William S. Varnum
Los Alamos National Laboratory
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Featured researches published by William S. Varnum.
Physics of Plasmas | 1999
T. R. Dittrich; S. W. Haan; M. M. Marinak; Stephen M. Pollaine; D. E. Hinkel; D. H. Munro; C. P. Verdon; George L. Strobel; R. McEachern; R. Cook; C.C. Roberts; D. C. Wilson; P. A. Bradley; Larry R. Foreman; William S. Varnum
Several inertial confinement fusion (ICF) capsule designs have been proposed as possible candidates for achieving ignition by indirect drive on the National Ignition Facility (NIF) laser [Paisner et al., Laser Focus World 30, 75 (1994)]. This article reviews these designs, their predicted performance using one-, two-, and three-dimensional numerical simulations, and their fabricability. Recent design work at a peak x-ray drive temperature of 250 eV with either 900 or 1300 kJ total laser energy confirms earlier capsule performance estimates [Lindl, Phys. Plasmas 2, 3933 (1995)] that were based on hydrodynamic stability arguments. These simulations at 250 eV and others at the nominal 300 eV drive show that capsules having either copper doped beryllium (Be+Cu) or polyimide (C22H10N2O4) ablators have favorable implosion stability and material fabrication properties. Prototypes of capsules using these ablator materials are being constructed using several techniques: brazing together machined hemishells (Be+Cu)...
Physics of Plasmas | 1996
William J. Krauser; Nelson M. Hoffman; Douglas Wilson; Bernhard H. Wilde; William S. Varnum; David B. Harris; Fritz J. Swenson; P. A. Bradley; S. W. Haan; Stephen M. Pollaine; A. S. Wan; J. C. Moreno; Peter A. Amendt
Recent results are presented from two‐dimensional LASNEX [G. B. Zimmerman and W. L. Kruer, Comments Plasmas Phys. Controlled Thermonucl. Fusion 2, 51 (1975)] calculations of the indirectly driven hohlraum and ignition capsules proposed for the National Ignition Facility (NIF). The calculations concentrate on two capsule designs, the baseline design that has a bromine‐doped plastic ablator, and the beryllium design that has a copper‐doped beryllium ablator. Both capsules have a cryogenic fuel layer. Primary emphasis in these calculations is placed upon robustness studies detailing various sensitivities. Because of computer modeling limitations these studies fall into two categories: those performed with integrated modeling where the capsule, hohlraum, and laser rays all are modeled simultaneously with the laser power levels as the only energy input; and those performed in a capsule‐only mode where an externally imposed radiative flux is applied to the exterior of the capsule, and only the capsule performan...
Physics of Plasmas | 2000
G. R. Bennett; J. M. Wallace; T. J. Murphy; R. E. Chrien; Norman D. Delamater; Peter L. Gobby; Allan A. Hauer; K. A. Klare; John A. Oertel; Robert G. Watt; Daniel C. Wilson; William S. Varnum; R. S. Craxton; V. Yu. Glebov; Jeremy David Schnittman; C. Stoeckl; Stephen M. Pollaine; R. E. Turner
A highly uniform thermal x-radiation field for indirect-drive inertial confinement fusion implosions may be obtained by irradiating a four-hole, tetrahedral geometry, spherical hohlraum with all 60 Omega laser beams. Implosion studies and calculations [J. M. Wallace et al., Phys. Rev. Lett. 82, 3807 (1999)] indicate a drive uniformity comparable to that expected for the National Ignition Facility [J. A. Painser et al., Laser Focus World 30, 75 (1994)]. With 60 beams distributed over the cavity wall, tetrahedral hohlraums have a natural insensitivity to power balance and pointing errors. Standard, smooth Nova capsules imploded with this drive indicate that moderate convergence-ratio implosions, Cr∼18, have measured-neutron yield to calculated-clean-one-dimensional-neutronyield ratios similar to those previously investigated using the comparatively poor drive uniformity of Nova cylindrical hohlraums. This may indicate that a nonsymmetry-related neutron yield degradation mechanism, e.g., hydrodynamic mixing ...
