Caudill, L.D.; Chandler, G.I.; Hall, C.R.; Trujillo, J.F.
Los Alamos National Lab., NM (USA)1986
Los Alamos National Lab., NM (USA)1986
AbstractAbstract
[en] The computer control system for the ZT-P experiment has been implemented using a fiber-optic link in all 161 control signal paths. Four classes of control signals are used in this design. These are: (a) digital-out, an on-off signal from computer to machine actuator, (b) digital-in, an on-off signal from machine sensor to computer, (c) analog-out, a 0 to 10 volt analog signal from computer to machine actuator, (d) analog-in, a 0 to +1 milliampere analog signal from machine sensor to computer. The digital-in and the digital-out class of signals require no control power at the machine. The analog-out and the analog-in class of signals use available machine power for control. This unique power arrangement and the use of fiber-optic links totally isolate the electrically noisy machine areas from the sensitive electronics in the computer control. Advantages of this system including low cost, small size, personnel safety, and ease of maintenance and modification are discussed
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1986; 14 p; High temperature plasma diagnostics; Hilton Head Island, SC (USA); 9-13 Mar 1986; CONF-860324--20; Available from NTIS, PC A02/MF A01 as DE86008719
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AbstractAbstract
[en] The ZTH reversed-field pinch to be installed in the Confinement Physics Research Facility (CPRF) will produce a significant ambient magnetic field. To avoid ground-loop and other electrical problems, the diagnostics in direct or possible contact with the experiment will be accessed through a fiber optic data way. The frequency-modulated analog links developed for this system have a bandwidth of dc to 100 kHz and a signal-to-noise ratio of better than 60 dB. The fiber optic transmitter units include a signal conditioner and a microprocessor controller. The conditioners can be configured as dc-coupled, low-noise differential amplifiers, or as high-gain, low-drift differential integrators with a very long droop time constant. Magnetic field pickup is minimized by balancing sensitive circuit areas to within 5 mm2 in all three planes of the PC boards. The gain, offset, and integrator reset are controlled and monitored by the microprocessor, and their status is displayed on the front panel of the transmitter unit. The signal conditioner can be controlled locally, or by way of a fiber optic coupled control network. The system allows fast, convenient, noise-immune control of a large number of signal conditioners from a central host computer. By varying the offset, the computer can verify the operational integrity of the data links. 2 refs., 6 figs
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1989; 5 p; 13. international symposium on fusion engineering; Knoxville, TN (USA); 2-6 Oct 1989; CONF-891007--68; CONTRACT W-7405-ENG-36; Available from NTIS, PC A02/MF A01 as DE90002444; OSTI; INIS; US Govt. Printing Office Dep
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Caudill, L.D.; Chandler, G.I.; Hall, C.R.; Trujillo, J.F.
