COMPACT FLASH X-RAY UNITS. Abstract

Similar documents
ANALYSIS OF A PULSED CORONA CIRCUIT

A COMPACT, 1-MV, 6-kA RADIOGRAPHY SOURCE WITH A ONE- METER EXTENSION AND RIGHT-ANGLE BEND

RAVEN, A 5 kj, 1.5 MV REPETITIVE PULSER* G. J. Rohwein Sandia National Laboratories Albuquerque, New Mexico 87185

PULSED BREAKDOWN CHARACTERISTICS OF HELIUM IN PARTIAL VACUUM IN KHZ RANGE

TRANSMISSION LINE AND ELECTROMAGNETIC MODELS OF THE MYKONOS-2 ACCELERATOR*

OPTICAL EMISSION CHARACTERISTICS OF HELIUM BREAKDOWN AT PARTIAL VACUUM FOR POINT TO PLANE GEOMETRY

ANALYSIS OF SWITCH PERFORMANCE ON THE MERCURY PULSED- POWER GENERATOR *

8.2. Washington, D. C delivered 65 kj into a matched load with 63 ns FWHM. Peak power was about 1 TW.

A NEW BROADBAND PULSED HIGH VOLTAGE MONITOR *

FLASH X-RAY (FXR) ACCELERATOR OPTIMIZATION BEAM-INDUCED VOLTAGE SIMULATION AND TDR MEASUREMENTS *

Adaptation of ASTERIX to Positive Polarity for 2 to 4-MV Rod-Pinch Diode Experiments and Diode Electrical Analysis *

DEVELOPMENT OF AN ULTRA-COMPACT EXPLOSIVELY DRIVEN MAGNETIC FLUX COMPRESSION GENERATOR SYSTEM

IB2-1 HIGH AVERAGE POWER TESTS OF A CROSSED-FIELD CLOSING SWITCH>:< Robin J. Harvey and Robert W. Holly

INVESTIGATION OF A HIGH VOLTAGE, HIGH FREQUENCY POWER CONDITIONING SYSTEM FOR USE WITH FLUX COMPRESSION GENERATORS

EVALUATION OF RESISTORS FOR TRANSIENT HIGH-VOLTAGE APPLICATIONS

9.4 A HIGH CURRENT PULSER FOR EXPERIMENT 11225, "NEUTRINO ELECTRON ELASTIC SCATTERING" C. Dalton, G. Krausse, and J. Sarjeant

PHASING CAPABILITY. Abstract ARRAY. level. up to. to 12 GW. device s outpu antenna array. Electric Mode. same physical dimensions.

PERFORMANCE OF A 10 KV, 625 KA, 85 KJ ENERGY DISCHARGE MODULE UTILIZING A SOLID DIELECTRIC SWITCH.*

PULSED POWER SWITCHING OF 4H-SIC VERTICAL D-MOSFET AND DEVICE CHARACTERIZATION

ULTRA FAST, HIGH REP RATE, HIGH VOLTAGE SPARK GAP PULSER

Strategic Technical Baselines for UK Nuclear Clean-up Programmes. Presented by Brian Ensor Strategy and Engineering Manager NDA

A 1.1 MV REP-RATE IN-LINE OUTPUT SWITCH AND TRIGGERING SYSTEM

Development of a charged-particle accumulator using an RF confinement method FA

REPORT DOCUMENTATION PAGE

DEVELOPMENT OF STITCH SUPER-GTOS FOR PULSED POWER

Report Documentation Page

HIGH TEMPERATURE (250 C) SIC POWER MODULE FOR MILITARY HYBRID ELECTRICAL VEHICLE APPLICATIONS

An experimental system was constructed in which

Durable Aircraft. February 7, 2011

A LASER-TRIGGERED MINI-MARX FOR LOW-JITTER, HIGH-VOLTAGE APPLICATIONS

VHF/UHF Imagery of Targets, Decoys, and Trees

Investigation of a Forward Looking Conformal Broadband Antenna for Airborne Wide Area Surveillance

UPGRADES TO THE DARHT SECOND AXIS INDUCTION CELLS

"OPTIMAL SIMULATION TECHNIQUES FOR DISTRIBUTED ENERGY STORE RAILGUNS WITH SOLID STATE SWITCHES"

