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Dive into the research topics where Paul G. Weber is active.

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Featured researches published by Paul G. Weber.


Physics of fluids. B, Plasma physics | 1990

Energetic electron measurements in the edge of a reversed-field pinch

J.C. Ingraham; R. F. Ellis; J.N. Downing; C.P. Munson; Paul G. Weber; G. A. Wurden

The edge plasma of the ZT‐40M [Fusion Technol. 8, 1571 (1985)] reversed‐field pinch has been studied using a combination of three different plasma probes: a double‐swept Langmuir probe, an electrostatic energy analyzer, and a calorimeter–Langmuir probe. The edge plasma has been measured both with and without a movable graphite tile limiter present nearby in the plasma. Without a limiter a fast nonthermal tail of electrons (T≂350 eV) is detected in the edge plasma with nearly unidirectional flow along B and having a density between 2% and 10% of the cold edge plasma (T≂20 eV). The toroidal sense of this fast electron flow is against the force of the applied electric field. A large power flux along B is measured flowing in the same direction as the fast electrons and is apparently carried by the fast electrons. With the limiter present the fast electrons are still detected in the plasma, but are strongly attenuated in the shadow of the limiter. The measured scrape‐off lengths for both the fast electrons and...


Physics of Fluids | 1987

Asymmetric magnetic flux generation, m=1 activity, and edge phenomena on a reversed-field pinch

R. B. Howell; J.C. Ingraham; G. A. Wurden; Paul G. Weber; C. J. Buchenauer

The ZT‐40M [Fusion Tech. 8, 1571 (1985)] reversed‐field pinch has been used to study magnetic flux perturbations during high‐θ [θ=Bθ(a)/〈Bφ〉>1.6] discharges. Asymmetric toroidal magnetic flux perturbations are found to be associated with magnetic flux emerging through the toroidal shell gap and with m=0 magnetic disturbances moving toroidally. Ramping current discharges, which are a special case of high‐θ operation, show the most robust self‐generation of toroidal flux. The electron density fluctuations on the inside major radius and associated m=1 and m=0 fluctuations seen on edge magnetic field probes provide a clearer picture of activity during a soft x‐ray sawtooth crash. During the sawtooth crash, significant magnetic energy is apparently converted into kinetic energy of the particles.


SPIE's International Symposium on Optical Science, Engineering, and Instrumentation | 1999

Multispectral Thermal Imager mission overview

Paul G. Weber; Brian C. Brock; Alfred J. Garrett; Barham W. Smith; Christoph C. Borel; William B. Clodius; Steven C. Bender; R. Rex Kay; Max L. Decker

The Multispectral Thermal Imager (MTI) is a research and development project sponsored by the Department of Energy and executed by Sandia and Los Alamos National Laboratories and the Savannah River Technology Center. Other participants include the U.S. Air Force, universities, and many industrial partners. The MTI mission is to demonstrate the efficacy of highly accurate multispectral imaging for passive characterization of industrial facilities and related environmental impacts from space. MTI provides simultaneous data for atmospheric characterization at high spatial resolution. Additionally, MTI has applications to environmental monitoring and other civilian applications. The mission is based in end-to-end modeling of targets, signatures, atmospheric effects, the space sensor, and analysis techniques to form a balanced, self-consistent mission. The MTI satellite nears completion, and is scheduled for launch in late 1999. This paper describes the MTI mission, development of desired system attributes, some trade studies, schedule, and overall plans for data acquisition and analysis. This effort drives the sophisticated payload and advanced calibration systems, which are the overall subject of the first session at this conference, as well as the data processing and some of the analysis tools that will be described in the second segment.