Laser and Particle Beams | 1999
T. R. Dittrich; S. W. Haan; M. M. Marinak; D. E. Hinkel; Stephen M. Pollaine; R. McEachern; Robert Cook; C.C. Roberts; D. C. Wilson; P. A. Bradley; William S. Varnum
Several choices exist in the design and production of capsules intended to ignite and propagate fusion burn of the DT fuel when imploded by indirect drive at the National Ignition Facility. These choices include ablator material, ablator dopant concentration and distribution, capsule dimensions, and x-ray drive profile (shock timings and strengths). The choice of ablator material must also include fabrication and material characteristics, such as attainable surface finishes, permeability, strength, transparency to radio frequency and infrared radiation, thermal conductivity, and material homogeneity. Understanding the advantages and/or limitations of these choices is an ongoing effort for LLNL and LANL designers. At this time, simulations in one- two- and three- dimensions show that capsules with either a copper doped beryllium or a polyimide (C 22 H 10 N 2 O 4 ) ablator material have both the least sensitivity to initial surface roughnesses and favorable fabrication qualities. Simulations also indicate the existence of capsule designs based on these ablator materials which ignite and burn when imploded by less than nominal laser performance (900 kJ energy, 250 TW power, producing 250 eV peak radiation temperature). We will describe and compare these reduced scale capsules, in addition to several designs which use the expected 300 eV peak x-ray drive obtained from the nominal NIF laser (1.3 MJ, 500 TW).
Laser interaction and related plasma phenomena: 12th international conference | 1996
Nelson M. Hoffman; Douglas Wilson; William S. Varnum; William J. Krauser; Bernhard H. Wilde
We examine the hydrodynamic stability of imploding ICF capsules by explicitly calculating the evolution of a realistic surface perturbation far into its nonlinear regime, using a 2D Lagrangian radiation‐hydrodynamics code. The perturbation, which consists initially of mesh displacements in the capsule, is represented by the sum of many spherical harmonic modes, having finite amplitudes and realistic spectrum. A 90‐degree sector of the capsule is modeled, allowing proper boundary conditions for all modes simultaneously. Because of the large distortion of the mesh that occurs during the calculations, it is necessary to rezone the mesh frequently, by mapping physical variables to a new undistorted mesh. No model‐specific parameters are required in this technique. We have used the technique to calculate the yield of several designs for a National Ignition Facility capsule as a function of initial root‐mean‐square surface roughness σ of the outer ablator surface or the inner cryogenic DT surface. Typically for...
Laser and Particle Beams | 2005
George A. Kyrala; Norman D. Delamater; Douglas Wilson; Joyce Ann Guzik; Don Haynes; Mark Gunderson; K. A. Klare; Robert W. Watt; William Monford Wood; William S. Varnum
Fusion Technology | 1999
J.R. Duke; Norman E. Elliott; Joyce E. Moore; Veronica M. Gomez; Ruben Manzanares; Gerald Rivera; Robert G. Watt; William S. Varnum; Peter L. Gobby
Archive | 2000
Norman D. Delamater; Teri J. Murphy; William S. Varnum; Daniel C. Wilson; S. C. Evans; Kevin Kent Gifford; Stephen M. Pollaine; Robert E. L. Turner; V. Yu. Glevov; C. Stoeckl; J. M. Soures
Archive | 2004
George A. Kyrala; Norman D. Delamater; Daniel C. Wilson; Joyce Ann Guzik; Donald Arthur Haynes; Michael Arthur Gunderson; Ken Klare; William S. Varnum; Warren Garbett
Archive | 2003
George A. Kyrala; Norman D. Delamater; Daniel C. Wilson; Robert G. Watt; Joyce Ann Guzik; William Monford Wood; William S. Varnum; Donald Arthur Haynes; George D. Pollak; Michael Arthur Gunderson; Ken Klare; Warren Garbett; A. Michael Dunne; Peter Graham