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Featured researches published by R. C. Mock.


Physics of Plasmas | 1998

Tungsten wire-array Z-pinch experiments at 200 TW and 2 MJ

Rick B. Spielman; C. Deeney; Gordon Andrew Chandler; M.R. Douglas; D. L. Fehl; M. K. Matzen; D. H. McDaniel; T. J. Nash; John L. Porter; T. W. L. Sanford; J. F. Seamen; W. A. Stygar; K.W. Struve; Stephen P. Breeze; J. McGurn; J. Torres; D. M. Zagar; T. Gilliland; D. Jobe; J. L. McKenney; R. C. Mock; M. Vargas; T. Wagoner; D.L. Peterson

Here Z, a 60 TW/5 MJ electrical accelerator located at Sandia National Laboratories, has been used to implode tungsten wire-array Z pinches. These arrays consisted of large numbers of tungsten wires (120–300) with wire diameters of 7.5 to 15 μm placed in a symmetric cylindrical array. The experiments used array diameters ranging from 1.75 to 4 cm and lengths from 1 to 2 cm. A 2 cm long, 4 cm diam tungsten array consisting of 240, 7.5 μm diam wires (4.1 mg mass) achieved an x-ray power of ∼200 TW and an x-ray energy of nearly 2 MJ. Spectral data suggest an optically thick, Planckian-like radiator below 1000 eV. One surprising experimental result was the observation that the total radiated x-ray energies and x-ray powers were nearly independent of pinch length. These data are compared with two-dimensional radiation magnetohydrodynamic code calculations.


Physics of Plasmas | 1999

High Temperature Dynamic Hohlraums on the Pulsed Power Driver Z

T. J. Nash; Mark S. Derzon; Gordon Andrew Chandler; R. J. Leeper; D. L. Fehl; Joel Staton Lash; C. L. Ruiz; G. W. Cooper; J. F. Seaman; J. McGurn; S. Lazier; J. Torres; D. Jobe; T. Gilliland; M. J. Hurst; R. C. Mock; P. Ryan; Dan S. Nielsen; J. C. Armijo; J. L. McKenney; R. Hawn; D. E. Hebron; J. J. MacFarlane; D. Petersen; R.L. Bowers; W. Matuska; D. D. Ryutov

In the concept of the dynamic hohlraum an imploding Z pinch is optically thick to its own radiation. Radiation may be trapped inside the pinch to give a radiation temperature inside the pinch greater than that outside the pinch. The radiation is typically produced by colliding an outer Z-pinch liner onto an inner liner. The collision generates a strongly radiating shock, and the radiation is trapped by the outer liner. As the implosion continues after the collision, the radiation temperature may continue to increase due to ongoing PdV (pressure times change in volume) work done by the implosion. In principal, the radiation temperature may increase to the point at which the outer liner burns through, becomes optically thin, and no longer traps the radiation. One application of the dynamic hohlraum is to drive an ICF (inertial confinement fusion) pellet with the trapped radiation field. Members of the dynamic hohlraum team at Sandia National Labs have used the pulsed power driver Z (20 MA, 100 ns) to create...


Physics of Plasmas | 2002

Dynamics and characteristics of a 215-eV dynamic-hohlraum x-ray source on Z

T. W. L. Sanford; R.W. Lemke; R. C. Mock; Gordon Andrew Chandler; R. J. Leeper; C. L. Ruiz; D.L. Peterson; R. E. Chrien; George C. Idzorek; Robert G. Watt; J. P. Chittenden

A radiation source has been developed on the 20-MA Z facility that produces a high-power x-ray pulse, generated in the axial direction primarily from the interior of a collapsing dynamic hohlraum (DH). The hohlraum is created from a solid cylindrical CH2 target centered within an imploding tungsten wire-array Z pinch. Analyses and interpretation of measurements made of the x-ray generation within and radiated from the hohlraum target have been done using radiation-magnetohydrodynamic-code simulations in the r-z plane that take account of the magnetic Rayleigh–Taylor (RT) instability. These analyses suggest that a significantly reduced RT seed (relative to that used to explain targetless Z-pinch data on Z) is required to explain the observations. Although some quantitative and qualitative agreement with the measurements is obtained with the reduced RT seed, differences remain. Initial attempts to include into the simulations a precursor plasma, arising from wire material driven ahead of the main implosion,...