EXPERIMENTS ON A HIGH-VACUUM, HIGH-ELECTRIC FIELD STRESS PULSED POWER INTERFACE

TIME DEPENDENT IMAGING OF CYLINDRICAL SHOCKS AT THE PEGASUS FACILITY

CHARACTERIZATION OF PASCHEN CURVE ANOMOLIES AT HIGH P*D VALUES

Research on High Power Railguns at the Naval Research Laboratory

CHARGING INDUCTOR VIEWPORT

REGULATED CAPACITOR CHARGING CIRCUIT USING A HIGH REACTANCE TRANSFORMER 1

DESIGN OPTIONS FOR A PULSED-POWER UPGRADE OF THE Z ACCELERATOR *

Fuse and Load Testing With Mid-Sized, High Energy Density Flux Compression Generators

Robotics and Artificial Intelligence. Rodney Brooks Director, MIT Computer Science and Artificial Intelligence Laboratory CTO, irobot Corp

A R Miller Maxwell Laboratories, Inc Balboa Ave., San Diego, CA

EFFECTS OF ELECTROMAGNETIC PULSES ON A MULTILAYERED SYSTEM

COM DEV AIS Initiative. TEXAS II Meeting September 03, 2008 Ian D Souza

FY07 New Start Program Execution Strategy

FLASH X-RAY (FXR) ACCELERATOR OPTIMIZATION INJECTOR VOLTAGE-VARIATION COMPENSATION VIA BEAM-INDUCED GAP VOLTAGE *

Experimental Observation of RF Radiation Generated by an Explosively Driven Voltage Generator

IREAP. MURI 2001 Review. John Rodgers, T. M. Firestone,V. L. Granatstein, M. Walter

Loop-Dipole Antenna Modeling using the FEKO code

David L. Lockwood. Ralph I. McNall Jr., Richard F. Whitbeck Thermal Technology Laboratory, Inc., Buffalo, N.Y.

ULTRASTABLE OSCILLATORS FOR SPACE APPLICATIONS

14. Model Based Systems Engineering: Issues of application to Soft Systems

Effects of Fiberglass Poles on Radiation Patterns of Log-Periodic Antennas

Thermal Simulation of a Silicon Carbide (SiC) Insulated-Gate Bipolar Transistor (IGBT) in Continuous Switching Mode

0.9Vo II. SYNTHESIZER APPROACH

SA Joint USN/USMC Spectrum Conference. Gerry Fitzgerald. Organization: G036 Project: 0710V250-A1

MINIATURIZED ANTENNAS FOR COMPACT SOLDIER COMBAT SYSTEMS

Active Denial Array. Directed Energy. Technology, Modeling, and Assessment

INFRASOUND SENSOR MODELS AND EVALUATION. Richard P. Kromer and Timothy S. McDonald Sandia National Laboratories

0.18 μm CMOS Fully Differential CTIA for a 32x16 ROIC for 3D Ladar Imaging Systems

Fuzzy Logic Approach for Impact Source Identification in Ceramic Plates

Non-Data Aided Doppler Shift Estimation for Underwater Acoustic Communication

Student Independent Research Project : Evaluation of Thermal Voltage Converters Low-Frequency Errors

Underwater Intelligent Sensor Protection System

Frequency Stabilization Using Matched Fabry-Perots as References

SOLID-STATE POWER SWITCHES FOR HPM MODULATORS. L.E. Kingsley, R. Pastore, & H. Singh. G. Ayres and R. Burdalski. J.F. Agee

Solar Radar Experiments

Thermal Simulation of Switching Pulses in an Insulated Gate Bipolar Transistor (IGBT) Power Module

Technology Maturation Planning for the Autonomous Approach and Landing Capability (AALC) Program

Diver-Operated Instruments for In-Situ Measurement of Optical Properties

FAA Research and Development Efforts in SHM

PERFORMANCE CHARACTERISTICS OF A 1 MV MINIATURE MARX BANK*

August 9, Attached please find the progress report for ONR Contract N C-0230 for the period of January 20, 2015 to April 19, 2015.

