J. Zier
University of Michigan
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Featured researches published by J. Zier.
IEEE Transactions on Plasma Science | 2008
Brad W. Hoff; Ronald M. Gilgenbach; N.M. Jordan; Y. Y. Lau; E. Cruz; David M. French; M. R. Gomez; J. Zier; T.A. Spencer; D. Price
Experiments have been performed in testing magnetic priming at the cathode of a relativistic magnetron to study the effects on high-power microwave performance. Magnetic priming consists of N/2 azimuthal magnetic perturbations applied to an N-cavity magnetron for rapid generation of the desired number of electron spokes for the pi-mode. Magnetic perturbations were imposed by utilizing three high-permeability nickel-iron wires embedded beneath the emission region of the cathode, spaced 120 apart. Magnetic priming was demonstrated to increase the percentage of pi-mode shots by 15% over the baseline case. Mean peak power for -mode shots was found to be higher in the magnetically primed case by almost a factor of two. Increases in mean microwave pulsewidth were also observed in the magnetically primed case when compared to the unprimed case (66-ns primed versus 50-ns unprimed). Magnetron starting current for the magnetically primed pi-mode exhibited a reduction to 69% of the unprimed baseline starting current.
Physics of Plasmas | 2012
J. Zier; Ronald M. Gilgenbach; D.A. Chalenski; Y. Y. Lau; David M. French; M. R. Gomez; Sonal Patel; I. M. Rittersdorf; A.M. Steiner; Matthew Weis; Peng Zhang; M.G. Mazarakis; M. E. Cuneo; M. R. Lopez
Experiments have been performed on a nominal 100 ns rise time, MegaAmpere (MA)-class linear transformer driver to explore the magneto-Rayleigh-Taylor (MRT) instability in planar geometry. Plasma loads consisted of ablated 400 nm-thick, 1 cm-wide aluminum foils located between two parallel-plate return-current electrodes. Plasma acceleration was adjusted by offsetting the position of the foil (cathode) between the anode plates. Diagnostics included double-pulse, sub-ns laser shadowgraphy, and machine current B-dot loops. Experimental growth rates for MRT on both sides of the ablated aluminum plasma slab were comparable for centered-foils. The MRT growth rate was fastest (98 ns e-folding time) for the foil-offset case where there was a larger magnetic field to accelerate the plasma. Other cases showed slower growth rates with e-folding times of about ∼106 ns. An interpretation of the experimental data in terms of an analytic MRT model is attempted.
Review of Scientific Instruments | 2008
M. R. Gomez; J. Zier; Ronald M. Gilgenbach; David M. French; Wilkin Tang; Y. Y. Lau
Soft metal gaskets (indium and silver) were used to reduce contact resistance between the wire and the electrode in an aluminum wire Z pinch by more than an order of magnitude over the best weighted contact case. Clamping a gasket over a Z-pinch wire compresses the wire to the electrode with a greater normal force than possible with wire weights. Average contact resistance was reduced from the range of 100-3000 Omega (depending on wire weight mass) to 1-10 Omega with soft metal gaskets. Single wire experiments (13 microm Al 5056) on a 16 kA, 100 kV Marx bank showed an increase in light emission (97%) and emission volume (100%) of the plasma for the reduced contact resistance cases. The measured increases in plasma volume and light emission indicate greater energy deposition in the ablated wire. Additionally, dual-wire experiments showed plasma edge effects were significantly decreased in the soft metal gasket contact case. The average height of the edge effects was reduced by 51% and the width of the edge effects was increased by 40%, thus the gasket contact case provided greater axial uniformity in the plasma expansion profile of an individual wire.
DENSE Z‐PINCHES: Proceedings of the 7th International Conference on Dense#N#Z‐Pinches | 2009
R. M. Gilgenbach; M. R. Gomez; J. Zier; Wilkin Tang; D. M. French; Y. Y. Lau; M.G. Mazarakis; M. E. Cuneo; Mark D. Johnston; B.V. Oliver; T.A. Mehlhorn; A. A. Kim; V. A. Sinebryukhov
Researchers at The University of Michigan have constructed and tested a 1‐MA Linear Transformer Driver (LTD), the first of its type to reach the USA. The Michigan Accelerator for Inductive Z‐pinch Experiments, (MAIZE), is based on the LTD developed at the Institute of High Current Electronics in collaboration with Sandia National Labs and UM. This LTD utilizes 80 capacitors and 40 spark gap switches, arranged in 40 “bricks,” to deliver a 1 MA, 100 kV pulse with 100 ns risetime into a matched resistive load. Preliminary resistive‐load test results are presented for the LTD facility.Planned experimental research programs at UM include: a) Studies of Magneto‐Raleigh‐Taylor instability of planar foils, and b) Vacuum convolute studies including cathode and anode plasma.