Proceedings of the 6th topical conference on high temperature plasma diagnostics1986
Proceedings of the 6th topical conference on high temperature plasma diagnostics1986
AbstractAbstract
[en] The computer control system for the ZT-P experiment has been implemented using a fiber-optic link in all 161 control signal paths. Four classes of control signals are used in this design. These are: digital-out; an on-off signal from computer to machine actuator, digital-in, and on-off signal from machine sensor to computer, analog-out, a 0 - 10 volt analog signal from computer to machine actuator, analog-in, 0 to +1 milliampere analog signal from machine sensor to computer. The digital-in and the digital-out class of signals require no control power at the machine end. The analog-out and the analog-in class of signals use available machine power for control. This unique power arrangement and the use of fiber-optic links serve to totally isolate electrically noisy machine areas from the sensitive electronics in the computer control. Advantages, including low cost, small size, personnel safety, and ease of maintenance and modification are discussed
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Anon; 92 p; 1986; p. F/18; Princeton Plasma Physics Laboratory; Princeton, NJ (USA); 6. topical conference on high temperature plasma diagnostics; Hilton Head Island, SC (USA); 9-13 Mar 1986; CONF-860324--; Princeton Plasma Physics Laboratory, P.O. Box4 51, Princeton, NJ 08544 (USA)
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[en] Of 500 patients referred for an examination of the upper gastrointestinal tract, 15% were found to have radiographic evidence of esophageal disease. A cursory esophageal survey appears to be insufficient. Thorough evaluation should consist of a minimal multiphasic approach involving double- and single-contrast radiography, fluoroscopic studies of motility, and a mucosal relief study
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Journal Article
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Radiology; ISSN 0033-8419; ; v. 147(1); p. 65-70
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AbstractAbstract
[en] The computer control system for the ZT-P experiment has been implemented using a fiber-optic link in all 161 control signal paths. Four classes of control signals are used in this design. These are (a) digital-out, an on--off signal from computer to machine actuator, (b) digital-in, an on--off signal from machine sensor to computer, (c) analog-out, a 0--10-V analog signal from computer to machine actuator, (d) analog-in, a 0--1-mA analog signal from machine sensor to computer. The digital-in and the digital-out class of signals require no control power at the machine. The analog-out and the analog-in class of signals use available machine power for control. This unique power arrangement and the use of fiber-optic links totally isolate the electrically noisy machine areas from the sensitive electronics in the computer control. Advantages of this system including low cost, small size, personnel safety, and ease of maintenance and modification are discussed
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Journal Article
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Ekdahl, C.A.; Abeyta, E.O.; Caudill, L.D.; Dalmas, D.A.; Eversole, S.A.; Harrison, J.F.; Holzscheiter, M.H.; Johnson, J.B.; Jacquez, E.B.; McCuistian, B.T.; Nielson, K.E.; Oro, D.M.; Schauer, M.M.; Studebaker, J.K.; Sullivan, G.K.; Temple, R.D.
Los Alamos National Laboratory (United States). Funding organisation: US Department of Energy (United States)2003
Los Alamos National Laboratory (United States). Funding organisation: US Department of Energy (United States)2003
AbstractAbstract
[en] The second axis of the Dual Axis Radiographic Hydro-Test (DARHT) facility will provide up to four short (<100 ns) radiation pulses for flash radiography of high-explosive driven implosion experiments. To accomplish this the DARHT-I1 linear induction accelerator (LIA) will produce a 2-kA electron beam with 18-MeV kinetic energy, constant to within 2 0.5% for 2-ps. A fast kicker will cleave four short pulses out of the 2-ps flattop, with the bulk of the beam diverted into a dump. The short pulses will then be transported to the final-focus magnet, and focused onto a tantalum target for conversion to bremsstrahlung pulses for radiography. DARHT-II is a collaborative effort between Los Alamos, Livermore, and Berkeley National Laboratories. The first tests of the second axis accelerator, described herein, were performed to demonstrate the technology and to meet the performance requirements for closing out the DARHT-II construction project.
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1 Jan 2003; 5 p; 2003 Particle Accelerator Conference; Portland, OR (United States); 12-16 May 2003; Available from http://lib-www.lanl.gov/cgi-bin/getfile?01045263.pdf; PURL: https://www.osti.gov/servlets/purl/976631-ynxnAV/
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Jaitly, N.C.; Ramrus, A.; Coleman, M.D.; Earley, L.M.; Downing, J.N.; Reisch, H.H.; Caudill, L.D.; Eversol, S.A.
