Technical Issues: Approach: Construct a system that will allow high frequency, high voltage switching to monitor the recovery rate and jitter of different.

Slides:



Advertisements
Similar presentations
Chapter 13 Transmission Lines
Advertisements

Nonequilibrium Thermodynamics Laboratories The Ohio State University OH Laser-Induced Fluorescence Measurements in Nanosecond Pulse Discharge Plasmas Inchul.
CHAPTER 3 MICROWAVE ‘O’ TYPE TUBES
Voltage and Its Measurements
Analysis & Selection of Ignition System P M V Subbarao Professor Mechanical Engineering Department Strong and Reliable Ignition Ensures Efficient Combustion.
NON-THERMAL ATMOSPHERIC PRESSURE PLASMAS FOR AERONAUTIC APPLICATIONS Richard B. Miles, Dmitry Opaits, Mikhail N. Shneider, Sohail H. Zaidi - Princeton.
Post Deflection Acceleration
427 PHC.  Atomic emission spectroscopy (AES) is based upon emission of electromagnetic radiation by atoms.
Fusion Physics - Energy Boon or Nuclear Gloom? David Schilter and Shivani Sharma.
Chamber Dynamic Response Modeling Zoran Dragojlovic.
Beam Loss Analysis Tool for the CTF3 PETS Tank M. Velasco, T. Lefevre, R. Scheidegger, M. Wood, J. Hebden, G. Simpson Northwestern University, Evanston,
Harbin Institute of Technology (Weihai) 1 Chapter 2 Channel Measurement and simulation  2.1 Introduction  Experimental and simulation techniques  The.
Electric Curcuits and Measurements Basic Electrical components and their functions Measurements of electrical circuits characteristics - Multimeter - Oscilloscope.
Sensors used in EFI (Electronic Fuel Injection)
Chapter 8 Inverters AC Power • Inverters • Power Conditioning Units • Inverter Features and Specifications.
Pulse Width Modulation (PWM) LED Dimmer Circuit
ALPHA Storage Ring Indiana University Xiaoying Pang.
Pulse Width Modulation (PWM) LED Dimmer Circuit
Linac 6575 Modulator PFN Charging Power Supply Upgrade Minh Nguyen December 5, 2012.
Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator.
Chapter 5 Lecture 10 Spring Nonlinear Elements 1. A nonlinear resistance 2. A nonlinear reactance 3. A time varying element in you circuit or system.
Slide # 1 Examples of pressure sensor packaging Temperature characteristics of a piezoresistive pressure sensor. Transfer function at three different temperatures.
Atomic Emission Spectroscopy
CERN DC Spark System Capabilities Anders Korsbäck, BE-RF-LRF University of Helsinki.
Chapter 5 Engineering Tools for Electrical and Computer Engineers.
Experiences with RPC Detectors in Iran and their Potential Applications Tarbiat Modares University Ahmad Moshaii A. Moshaii, IPM international school and.
STRIPLINE KICKER STATUS. PRESENTATION OUTLINE 1.Design of a stripline kicker for beam injection in DAFNE storage rings. 2.HV tests and RF measurements.
COMPUTED ENVELOPE LINEARITY OF SEVERAL FM BROADCAST ANTENNA ARRAYS J. Dane Jubera 2008 NAB Engineering Conference.
Means & Methods of Homogeneous Charge Combustion P M V Subbarao Professor Mechanical Engineering Department A Sudden Combustion, Yet Needs A Care & takes.
Chamber parameters that we can modify and that affect the rising time Number of ionisation clusters produced in the drift gap: Poisson Distribution Probability.
KICKER LNF David Alesini LNF fast kickers study group* * D. Alesini, F. Marcellini P. Raimondi, S. Guiducci.
DEVELOPMENT OF A COMPACT PULSE GENERATOR FOR X-RAY BACKLIGHTING OF PLANAR FOIL ABLATION EXPERIMENTS* This work was supported by DoE Award number DE-SC ,
TDS8000 and TDR Considerations to Help Solve Signal Integrity Issues.
Performance Improvement of APS Booster Ring Dipole Magnet Power Supplies Ju Wang The 3 rd Workshop on Power Converters for Particle.