Physics of Fluids | 1988

Oscillating field current drive experiments in a reversed field pinch

Kurt F. Schoenberg; J.C. Ingraham; C.P. Munson; Paul G. Weber; D.A. Baker; R.F. Gribble; R. B. Howell; Guthrie Miller; W.A. Reass; A.E. Schofield; S. Shinohara; G. A. Wurden

Steady‐state current sustainment by oscillating field current drive (OFCD) utilizes a technique in which the toroidal and poloidal magnetic fields at the plasma surface are modulated at audio frequencies in quadrature. Experiments on the ZT‐40M reversed field pinch [Fusion Technol. 8, 1571 (1985)] have examined OFCD over a range of modulation amplitude, frequency, and phase. For all cases examined, the magnitude of the plasma current is dependent on the phase of the modulations as predicted by theory. However, evidence of current drive has only been observed at relatively low levels of injected power. For larger modulation amplitudes, the data suggest that substantial current drive is offset by increased plasma resistance as a result of modulation enhanced plasma–wall interactions. The initial experimental results and supporting theoretical interpretations of OFCD are discussed.


SPIE's International Symposium on Optical Science, Engineering, and Instrumentation | 1999

Multispectral Thermal Imager (MTI) Payload Overview

Steven C. Bender; Brian C. Brock; D.M. Bullington; D.A. Byrd; P.J. Claassen; Max L. Decker; T.D. Henson; R. Rex Kay; R.E. Kidner; C.E. Lanes; C. Little; K.D. Marbach; N.G. Rackley; Jeffrey L. Rienstra; Barham W. Smith; R.B. Taplin; Paul G. Weber

MTI is a comprehensive research and development project that includes up-front modeling and analysis, satellite system design, fabrication, assembly and testing, on-orbit operations, and experimentation and data analysis. The satellite is designed to collect radiometrically calibrated, medium resolution imagery in 15 spectral bands ranging from 0.45 to 10.70 micrometer. The payload portion of the satellite includes the imaging system components, associated electronics boxes, and payload support structure. The imaging system includes a three-mirror anastigmatic off-axis telescope, a single cryogenically cooled focal plane assembly, a mechanical cooler, and an onboard calibration system. Payload electronic subsystems include image digitizers, real-time image compressors, a solid state recorder, calibration source drivers, and cooler temperature and vibration controllers. The payload support structure mechanically integrates all payload components and provides a simple four point interface to the spacecraft bus. All payload components have been fabricated and tested, and integrated.


Nuclear Fusion | 1991

Fluctuations and transport in a reversed field pinch edge plasma

H.Y.W. Tsui; Ch. P. Ritz; Guthrie Miller; J.C. Ingraham; C.P. Munson; Kurt F. Schoenberg; Paul G. Weber

Edge fluctuations are characterized and their associated transport is determined from Langmuir probe measurements in the ZT-40M reversed field pinch. It is found that the fluctuations have high normalized amplitudes and |n|/n = 0.4). There are significant contributions from magnetic perturbations acting on the equilibrium gradients. Compared to the global estimates, the fluctuation driven particle flux is large, whereas the corresponding electron energy flux is not. In the limiter shadow, the equilibrium density and electron temperature scale lengths are shorter and the fluctuation levels are higher. The fluctuation driven particle flux in the limiter shadow is 60% less than that in the plasma edge; most of the reduction is in the low frequency spectral region, which is where global MHD magnetic fluctuations are strongest.


IEEE Transactions on Geoscience and Remote Sensing | 2005

Multispectral thermal imager: mission and applications overview

John J. Szymanski; Paul G. Weber

The Multispectral Thermal Imager (MTI) satellite is a research and development project sponsored by the U.S. Department of Energy. The primary mission is to demonstrate advanced multispectral and thermal imaging from a satellite, including new technologies, data processing, and analysis techniques and validation by reference to ground truth. The MTI builds on the efforts of a number of earlier efforts, including Landsat, National Aeronautics and Space Administration remote sensing missions, and others, but the MTI incorporates a unique combination of attributes designed to advance the state of the art. The MTI satellite was launched on March 12, 2000 into a 580 km/spl times/610 km, sun-synchronous orbit with nominal 1 a.m. and 1 p.m. equatorial crossing times. The Air Force Space Test Program provided the Orbital Sciences Taurus launch. The satellite-based sensors obtain radiance data that are subsequently processed into measurements of atmospheric and surface properties such as column water vapor, atmospheric aerosol loading, surface temperatures, material composition, and others. This paper provides an overview of the MTI research objectives, design, operations, data products, and data processing and analysis. Several other papers provide greater detail on selected topics.