Digital Radiography and X-ray Computed Tomography Slice Inspection of an Aluminum Truss Section

Signal Processing Architectures for Ultra-Wideband Wide-Angle Synthetic Aperture Radar Applications

EFFECT OF TRANSFORMER LEAKAGE INDUCTANCE ON THE THREE PHASE CAPACITIVE INPUT RECTIFIER

L. B. Gordon Space Power Institute 231 Leach Center Auburn University, Alabama 36849

EVAUATION OF THE ROD-PINCH DIODE AS A HIGH-RESOLUTION SOURCE FOR FLASHRADIOGRAPHY AT 2 TO 4 MV *

Innovative 3D Visualization of Electro-optic Data for MCM

Challenges in Imaging, Sensors, and Signal Processing

MONITORING RUBBLE-MOUND COASTAL STRUCTURES WITH PHOTOGRAMMETRY

A Multi-Use Low-Cost, Integrated, Conductivity/Temperature Sensor

N C-0002 P13003-BBN. $475,359 (Base) $440,469 $277,858

Lattice Spacing Effect on Scan Loss for Bat-Wing Phased Array Antennas

Report Documentation Page

Pulse Power Performance of the Cygnus 1 and 2 Radiographic Sources

SILICON CARBIDE FOR NEXT GENERATION VEHICULAR POWER CONVERTERS. John Kajs SAIC August UNCLASSIFIED: Dist A. Approved for public release

Remote Sediment Property From Chirp Data Collected During ASIAEX

NEURAL NETWORKS IN ANTENNA ENGINEERING BEYOND BLACK-BOX MODELING

Advances in SiC Power Technology

MEASUREMENTS OF THE RADIATED FIELDS AND CONDUCTED CURRENT LEAKAGE FROM THE PULSED POWER SYSTEMS IN THE NATIONAL IGNITION FACILITY AT LLNL

Experimental Studies of Vulnerabilities in Devices and On-Chip Protection

Acoustic Measurements of Tiny Optically Active Bubbles in the Upper Ocean

Evanescent Acoustic Wave Scattering by Targets and Diffraction by Ripples

Department of Energy Technology Readiness Assessments Process Guide and Training Plan

REPORT DOCUMENTATION PAGE. A peer-to-peer non-line-of-sight localization system scheme in GPS-denied scenarios. Dr.

Conversion of Mercury (a 2-TW Inductive Voltage Adder) to Positive Polarity

Acoustic Change Detection Using Sources of Opportunity

Transcription:

COMPACT FLASH X-RAY UNITS David Platts, Mary P. Hockaday, David Beck, William Coulter, R. Clayton Smith Los Alamos National Laboratory Los Alamos, New Mexico, USA Abstract Flash x-ray units are used to diagnose pulsed power driven experiments on the Pegasus machine at Los Alamos. Several unique designs of Marx powered flash x-ray units have been developed to meet the requirements of the Pegasus experiments. All of these units are compact, battery powered, fiber optically controlled, and EMP shielded. Some of these units are operated with a windowless x-ray tube in the Pegasus machine vacuum tank thereby making the full bremsstrahlung spectrum available for both hard and soft x ray images. Other units obtain multiple x-ray flashes that are almost collinear by employing an x-ray tube configuration which allows closely spaced x-ray emitting anodes. These units all emit a 10 ns FWHM x-ray pulse. Their Marx banks store from 12 to 100 Joules of electrical energy. The x-ray output ranges from 20 to 100 mr at.3m with endpoint energies from 100 to 500 KeV. Introduction The Pegasus machine is often used to implode a thin aluminum liner onto experimental packages. Flash x-rays are used to diagnose the liner implosion and sometimes the reaction of the experimental package. The flash x-ray units must be able to withstand the EMP environment and meet the operating constraints of Pegasus. The compact single unit construction makes EMP shielding them easier as well as making them more convenient to use. The operating constraints of the Pegasus machine require battery power and fiber optic control. The Pegasus machine has 3 sets of ports perpendicular to the axis of the implosion so up to 3 radial flash x-rays can be taken on each shot without resorting to multiple exposure units. A typical radial flash x-ray unit will be described in detail. A Typical Radial Flash X-Ray Unit These units are built around a 12 stage, 12 Joule, 360 kv Marx bank which was derived from an 8 stage spark-gap-trigger Marx1 which is still available commercially2. The unique feature of this Marx design is its 1 ns risetime which is obtained because they are built with a high stage to ground capacitance compared to the stage to stage capacitance. This insures that the Marx erects sequentially since the stage to ground capacitance prevents subsequent stages from seeing voltage until the presently firing stage is fully turned on. As the Marx erects, energy is stored in the stage to ground capacitance of each stage, and each stage in effect pulse charges the next. When the output stage fires it discharges the energy stored in the stage to ground capacitance of the last stage directly into the output. Since this last stage has been pulse charged in a similar 1 ns time period the output gap will hold off enough voltage for its stage to ground capacitance to become fully charged. These factors allow this Marx design to have such a short risetime to full voltage with a measured output impedance around 45 ohms. 892