Journal of Applied Physics | 1989

Measurement of electron energy deposition necessary to form an anode plasma in Ta, Ti, and C for coaxial bremsstrahlung diodes

T. W. L. Sanford; J. A. Halbleib; J. W. Poukey; Arian L. Pregenzer; R. C. Pate; C. E. Heath; R. C. Mock; G. A. Mastin; D. C. Ghiglia; T. J. Roemer; P. W. Spence; G. A. Proulx

Measurements are made of surface doses necessary to initiate an anode plasma by electron bombardment of Ta, Ti, and C anodes for coaxial geometries characteristic of high‐power electron‐beam diodes. Measured lower and upper bounds of doses necessary to form an anode plasma are 54±7–139±16 J/g in Ta, 214±23–294±71 J/g in Ti, and 316±33–494±52 J/g in C. Within these bounds, probable values for the threshold are given under specific assumptions. The measurements are consistent with a thermal desorption model for plasma formation.


Physics of Plasmas | 1997

Dynamics of a high-power aluminum-wire array Z-pinch implosion

T. W. L. Sanford; T. J. Nash; R. C. Mock; Rick B. Spielman; K.W. Struve; Joseph Hammer; J. S. De Groot; K. G. Whitney; J. P. Apruzese

Annular Al-wire Z-pinch implosions on the Saturn accelerator [D. D. Bloomquist et al., Proceedings, 6th Pulsed Power Conference (Institute of Electrical and Electronics Engineers, New York, 1987), p. 310] that have high azimuthal symmetry exhibit both a strong first and weaker second x-ray burst that correlate with strong and weaker radial compressions, respectively. Measurements suggest that the observed magnetic Rayleigh–Taylor (RT) instability prior to the first compression seeds an m=0 instability observed later. Analyses of axially averaged spectral data imply that, during the first compression, the plasma is composed of a hot core surrounded by a cooler plasma halo. Two-dimensional (2-D) radiation magnetohydrodynamic computer simulations show that a RT instability grows to the classic bubble and spike structure during the course of the implosion. The main radiation pulse begins when the bubble reaches the axis and ends when the spike finishes stagnating on axis and the first compression ends. These ...


Physics of Plasmas | 2000

Dynamics of a Z-pinch x-ray source for heating inertial-confinement-fusion relevant hohlraums to 120–160 eV

T. W. L. Sanford; R. E. Olson; R. C. Mock; Gordon Andrew Chandler; R. J. Leeper; T. J. Nash; Laurence E. Ruggles; Walter W. Simpson; K.W. Struve; W. Matuska

A z-pinch radiation source has been developed that generates 60 {+-} 20 KJ of x-rays with a peak power of 13 {+-} 4 TW through a 4-mm diameter axial aperture on the Z facility. The source has heated NIF (National Ignition Facility)-scale (6-mm diameter by 7-mm high) hohlraums to 122 {+-} 6 eV and reduced-scale (4-mm diameter by 4-mm high) hohlraums to 155 {+-} 8 eV -- providing environments suitable for indirect-drive ICF (Inertial Confinement Fusion) studies. Eulerian-RMHC (radiation-hydrodynamics code) simulations that take into account the development of the Rayleigh-Taylor instability in the r-z plane provide integrated calculations of the implosion, x-ray generation, and hohlraum heating, as well as estimates of wall motion and plasma fill within the hohlraums. Lagrangian-RMHC simulations suggest that the addition of a 6 mg/cm{sup 3} CH{sub 2} fill in the reduced-scale hohlraum decreases hohlraum inner-wall velocity by {approximately}40% with only a 3--5% decrease in peak temperature, in agreement with measurements.


Review of Scientific Instruments | 1997

Time-dependent electron temperature diagnostics for high-power, aluminum z-pinch plasmas

T. W. L. Sanford; T. J. Nash; R. C. Mock; Rick B. Spielman; J. F. Seamen; J. McGurn; D. Jobe; T. Gilliland; M. Vargas; K. G. Whitney; J. W. Thornhill; P. E. Pulsifer; J. P. Apruzese

Time-resolved x-ray pinhole photographs and time-integrated radially resolved x-ray crystal-spectrometer measurements of azimuthally symmetric aluminum-wire implosions suggest that the densest phase of the pinch is composed of a hot plasma core surrounded by a cooler plasma halo. The slope of the free-bound x-ray continuum, provides a time-resolved, model-independent diagnostic of the core electron temperature. A simultaneous measurement of the time-resolved K-shell line spectra provides the electron temperature of the spatially averaged plasma. Together, the two diagnostics support a one-dimensional radiation–hydrodynamic model prediction of a plasma whose thermalization on axis produces steep radial gradients in temperature, from temperatures in excess of 1 kV in the core to below 1 kV in the surrounding plasma halo.


