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Dive into the research topics where B.W. Stallard is active.

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Featured researches published by B.W. Stallard.


Nuclear Fusion | 1979

Field-reversal experiments in a neutral-beam-injected mirror machine

W. C. Turner; J.F. Clauser; F.H. Coensgen; D.L. Correll; W.F. Cummins; R.P. Freis; R.K. Goodman; A. L. Hunt; T.B. Kaiser; G.M. Melin; W.E. Nexsen; T.C. Simonen; B.W. Stallard

Data on field-reversal experiments in the neutral-beam-injected 2XIIB mirror machine are reported. The best result is an estimated field-reversal parameter ζ = ΔB/Bvac = 0.9 ± 0.2 with vacuum field strength Bvac = 4.35 kG. Experiments at higher field strength Bvac = 6.7 kG achieved ζ = 0.6 ± 0.1. Ion energy confinement nτEi for the Bvac = 6.7 kG experiment is less than that predicted by classical Spitzer electron drag. Ion-cyclotron oscillations increasing with injected neutral-beam current suggest that ion-cyclotron losses are present and that ΔB/Bvac could be increased by improving stabilization of the ion-cyclotron oscillations.


Nuclear Fusion | 1983

Fokker-Planck calculations of hot-electron formation by electron cyclotron resonance heating in the TMX-Upgrade tandem mirror

B.W. Stallard; Y. Matsuda; W. M. Nevins

The paper studies cold plasma trapping and heating of hot electrons in mirror geometry using a time-dependent, bounce-averaged Fokker-Planck code with quasi-linear diffusion due to RF heating at fundamental and second harmonic frequencies. With the restriction k|| = 0, the code models the beam-controlled heating (spatially restricted electric fields) that will be used to create thermal barriers in the TMX-Upgrade tandem-mirror experiment. By spatially localizing the microwave beams, which are strongly absorbed in a single pass, the mean hot-electron energy may be controlled. Heating is away from the midplane to control anisotropy (P⊥/P|| ). For a given magnetic field geometry and cold-plasma source temperature Ts, the parameters of the hot electrons scale with the quantity χ ≡ 2/nsω, where is the electric field, ns is the cold-plasma density, and ω is the frequency.


Nuclear Fusion | 1982

Ambipolar potential formation and axial confinement in TMX

D.L. Correll; S.L. Allen; T.A. Capser; J.F. Clauser; P. Coakley; F.H. Coensgen; W.C. Condit; W.F. Cummins; J. C. Davis; R. P. Drake; J.H. Foote; A.H. Futch; R.K. Goodman; D. P. Grubb; Gary Hallock; E. B. Hooper; R. S. Hornady; A. L. Hunt; C. V. Karmendy; A.W. Molvik; W.E. Nexsen; W. L. Pickles; P. Poulsen; T.C. Simonen; B.W. Stallard; O.T. Strand

TMX experimental data on ambipolar potential control and on the accompanying electrostatic confinement are reported. In the radial core of the central cell, measurements of electrostatic potentials of 150 V which augment axial ion confinement are in agreement with predictions using the Maxwell-Boltzmann result. Central-cell ion confinement was observed to scale according to electrostatic potential theory up to average enhancement factors of eight times over mirror confinement alone.


Nuclear Fusion | 1980

Production of large-radius, high-beta, confined mirror plasmas

D.L. Correll; J.H. Clauser; F.H. Coensgen; W.F. Cummins; R. P. Drake; J.H. Foote; A.H. Futch; R.K. Goodman; D. P. Grubb; G.M. Melin; W.E. Nexsen; T.C. Simonen; B.W. Stallard; W. C. Turner

This paper reports results of experiments in which mirror-confined plasmas with radii as high as 7 ion gyro-radii are produced and maintained by neutral-beam injection. In these plasmas, betas as high as 0.45 were achieved and limited only by the available neutral-beam power. Electron temperature and ion-energy confinement increased with larger plasma size.


Nuclear Fusion | 1981

The effect of end-cell stability on the confinement of the central-cell plasma in TMX

R. P. Drake; T.A. Casper; J.F. Clauser; F.H. Coensgen; D.L. Correll; W.F. Cummins; J. C. Davis; J. H. Foote; A.H. Futch; R.K. Goodman; D. P. Grubb; R. S. Hornady; W.E. Nexsen; T.C. Simonen; B.W. Stallard

In the Tandem Mirror Experiment (TMX), the central-cell losses provide the warm unconfined plasma necessary to stabilize the drift-cyclotron loss-cone instability in the end cells. This places a theoretical limit on central-cell confinement, which is expressed as a limit on the end-cell to central-cell density ratio. As this density ratio increases in a TMX experiment, large increases of end-cell ion-cyclotron-frequency plasma fluctuations are observed. These fluctuations cause the central-cell confinement to decrease, in agreement with a theoretical model.


Journal of Nuclear Materials | 1976

Control of first-wall surface conditions in the 2XIIB magnetic mirror plasma confinement experiment

T.C. Simonen; R.H. Bulmer; F.H. Coensgen; W.F. Cummins; C. Gormezano; B.C. Logan; A.W. Molvik; W.E. Nexsen; W.C. Turner; B.W. Stallard; G.E. Vogtlin; R.R. Vandervoort

The control of first-wall surface conditions in the 2XIIB Magnetic Mirror Plasma Confinement experiment is described. Before each plasma shot, the first wall is covered with a freshly gettered titanium surface. Up to 5 MW of neutral beam power has been injected into 2XIIB, resulting in first-wall bombardment fluxes of 10


Nuclear Fusion | 1989

Scaling of plasma potentials in TMX-U with the end walls grounded

G.D. Porter; S.L. Allen; C. J. Burdett; M. R. Carter; D.L. Correll; J. H. Foote; R. S. Hornady; W.E. Nexsen; B.W. Stallard

sup 17


Proceedings of the International Symposium on Plasma Wall Interaction | 1977

Plasma wall charge-exchange interactions in the 2XIIB magnetic mirror experiment

B.W. Stallard; F.H. Coensgen; W.F. Cummins; C. Gormezano; B.G. Logan; A.W. Molvik; W.E. Nexsen; T.C. Simonen; W. C. Turner

atoms.cm


international conference on plasma science | 1995

Wave-electron coupling in helicon source

A.W. Molvik; B.W. Stallard; E. B. Hooper

sup -2


Physical Review Letters | 1975

Stabilization of a neutral-beam-sustained, mirror-confined plasma

F.H. Coensgen; W.F. Cummins; B.G. Logan; A.W. Molvik; W.E. Nexsen; T.C. Simonen; B.W. Stallard; W.C. Turner

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W.E. Nexsen

Lawrence Livermore National Laboratory

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F.H. Coensgen

Lawrence Livermore National Laboratory

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T.C. Simonen

Lawrence Livermore National Laboratory

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W.F. Cummins

Lawrence Livermore National Laboratory

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A.W. Molvik

Lawrence Livermore National Laboratory

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D.L. Correll

Lawrence Livermore National Laboratory

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J.F. Clauser

Lawrence Livermore National Laboratory

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R.K. Goodman

Lawrence Livermore National Laboratory

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B.G. Logan

Lawrence Livermore National Laboratory

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D. P. Grubb

Lawrence Livermore National Laboratory

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