Report Documentation Page Form Approved OMB No. 0704-0188 Public reporting burden for the collection of information is estimated to average 1 hour per response, including the time for reviewing instructions, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing the collection of information. Send comments regarding this burden estimate or any other aspect of this collection of information, including suggestions for reducing this burden, to Washington Headquarters Services, Directorate for Information Operations and Reports, 1215 Jefferson Davis Highway, Suite 1204, Arlington VA 22202-4302. Respondents should be aware that notwithstanding any other provision of law, no person shall be subject to a penalty for failing to comply with a collection of information if it does not display a currently valid OMB control number. 1. REPORT DATE JUL 1995 4. TITLE AND SUBTITLE Compact Flash X-Ray Units 2. REPORT TYPE N/A 3. DATES COVERED - 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S) 5d. PROJECT NUMBER 5e. TASK NUMBER 5f. WORK UNIT NUMBER 7. PERFORMING ORGANIZATION NAME(S) AND ADDRESS(ES) Los Alamos National Laboratory Los Alamos, New Mexico, USA 8. PERFORMING ORGANIZATION REPORT NUMBER 9. SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS(ES) 10. SPONSOR/MONITOR S ACRONYM(S) 12. DISTRIBUTION/AVAILABILITY STATEMENT Approved for public release, distribution unlimited 11. SPONSOR/MONITOR S REPORT NUMBER(S) 13. SUPPLEMENTARY NOTES See also ADM002371. 2013 IEEE Pulsed Power Conference, Digest of Technical Papers 1976-2013, and Abstracts of the 2013 IEEE International Conference on Plasma Science. Held in San Francisco, CA on 16-21 June 2013. U.S. Government or Federal Purpose Rights License. 14. ABSTRACT Flash x-ray units are used to diagnose pulsed power driven experiments on the Pegasus machine at Los Alamos. Several unique designs of Marx powered flash x-ray units have been developed to meet the requirements of the Pegasus experiments. All of these units are compact, battery powered, fiber optically controlled, and EMP shielded. Some of these units are operated with a windowless x-ray tube in the Pegasus machine vacuum tank thereby making the full bremsstrahlung spectrum available for both hard and soft xray images. Other units obtain multiple x-ray flashes that are almost collinear by employing an x-ray tube configuration which allows closely spaced x-ray emitting anodes. These units all emit a 10 ns FWHM x-ray pulse. Their Marx banks store from 12 to 100 Joules of electrical energy. The x-ray output ranges from 20 to 100 mr at.3m with endpoint energies from 100 to 500 KeV. 15. SUBJECT TERMS 16. SECURITY CLASSIFICATION OF: 17. LIMITATION OF ABSTRACT SAR a. REPORT unclassified b. ABSTRACT unclassified c. THIS PAGE unclassified 18. NUMBER OF PAGES 5 19a. NAME OF RESPONSIBLE PERSON Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

Power Supply Housing Mounting Plat Electronics Housing Marx Figure 1. Side view of a complete radial flash x-ray unit showing the relative placement of the components. Capacitors Insulator Rail Electronics Housing Mounting Plate Figure 2. End view of a radial flash x-ray unit showing the Marx and mounting plate details. Figures 1 & 2 show the layout of these units. All the housings are aluminum cans which have been Alodined3 to prevent oxide formation which would cause poor joint contact 893

