astrophysical and laboratory plasmas. Also, codes like ATHENA and ZEUS or FLASH, were evaluated and tested among others in the Noh Z-Pinch problem and implosion dynamics of wire-array Z-pinches [32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…Plasma production from pulsed power plasma devices loaded as Z-pinch and X-pinch is essential for plasma physics MULTI-2D [14][15][16] or Arbitrary Lagrangian Eulerian codes like ALEGRA [17][18][19][20] and MACH2 [21,22], are capable of describing astrophysical and laboratory plasmas. Codes like ATHENA, ZEUS 2D, MARED 2D and FLASH are evaluated and tested in the Noh Z-Pinch problem and implosion dynamics of wire-array Z-pinches [23][24][25][26][27]. Especially, the GORGON Eulerian code is ideal for MHD plasma applications such as laser-produced magnetized jets [28][29][30], Z and X-pinch wire configurations [31][32][33][34], Z-pinch wire arrays [35][36][37][38][39], conical arrays, radial wire arrays and foils which create magnetically driven outflows and are studied in laboratory astrophysics experiments mainly for jets of young stellar objects [29,30,[40][41][42][43][44].…”
Section: Introductionmentioning
confidence: 99%