Swedish Defence Research Agency (FOI), Defence & Security, Systems and Technology Presented at The IET International Conference on Pulsed Power, CERN,
Photos placed in horizontal position with even amount of white space between photos and header Sandia National Laboratories is a multi-program laboratory.
DC12 Commissioning Status GOALS: establish operating conditions, determine initial calibration parameters and measure operating characteristics for the.
FAST KICKER STATUS Fabio Marcellini On behalf of LNF fast kickers study group* * D. Alesini, F. Marcellini P. Raimondi, S. Guiducci.
The dynamic behaviour of Resistive Plate Chambers
Design of a readout system for RPCs Olu Amoda2 The LODEN Group The group is an association of Fermilab scientists who teamed up to build a cosmic ray.
Instrumentation & Power Electronics
Power Supply System for DRFS
Study of UV absorption and photoelectron emission in RPC (Resistive Plate Counters) detector with an UV source Carlo Gustavino (INFN-LNGS) RPC and their.
Experimental and Numerical studies on Bulk Micromegas SINP group in RD51 Applied Nuclear Physics Division Saha Institute of Nuclear Physics Kolkata, West.
Techniques for Nuclear and Particle Physics Experiments By W.R. Leo Chapter Eight:
Kévin Pepitone 1CLIC project meeting, CERN, December 1st, 2015 Kevin PEPITONE, BE-RF Drive Beam Injector Gun.
Numerical Modelling of Needle-Grid Electrodes for Negative Surface Corona Charging System Y. Zhuang*, G. Chen and M. Rotaru University of Southampton,
Complementary MOS inverter “CMOS” inverter n channel enhancement mode (V TN > 0) in series with a p channel enhancement mode (V TP < 0) 0 < V in < V.
IMAGE DATA ACQUISITION
Simulations of various aspects of the PPS Various members of the collaboration, to be enumerated later.
1 Electrical Skills Voltage and Its Measurements.
DC Spark Developments Nick Shipman - Thursday, 16 August
Laboratory photo-ionized plasma David Yanuka. Introduction  Photo-ionized plasmas are common in astrophysical environments  Typically near strong sources.
PROPERTIES OF UNIPOLAR DC-PULSED MICROPLASMA ARRAYS AT INTERMEDIATE PRESSURES* Peng Tian a), Chenhui Qu a) and Mark J. Kushner a) a) University of Michigan,
1 NSTX EXPERIMENTAL PROPOSAL - OP-XP-712 Title: HHFW Power Balance Optimization at High B Field J. Hosea, R. Bell, S. Bernabei, L. Delgado-Aparicio, S.
Tao Tang, Craig Burkhart
PS-ESS and LEBT State of the art Lorenzo Neri Istituto Nazionale di Fisica Nucleare Laboratori Nazionali del Sud.
Kévin Pepitone 1CLIC workshop, CERN, January 2016 Kevin PEPITONE, BE-RF LEETCHI: Drive Beam Electron Source.
Chapter 9 CAPACITOR.
RPCs with Ar-CO2 mix G. Aielli; R.Cardarelli; A. Zerbini For the ATLAS ROMA2 group.
1 PEBB-based Power Electronic Systems to Support MVDC Studies Herbert L. Ginn III, Mississippi State University.
Mg Films Grown by Pulsed Laser Deposition as Photocathodes: QE and surface adsorbates L. Cultrera INFN – National Laboratories of Frascati.
FUNCTION GENERATOR.
Residential Cabling Technologies Copyright © 2005 Heathkit Company, Inc. All Rights Reserved Electrical Measurements.
X-ray Production Sharif Qatarneh Medical Physics Division
Radiation Detectors : Detection actually means measurement of the radiation with its energy content and other related properties. The detection system.
Lecture 14. Diagnostic equipment of the accelerators
More Circuit Components: Capacitors, Inductors, and Diodes
Basic Principles for Design of Ignition Systems
Results of A Compact Reflex Triode With Multi Cavity Adjustment
Presentation transcript:

Technical Issues: Approach: Construct a system that will allow high frequency, high voltage switching to monitor the recovery rate and jitter of different gases and gas mixtures from atmospheric to high pressures (1000 psi) Construct a parallel test system for material lifetime and geometry evaluation Payoff: High rep-rate low loss switch for pulsed ring- down applications. End Goals: Allow accurate switching for a pulsed ring down phased array antenna that has both good recovery rate and low jitter Accomplishments: -Completed project design and construction -Integration and improvement of project subsystems -Basic diagnostics setup and initial testing -Triggered repetitive operation (100Hz, 65 kV, 400 psi nitrogen) -Performed initial lifetime testing JITTER AND RECOVERY RATE OF A TRIGGERED SPARK GAP WITH HIGH PRESSURE GAS MIXTURES James Dickens, Use hermetically sealed high pressure spark gap design -Introduce a simple effective gas mixing subsystem -Fast diagnostics and data acquisition techniques -Modular design for both simple system integration and minimal corona and breakdown possibilities -System integrity at high voltages and high pressures

PROJECT DESIGN IMAGES Diagnostics Trigger High pressure gases Charge Line Switch Vacuum Charge resistor 6, 300 Ω HV resistors Load Containment Chamber HV Charger  Hermetically sealed  >300 psi  RG 220 (10m)  50 Ohm, 100 ns pulse, ~1 nF  >50kV, 25mA  Safety containment  Gas backfill accessible  SOS pulser  100 kV, 10 ns rise-time 1kHz in burst mode  >400V, 1.5 A power supply  >10V trigger  dry air, N2, H2, SF6  various gas mixtures 1” Lexan Cover Gas mix output Exhaust Gas Mix Chamber  Hold >1500 psi  Provide simple gas mixing Pressure monitor

Gas flow Copper tungsten electrode Kel-F lining G-10 housing Gas input RG220 fitting Set screw Switch Design

Spark Gap G-10 Housing Al Connecting Pieces CuW Electrodes KEL-F Liner Al Baffle

Polished CuW Electrodes

Eroded CuW Electrodes Electrode wear after ~10 4 shots Example of minimal erosion Ablation measurements indicate negligible material loss

PROJECT IMAGES HV Charge Line 125 KΩ Charging Resistor Feed-through for seal and corona reduction 50 Ω Load XHR DC Power Supply BNC 565 Pulse/Delay Generator

Project wave forms BNC trigger to capture 10 th pulse Rep-rated Self Break (30 kV, 30psi Nitrogen) Externally triggered 35 kV, 10Hz operation Signal from Capacitive V- probe Integral of Capacitive V- probe signal Triggered 35kV, 10Hz pulses

Lifetime Test Setup Main and peaking gaps pressurized to ~500psig Charging voltage = 90kVDC Trigger pulse is created by peaking gap self-break Voltage probes on the load side of peaking and main gap record pulse

FY07-FY08 SCHEDULE  Improve system connections for enhanced power transfer and corona reduction  Test with higher voltage and pressure to improve rise-time and jitter  Compare rise-time and jitter of different gasses  Introduce gas mixtures and record effects on jitter and rise-time