ieee international pulsed power conference | 2009
M.G. Mazarakis; S. Cordova; William E. Fowler; K. LeChien; Joshua J. Leckbee; Finis W. Long; M. K. Matzen; D. H. McDaniel; R. McKee; J. L. McKenney; B.V. Oliver; C.L. Olson; John L. Porter; S.T. Rogowski; K.W. Struve; W. A. Stygar; J.W. Weed; J. R. Woodworth; A.A. Kim; Vadim A. Sinebryukhov; Ronald M. Gilgenbach; M. R. Gomez; D. M. French; Y.Y. Lau; J. Zier; D.L. Johnson; D. M. VanDevalde; R. A. Sharpe; K. Ward
Most of the modern high-current high-voltage pulsed power generators require several stages of pulse conditioning (pulse forming) to convert the multi-microsecond pulses of the Marx generator output to the 40–300 ns pulse required by a number of applications including x-ray radiography, pulsed high current linear accelerators, Z-pinch, Isentropic Compression (ICE), and Inertial Fusion Energy (IFE) drivers. This makes the devices large, cumbersome to operate, and expensive. Sandia, in collaboration with a number of other institutions, is developing a new paradigm in pulsed power technology; the Linear Transformer Driver (LTD) technology. This technological approach can provide very compact devices that can deliver very fast high current and high voltage pulses. The output pulse rise time and width can be easily tailored to the specific application needs. Trains of a large number of high current pulses can be produced with variable inter-pulse separation from nanoseconds to milliseconds. Most importantly, these devices can be rep-rated to frequencies only limited by the capacitor specifications (usually is 10Hz). Their footprint as compared with current day pulsed power accelerators is considerably smaller since LTD do not require large oil and de-ionized water tanks. This makes them ideally fit for applications that require portability. In the present paper we present Sandia Laboratorys broad spectrum of developmental effort to design construct and extensively validate the LTD pulsed power technology.
Physics of Plasmas | 2014
Matthew Weis; Peng Zhang; Y. Y. Lau; I. M. Rittersdorf; J. Zier; Ronald M. Gilgenbach; Mark Hess; Kyle Peterson
Using the ideal magnetohydrodynamic model, we calculate the temporal evolution of initial ripples on the boundaries of a planar plasma slab that is subjected to the magneto-Rayleigh-Taylor instability. The plasma slab consists of three regions. We assume that in each region the plasma density is constant with an arbitrary value and the magnetic field is also constant with an arbitrary magnitude and an arbitrary direction parallel to the interfaces. Thus, the instability may be driven by a combination of magnetic pressure and kinetic pressure. The general dispersion relation is derived, together with the feedthrough factor between the two interfaces. The temporal evolution is constructed from the superposition of the eigenmodes. Previously established results are recovered in the various limits. Numerical examples are given on the temporal evolution of ripples on the interfaces of the finite plasma slab.
Physics of Plasmas | 2009
J. Zier; J. D. Douglass; I. C. Blesener; K. S. Blesener; D. A. Chalenski; Ronald M. Gilgenbach; J. B. Greenly; D. A. Hammer; P. F. Knapp; B. R. Kusse; Y. Y. Lau; R. D. McBride; W. Syed; E. P. Yu
Azimuthally correlated wire core ablation was compared for closely spaced versus widely spaced wires in a 1 MA Z-pinch. X-ray point-projection diagnostics revealed that 240 μm spaced wires exhibited a correlation coefficient approaching unity in both real space and in k-space. This correlated ablation between wires at a fixed axial location is believed to occur due to an enhanced, localized Joule heating. Wires separated by 2.47 mm or greater were uncorrelated in real space, but correlated in k-space, indicating the ablation structure between wires was shifted in phase.
IEEE Transactions on Plasma Science | 2008
J. Zier; M. R. Gomez; David M. French; Ronald M. Gilgenbach; Yue Y. Lau; Wilkin Tang; Michael Edward Cuneo; Thomas Alan Mehlhorn; Mark D. Johnston; M.G. Mazarakis
Heavier wire weights reduce contact resistance, which increases the energy deposition in wire plasma. Images from a two-wire Z-pinch showing the effects of wire tension on expansion performance are presented.
joint international conference on infrared millimeter waves and international conference on teraherz electronics | 2006
Brad W. Hoff; Ronald M. Gilgenbach; Y. Y. Lau; N.M. Jordan; W.M. White; J. Zier; E. Cruz; T.A. Spencer; D. Price
Magnetic priming [1] experiments performed on the UM/Titan relativistic magnetron (6-vane, -300kV, 5-10kA, 0.3-0.5 mus) have shown improvements in magnetron performance over baseline operation. In the current experimental setup, three, 4-cm long magnetic wires (Mu-Metal) are located within the cathode structure, centered beneath the emission region, and spaced 120 degrees apart. These wires produce magnetic perturbations with N/2 azimuthal-symmetry (for pi-mode in an N vane magnetron). Because of the close proximity of the priming structures to the cathode surface, the magnetic perturbations are strongest in the region where the electrons are emitted into the magnetron interaction space.
Applied Physics Letters | 2010
I. M. Rittersdorf; Y. Y. Lau; J. Zier; Ronald M. Gilgenbach; E. Cruz; John W. Luginsland
Peer-to-peer locking of two magnetrons is analyzed including the effects of a frequency chirp and of low frequency noise. It is found that complete phase locking cannot be achieved in either case. However, as long as the locking condition is well satisfied instantaneously, a high degree of locking occurs. This analysis in the time domain is adapted to locking in the spatial domain, in particular to the interpretation of some recent experiments on the spatial correlation of two ablating current-carrying wires that are placed sufficiently close to each other.