and reduce EMP shielding. The Marx bank is contained in a sealed can which is pressurized to 90 psi with dry air for spark gap operation and to reduce corona which would promote pretriggering. Because the pulse durations are only a few tens of nanoseconds the pressurized air also insulates the connection to the x-ray tube without high voltage breakdown. The capacitors are 2. 7 nf 30KV TDK ceramic doorknobs. Half mm thick brass straps mount the capacitors to the poly carbonate rail which holds the spark gaps. The Marx rail assembly fits tightly inside a nylon tube for support. The nylon tube is in tum a slip fit in the aluminum Marx tube. The Marx is charged by means of 2 watt carbon composition resistors in the Megohm impedance range. These resistors hold up well for Marx designs with one capacitor per stage, but start to fail when more capacitors are used in each stage. The power supply and trigger unit are contained in a separate non-pressurized can which is isolated by line filters from the 4an containing the sensitive electronics and batteries. A Gamma High Voltage Research RC-10 series power supply changes the 28 Vdc input to an adjustable regulated 30 kvdc output to charge the Marx. The trigger unit uses a Krytron tube to discharge a.1 uf 3 kv capacitor into a step up transformer whose 35 kv output pulse is applied to a Trigatron type gap in the first stage of the Marx. The fiber optic control consists of a fiber to tum on and charge the unit which is backed up by a separate key plug which must be inserted to operate the unit. Another fiber sends back a signal to indicate that the unit has reached full charge, while a third fiber fires the Marx bank trigger unit. The electronic controllers contain the safety links to the room entry doors and they activate the x-ray warning lights. The X-Ray Tube The radial units employ a windowless x-ray tube design which uses the vacuum inside the Pegasus tank as shown in Figure 3. High Pressure Air Insulation Nylon PEGASUS Tank (vacuum) X Rays Cathode Washer Tungsten Anode Figure 3. The flash x-ray tube showing the windowless design which emits the full x-ray spectrum. 894

The Marx pulses the anode to a high positive potential which starts electron emission from the cathode. The x-ray pulse ends when the Marx runs out of energy or the anode cathode gap is closed by plasma. The x-ray tube uses a.1 mm.metal washer as a cathode. More cathode washers somewhat spaced out and smaller holes lower the tube impedance. A matched impedance will give the best power transfer however more x-ray output may be obtained with somewhat higher tube voltages since the x-ray fluence is approximately proportional to the third power of the voltage on the tube. The anode is most often a tungsten rod, but other materials can be used to obtain different x-ray spectral distributions. The anode rods used range in diameter from several mm to sub mm. The smaller anodes produce less x-rays, but the images are sharper due to the smaller source sizes. The tube is easily modified so these tradeoffs can be determined experimentally by optimizing image quality. The x-ray pulse is normally about 10 ns FWHM, but changes in the tube configuration can modify this. If pulse length is critical it should be monitored when experimenting with tube configuration. To obtain a high contrast image of the thin aluminum liner and other small, low density objects it helps to use soft x-rays in the 5-30 kev range. Commercial sealed x-ray tubes use a thin stainless steel or kovar window to contain the vacuum. This window attenuates the spectrum below about 50 kev. Soft x-ray tubes use beryllium windows; however, this is not a material which one would want scattered around the inside of the vacuum chamber where one has to work to set up the next shot. The windowless tube design allows all the low energy x-rays that are produced by the tungsten target to be emitted. The spectrum is quite strong below 10 kev because of Tungsten L radiation and increased target transparency to continuous bremsstrahlung below the L adsorption edge. At the upper end of the energy range the film response is dropping off rapidly at 30 ke V so the harder x-rays contribute very little to the image. Behind the soft x-ray films hard x-ray images are also obtained by using films with fluorescent converter screens. II II I II I Rays from This Tube II X Rays from~ Other Sources 1 Window Figure 4. Transparent x-ray tube. 895

Axial X-Ray Units The axial x-ray units are larger versions of the radials since they must often penetrate considerable protection plus two mm of copper in the glide planes. When imaging the liner the path through the aluminum is about 2 em so it can be imaged with the hard x-rays that will penetrate the copper. A 15 stage, 90 Joule, 600 kv x-ray unit is commonly used on axis. This unit is built using the same general principles as the radials, but it uses 3 capacitors per stage. In some cases it is desirable to have multiple frames taken along approximately the same axial line of sight. This is accomplished by stacking several transparent( to x-rays) x-ray tubes along the axis. Figure 4 shows such a tube. Each x-ray tube has an independent Marx. The images are then recorded by multiple gated cameras imaging a fluor. Conclusion These compact flash x-ray units have been reliable and convenient to use. They are inexpensive to build, and would be useful in diagnosing other experiments. References 1. D. Platts, Proceedings of the Third IEEE International Pulsed Power Conference, Albuquerque, NM, 1981, p.485. 2. Veradyne Corp., 330 N. Victory Blvd., Burbank, CA 91502, (213) 849-6003. 3. Alodine is a conversion coating for aluminum by Parker Achem, Madison Hgts., MI. 4. Gamma High Voltage Research, Ormond Beach, FL 32174;(904) 677-7070. 896