Part Testing of the "MOL" Stand for the "BAIKAL" Project

Bakhtin, V. P.; Grabovsky, E. V.; Gribov, A. N.; Житлухин, А. М.; Krilov, M.K.; Levashov, V. F.; Lototsky, A.P.; Toporkov, D. A.; Umrikhin, N. M.; Halimullin, Yu.A.; Velikhov, E. P.; Dolgachev, G. I.; Kalinin, Yu. G.; Kingsep, A. S.; Smirnov, V. P.; Glukhih, V. A.; Kuchinsky, V.G.; Pechersky, O.P.; Kormilitsyn, A.I.; Kononenko, V.Yu.; Rikovanov, G.N.

doi:10.1109/ppc.2005.300658

Cited by 1 publication

(1 citation statement)

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“…Losses in the Z convolute prior to the refurbishment project for low-impedance z-pinch loads were as high as 1.5 MA out of 18.5 MA [22], but after refurbishment, the stored energy of Z doubled, and the convolute losses increased to 3 MA out of 23 MA for similar low-impedance loads [25]. This is significant because designs for new, highercurrent (50 þ MA) generators such as Baikal [30][31][32] and Z-Next [33,34] roughly quadruple the electrical power of Z, and their designs include a triple post-hole convolute to add current from six MITL levels into a single final power feed. In order to move forward with future highercurrent accelerators, a validated understanding of convolute science is required such that new convolute designs, which increase convolute efficiency, can be developed.…”

Section: Introductionmentioning

confidence: 99%

Experimental study of current loss and plasma formation in the Z machine post-hole convolute

Gómez

Gilgenbach

Cuneo

et al. 2017

Phys. Rev. Accel. Beams

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The Z pulsed-power generator at Sandia National Laboratories drives high energy density physics experiments with load currents of up to 26 MA. Z utilizes a double post-hole convolute to combine the current from four parallel magnetically insulated transmission lines into a single transmission line just upstream of the load. Current loss is observed in most experiments and is traditionally attributed to inefficient convolute performance. The apparent loss current varies substantially for z-pinch loads with different inductance histories; however, a similar convolute impedance history is observed for all load types. This paper details direct spectroscopic measurements of plasma density, temperature, and apparent and actual plasma closure velocities within the convolute. Spectral measurements indicate a correlation between impedance collapse and plasma formation in the convolute. Absorption features in the spectra show the convolute plasma consists primarily of hydrogen, which likely forms from desorbed electrode contaminant species such as H 2 O, H 2 , and hydrocarbons. Plasma densities increase from 1 × 10 16 cm −3 (level of detectability) just before peak current to over 1 × 10 17 cm −3 at stagnation (tens of ns later). The density seems to be highest near the cathode surface, with an apparent cathode to anode plasma velocity in the range of 35-50 cm=μs. Similar plasma conditions and convolute impedance histories are observed in experiments with high and low losses, suggesting that losses are driven largely by load dynamics, which determine the voltage on the convolute.

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