Physics of Plasmas | 1998

K-shell radiation physics in the ultrahigh optical depth pinches of the Z generator

J. P. Apruzese; P. E. Pulsifer; J. Davis; R. W. Clark; K. G. Whitney; J.W. Thornhill; T. W. L. Sanford; Gordon Andrew Chandler; C. Deeney; D. L. Fehl; T. J. Nash; Rick B. Spielman; W. A. Stygar; K.W. Struve; R. C. Mock; T. Gilliland; D. Jobe; J. McGurn; J. F. Seamen; J. Torres; M. Vargas

Al:Mg alloy wire arrays of mass loads 1.3–3.6 mg/cm have been imploded with peak currents of 19 MA on the 60 TW Z generator [R. B. Spielman et al., Phys. Plasmas 5, 2105 (1998)] at Sandia National Laboratories. The large mass loads have resulted in the highest K-shell x-ray line optical depths (∼103) produced to date in Z-pinches. Analysis of the time-resolved spectrum of a 2.1 mg/cm shot near the time of peak compression has yielded a temperature–density profile of the pinch that approximately reproduces all features of the x-ray data except the continuum above 5 keV, which is underpredicted. The Ly α/He α ratio for Al is shown to be enhanced relative to that of Mg by two mechanisms: photopumped ladder ionization and absorption of the Al He-like line in a cool outer halo. This analysis and comparisons to some Ti shots demonstrates that the K-shell yield of Al is significantly reduced by line and continuum self-absorption, but that of Ti is not.


Physics of Plasmas | 1998

Increased x-ray power generated from low-mass large-number aluminum-wire-array Z-pinch implosions

T. W. L. Sanford; R. C. Mock; Rick B. Spielman; D.L. Peterson; D. Mosher; N. F. Roderick

A Saturn accelerator study of annular, aluminum-wire-array, Z-pinch implosions in the calculated high-wire-number plasma-shell regime [Phys. Rev. Lett. 77, 5063 (1996)] shows that a factor of 2 decrease in pulse width and an associated doubling of the total radiated x-ray power occurs when the mass of 12 mm radius, 2 cm long array is reduced from above 1.9 mg to below 1.3 mg. The study utilized extensive time- and space-resolved measurements to characterize the implosion over the mass range 0.42–3.4 mg. Eulerian radiation-magnetohydrodynamic-code simulations in the r-z plane agree qualitatively with the measurements. They suggest that the pulse-width decrease with mass is due to the faster implosion velocity of the plasma shell relative to the growth of the shell thickness that arises from a two-stage development of the magnetic Rayleigh–Taylor instability. Over the bulk of the mass-range explored, the variation in K-shell (lines plus free-bound continuum) yield is in qualitative agreement with simple K-s...


Physics of Plasmas | 1998

Improved large diameter wire array implosions from increased wire array symmetry and on-axis mass participation

C. Deeney; T. J. Nash; Rick B. Spielman; J. F. Seaman; J. McGurn; D. Jobe; M. Vargas; T. Gilliland; R. C. Mock; K.W. Struve; K. G. Whitney; P. E. Pulsifer; J. P. Apruzese; J.W. Thornhill; J. Davis

Aluminum wire array, Z-pinch experiments have been performed on an 8 MA generator using arrays consisting of 24, 30, and 42 wires. These experiments were designed to scan through a region of (array mass, implosion velocity) space in which greater than 30% conversion of the implosion kinetic energy into K-shell x rays was predicted to occur [Thornhill et al., Phys. Plasmas 1, 321 (1994)]. Array masses between 120 and 2050 μg/cm were used in these experiments. An analysis of the x-ray data taken using 24 wire arrays, shows a one-to-one correspondence between the observed kilo-electron-volt yields (5–64 kJ) and the fraction of initial array mass (0.3%–60%) that is radiating from the K shell. The 30 and 42 wire experiments demonstrated that tighter pinches with increased radiated powers were achieved with these larger wire number, improved symmetry arrays. In addition, increases in the implosion mass and array diameter in the 30 and 42 wire number cases resulted in increases in the radiated yield over the cor...

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T. W. L. Sanford

Sandia National Laboratories

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T. J. Nash

Sandia National Laboratories

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D.L. Peterson

Los Alamos National Laboratory

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J. P. Apruzese

United States Naval Research Laboratory

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R. J. Leeper

Sandia National Laboratories

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K.W. Struve

Sandia National Laboratories

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Rick B. Spielman

Sandia National Laboratories

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D. Jobe

Sandia National Laboratories

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W. A. Stygar

Sandia National Laboratories

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