Technical Issues: Initial condition integration into model. Accurately accounting for material properties and effects. Proper modeling of a closing switch and the effects of jitter. Approach: Construct an accurate model of a single element pulsed ring-down antenna using the Comsol Multi-physics software package allowing exotic antenna structures to be evaluated before they are physically constructed. Payoff: Far field energy deposition for neutralization of Improvised Explosive Devices (IEDs) at long range distances. End Goals: Be able to accurately model and simulate various multi-element antenna structures and the effects upon the performance of a pulsed ring-down phased array. Accomplishments: Achieved accurate results of multiple antenna structures in a 2-D and 3-D regime using transient analysis. Constructed a two element array to demonstrate beam steer and the effect of high switch jitter. Achieved numerical results for energy density and magnitude at various far field points. Pulsed Ring-down Multi-Element Antenna

2-D and 3-D Modeling Monoconical Antenna 2-D Dual Dipole Array 3-D Electric Field 2-D Electric Field 3-D

Beam Steering

Far Field Results

PRDS array Example: radiated electric field for four dipole sources (spaced ½ wavelength apart), with no switch jitter Simulated single source radiated electric field waveform: Peak electric field vs. direction, measured relative to that received from a single source:

PRDS array Example: radiated electric field for four dipole sources (spaced ½ wavelength apart), with uniformly distributed switch jitter from 0 to ½ period (1 single shot) Simulated single source radiated electric field waveform: Peak electric field vs. direction, measured relative to that received from a single source:

PRDS array – Monte Carlo simulation Difficult to solve analytically for output variable statistical distributions given switch jitter distributions Use Monte Carlo method: simulate many firings of an array to build up output statistics Inputs: array parameters, simulated or experimentally measured switch jitter distributions Status: basic simulation is functional

PRDS array – advanced concept Sources mounted on multiple vehicles Firing controlled using GPS timing, coordinated to place “hot spot” on desired location High rep-rate sources could be controlled to rapidly scan an area Modeling to include GPS timing and position errors in addition to individual switch jitter

FY07-FY08 SCHEDULE Complete the Comsol model that accounts for material properties, initial charging conditions, and closing switch characteristics. Compare model to experimental results and adjust accordingly to match. Design and model various antenna structures along with the performance results when in an array. Examine the affect of jitter on a compact array (2 ft- 5ft antenna distance) and a large mobile array (2 m – 15 m antenna distance)

Technical Issues: Scaling laws and physics of ultra-fast switching are unknown Approach: Empirical analysis of fast switching gas Pulses: <150 ps rise, <300 ps FWHM V(t), I(t) with 50 ps sampling rate X-ray analysis through fast PMT Streak-camera luminosity analysis FEM analysis of geometric gap transition Distributed Monte-Carlo electron motion / amplification simulations Payoff: Scaling laws and design criteria for ultra- fast switching. End Goals: Improve transmission line switching for antenna coupling. Accomplishments: Empirical results –Gap currents determined through lumped parameter modeling –Formative delay times quantified –Runaway electron analysis –Ultra-fast luminosity imaging Monte-Carlo Analysis –Determination of electron multiplication rates –Direct calculation of space charge formation –Results support empirical analysis Ultra-Fast Gas Switching

PROJECT IMAGES 1) Experimental Setup 2) Essential Experimental Results Formative delay times as a function of pressure for different voltage amplitudes from kV. Streak-Camera results show breakdown structure as a function of time. The images show a region of high ionization near the cathode. The slope in the luminosity shows the transit time for the gap. Background gases are Argon and Dry Air with pressures from high vacuum to atmosphere. Rexolite lens between coaxial to biconical geometric transition limits wave distortion. FEM simulation of open gap for line characterization (time not to scale).

PROJECT IMAGES 3) Monte Carlo Simulation 4) Simulation Results Cathode Anode Electron amplification rates for varying pressures and field amplitudes can be combined with models to predict delay times. Space charges in the vicinity of the cathode lead to local fields on the order of the applied field. Ionization mapping shows a high ionization region near the cathode similar to the empirical results. Past this region electrons tend to accelerate to runaway velocities limiting further ionization. Simulations run on 32 node Beowulf cluster. Capable of > 5 Gflop/s Efficient internode communication using the standard message passing interface (MPI) Simulation based off null-collision method for determining collision type.