Los Alamos National Lab., NM (United States); Maxwell Labs., Inc., San Diego, CA (United States). Funding organisation: USDOE, Washington, DC (United States)1993
Los Alamos National Lab., NM (United States); Maxwell Labs., Inc., San Diego, CA (United States). Funding organisation: USDOE, Washington, DC (United States)1993
AbstractAbstract
[en] The DARHT Facility is being designed at Los Alamos National Laboratory to produce high resolution flash radiographs of hydrodynamic experiments. Two linear induction accelerators (LIA), each in the range of 16 to 20 MeV, will be used to produce intense bremsstrahlung X-ray pulses of short duration (60 ns flat top). Each LIA will produce a 3 kA, high brightness, electron beam using a 4 MeV injector and a series of 250 kV induction cells. Technology demonstration of key accelerator subsystems is under progress at the DARHT Integrated Test Stand (ITS). The eight inductions cells present in the ITS are driven by a Maxwell prototype Induction Cell Pulsed Power Supply (ICPPS) which provides 250 kV, 70ns pulses via four Blumleins. Each Blumlein drives two cells and is triggered using independently controlled trigger units. This turnkey DARHT Trigger System, consisting of four separate trigger units, provides 200 kV trigger pulses with low jitter and fast rise time to each of the four Blumlein coaxial spark gaps. Details of the trigger system design and results obtained during extensive testing at Maxwell are described
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1993; 8 p; CONTRACT W-7405-ENG-36; Also available from OSTI as DE94005667; NTIS; US Govt. Printing Office Dep
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Ekdahl, C.A.; Abeyta, E.O.; Caudill, L.D.; Dalmas, D.A.; Eversole, S.A.; Gallegos, R.A.; Harrison, J.F.; Holzscheiter, M.H.; Johnson, J.B.; Jacquez, E.B.; McCuistian, B.T.; Montoya, N.A.; Nath, S.; Neilsen, K.E.; Oro, D.M.; Rodriguez, L.R.; Rodriguez, P.; Sanchez, M.; Scarpetti, R.; Schauer, M.M.; Simmons, D.F.; Smith, H.V.; Studebaker, J.K.; Sullivan, G.W.; Swinney, C.A.; Temple, R.D.; Chen, Y.J.; Houck, T.L.; Henestroza, E.; Eylon, S.; Fawley, W.M.; Yu, S.; Bender, H.A.; Broste, W.B.; Carlson, C.A.; Durtschi, G.M.; Frayer, D.K.; Johnson, D.E.; Jones, K.C.; Meidinger, A.; Moy, K.J.; Sturgess, R.E.; Tom, C.Y.
Los Alamos National Laboratory (United States). Funding organisation: US Department of Energy (United States)2004
Los Alamos National Laboratory (United States). Funding organisation: US Department of Energy (United States)2004
AbstractAbstract
[en] The second axis of the Dual Axis Radiographic Hydro-Test (DARHT) facility will provide up to four short (< 150 ns) radiation pulses for flash radiography of high-explosive driven implosion experiments. To accomplish this the DARBT-II linear induction accelerator (LIA) will produce a 2-kA electron beam with 18-MeV kinetic energy, constant to within ±0.5% for 2-μs. A fast kicker will cleave four short pulses out of the 2-μs flattop, with the bulk of the beam diverted into a dump. The short pulses will then be transported to the final-focus magnet, and focused onto a tantalum target for conversion to bremsstrahlung pulses for radiography. DARHT-II is a collaborative effort between the Los Alamos, Lawrence Livermore, and Lawrence Berkeley National Laboratories of the University of California. The first tests of the second axis accelerator were designed to demonstrate the technology, and to meet the modest performance requirements for closing out. The DARHT-II construction project. These experiments demonstrated that we could indeed produce a 1.2 kA beam with pulse length 0.5-1.2 μs and accelerate it to 12.5 MeV. These de-rated parameters were chosen to minimize risk of damage in these first experiments with this novel accelerator. The beam showed no evidence of the BBU instability for these parameters. In fact, we had to reduce the magnetic guide field by a factor of 5 before BBU was observed.
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1 Jan 2004; 3 p; EPAC 2004: 9. European Particle Accelerator Conference; Lucerne (Switzerland); 5-9 Jul 2004; Available from http://lib-www.lanl.gov/cgi-bin/getfile?00639676.pdf; PURL: https://www.osti.gov/servlets/purl/977677-mF3dkr/
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