Review of Scientific Instruments | 1983

High‐intensity lithium‐ion source

Paul G. Weber

This high‐intensity lithium‐ion source is a modified duopigatron. The arc discharge between the cathode and anode in a working gas, typically helium or hydrogen, expands through an aperture in the anode into an expansion cup containing lithium vapor, which is subsequently ionized. Results of spectroscopy and mass analysis are reported. Total continuous output at low accelerating potentials has exceeded 15 mA/cm2 while operating at 10% of the maximum arc current capability.


IEEE Transactions on Geoscience and Remote Sensing | 2005

Modeling the MTI electro-optic system sensitivity and resolution

Bradly J. Cooke; Terrence S. Lomheim; Bryan E. Laubscher; Jeffrey L. Rienstra; William B. Clodius; Steve C. Bender; Paul G. Weber; Barham W. Smith; John L. Vampola; Paul J. Claassen; Mary Ballard; Amy E. Galbraith; Christoph C. Borel; William H. Atkins

We present an analysis methodology that offers efficient characterization of the Multispectral Thermal Imager (MTI) electro-optic system response to a wide range of user-specified system parameters and spectral scenarios. This methodology combines physics-based modeling of the MTI hardware with MTI prelaunch characterization data. The resulting models enable the user to generate application-specific sensitivity and resolution studies of the MTI image capture process, and aid in the development of calibration procedures and retrieval algorithms for MTI. In addition to quantifying the MTI response, the methodology developed in this paper is sufficiently general to permit the prototyping and evaluation of a variety of multispectral electro-optic systems. Finally, an example utilizing nominal orbital parameters and targeted MODTRAN scenarios that exercise the various spectral band functions is provided.


Proceedings of SPIE | 2001

MULTISPECTRAL THERMAL IMAGER - OVERVIEW

W. Randy Bell; Paul G. Weber

The Multispectral Thermal Imager, MTI, is a research and development project sponsored by the United States Department of Energy. The primary mission is to demonstrate advanced multispectral and thermal imaging from a satellite, including new technologies, data processing and analysis techniques. The MTI builds on the efforts of a number of earlier efforts, including Landsat, NASA remote sensing missions, and others, but the MTI incorporates a unique combination of attributes. The MTI satellite was launched on 12 March 2000 into a 580 km x 610 km, sun-synchronous orbit with nominal 1 am and 1 pm equatorial crossing times. The Air Force Space Test Program provided the Orbital Sciences Taurus launch vehicle. The satellite has a design lifetime of a year, with the goal of three years. The satellite and payload can typically observe six sites per day, with either one or two observations per site from nadir and off-nadir angles. Data are stored in the satellite memory and down-linked to a ground station at Sandia National Laboratory. Data are then forwarded to the Data Processing and Analysis Center at Los Alamos National Laboratory for processing, analysis and distribution to the MTI team and collaborators. We will provide an overview of the Project, a few examples of data products, and an introduction to more detailed presentations in this special session.

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Barham W. Smith

Los Alamos National Laboratory

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Christoph C. Borel

Los Alamos National Laboratory

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William B. Clodius

Los Alamos National Laboratory

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J.C. Ingraham

Los Alamos National Laboratory

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G. A. Wurden

Los Alamos National Laboratory

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C.P. Munson

Los Alamos National Laboratory

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James Theiler

Los Alamos National Laboratory

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John J. Szymanski

Los Alamos National Laboratory

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Anthony B. Davis

Los Alamos National Laboratory

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J.N. Downing

Los Alamos National Laboratory

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