Title: Electromagnetics and Pulsed Power Laboratories and EMITION Center at UNLV
1Electromagnetics and Pulsed Power Laboratories
and EMITION Center at UNLV
- Robert A. Schill, Jr., Satya Radhakrishna, Hari
Krishnan, Shaoru Garner, Brandon Blackstone,
Greggory Cornell, Richard Kant, Stan Goldfarb,
and Ved Nayyar - Department of Electrical and Computer
Engineering
- University of Nevada Las Vegas
- 4505 Maryland Parkway
- Nevada, Las Vegas 89154-4026
- Phone (702) 895-1526 Email schill_at_ee.unlv.edu
- http//EMandPPLabs.nscee.edu
2GOALS OBJECTIVES
- Goals
- Motivation to hypothesis driven research
- To display/exhibit/highlight research efforts in
EM and PP Laboratories
- Encourage collaboration
- Objectives
- Expound on a variety of research directions
- Note specialized equipment and modeling
infrastructure
3MOTIVATION TO RESEARCH
- What is Pulsed Power?
- Pulsed power is the ability to expend a finite
amount of energy over miniscule time intervals in
localized regions in space.
- Broad Application Objective
- Pulsed power (electrical, EM, optical, and/or
charged particle beam) has the potential to
selectively influence, manipulate and/or
sculpture particular physical mechanisms. In
general, physical processes occur over different
spatial and temporal scales. Therefore, the
objective is to couple pulsed power energy into
desired physical processes without inhibiting or
enhancing other processes that normally exist. - Consequence
- Managing the electromagnetic spectrum entwined
with material interactions captivates the essence
of ones ability to harness ones future.
- Experiment
4NEVADA SHOCKER
Anode
Marx Bank (MB)
Diode
Blumlein (BL)
Cathode
- Understanding the data requires understanding the
machine
Blumlein Coil
Water/Vacuum Plastic Barrier
5NOVEL ELECTRICAL SENSOR
- Novel Differential Dot
- Wide bandwidth Matched
- Symmetry
- Natural as a differential B-dot
- Shielded B and D - Dot combined
- No solder connections
- Patent Pending
- Calibrated for Magnetic Field
- Frequency domain
- Sig. Generator 1.5 GHz max.
- Student thesis
Novel Dot
6NEVADA SHOCKER - ANATOMY
- Experiment/Equipment
- Scopes Marx bank triggered
- 5 Scopes TDS 6604B (6GHz, 22Gb/s)
- Four dot detectors on 1.25 rad 5,6,7,8
- Embedded 1 mm below electrode surf.
- Vac. Press. 7.5X10-6 2.5x10-6 Torr
- Plastic Rexolite 1 dia., 1 and 2 long,
polished, 30-50 psi exerted on ends
Front Side
Back Side
7REXOLITE POLISHING HISTORY
- Crazing - Multitude of very fine cracks in the
matrix material
- Stress exceeding tensile strength of plastic
- Ex. Shrinkage, machining, impact shocks,
temperature
- Transition temperature 114oC (Rexolite surface
gels)
- C Lec Plastics Inc. (1 dia. rod stock)
- Cast the plastic - Sample shrinks unevenly
- Wet grounded to 1 dia. (rod surface - opaque
frost-like)
- UNLV Polishing Procedure
- Initial preparation - Band-saw cut
- Rough polishing in lathe (320 rpm) - 2 minute
procedure
- 3M Super Duty rubbing comp. microfiber cloth
T120o C
- Cleaned with water or 200 proof alcohol
- Fine polishing in lathe (320 rpm) - 4-5 minute
procedure
- Light Duty 3M Perfect-It II rubbing compound
T75o C
- Ave. optical opacity - 1.17 with stand. dev.
0.048 (15 samples)
Grain effect due to polishing
Magnification 20x optical, 150 digital
8RGA DATA NEVADA SHOCKER
- Water Vapor- Abundant
- 1 H,16 O,17 HO,18 H2O
- Atm.Leak (4 x more N2 than O2)
- 16 O, 28 N2, 32 O2, 40 Ar
- 44 CO2 -- elastomeric O-rings
- Fluorine(Teflon Cleaning Comp.)
- 19 F, 20 HF
- Hydrocarbon Fragments (CiHk)
1
91 AND 2 LONG, 1 DIA. REXOLITE SAMPLES, 2.5e-6
TORR
2 SAMPLE
1 SAMPLE
D
D
H
H
- Virgin Sample Distribution (Water switch - normal
position)
- Approx. sixty samples 1 2 long, 7.5e-6
2.5e-6 Torr
- Observed an open circuit charging characteristic
and then a short circuit behavior. Breakdown
resulted.
10SINGLE WIRE IMPLOSIONS
- Motivated by Flashover Studies
- With the large mismatch present in the system, is
there enough current to vaporize a copper wire?
- Typical flashover shot when a 0.25 mm wire is
attached with nail polish to a 1 polished,
virgin Rexolite sample.
- Unoptimized conditions, the copper wire vaporized
coating the plastic surface.
- UNR Sandia collaboration
11LASER STIMULATED DESORPTION
Desorption Test Stand
Optically Mag. And Digitally Enhance
d
- Empty Chamber 1e-10 Torr
- Localized excitation NdYAG laser
- Enhance subsurface diffusion of gas contaminants
leading to desorption
- Flashover fine gas layer present between hard
vacuum and solid
12ANALYSES
RGA
Laser Beam
Laser Plastic
- MATLAB
- Imaging interrogation tools
- Residual Gas Analyzer (RGA)
- Measures the partial pressure of gas released by
the medium
13INTERFEROMETRY SETUP OPTO-MECHANICAL MATERIAL
PROPERTIES
Universal Testing Machine
- Hypothesized Research
- Hardware
- Universal Test Machine
- Optical Components
- CCD Camera
- Optical Modeling Software
Sample Under Test
Mirror
Beamsplitter Cubes
14LIGHT INTENSITY, SPATIAL POSITION, COLOR
ANALYSIS
Intensity plot superimposed on image
Experiment
- Spatial Intensity Distribution
- VIBGYOR order of intensity profile
- Experimental and computational agreement
- MATLAB
- Imaging interrogation tools
- Shift in fringe corresponds to a mechanical
pressure
Simulation
15SEE TEST STAND
- Electron Gun
- Particle Position Detector
- Manipulator Arm
- Cryostat Rotary Table
- RGA Pressure Gauges
- Rough/Turbo/Cryo Pumps
16SURFACE SAMPLE POLISHING
0.5 mm Reticle
Grid Reflection
- Electropolish Technique
- Cornell Univ. - Two samples
- Surface removal no less than 125 microns
everywhere except inside grooves
- Buffered Chemical Polish
- LANL - Six samples
- Surface removal - 98 microns
- 112 ratio hydrofluoric acid, nitric acid,
phosphoric acid
- Temp. 8 - 10 oC
17ELECTRO-POLISHED - 1 keV Prim. Beam
0O Beveled Surf. (Normal Incidence)
15o Beveled Surf.
30o Beveled Surf.
Proc. Count 935
Proc. Count 2136
Proc. Count 604
CG(-4.45,-21.45) SD(7.81,9.01)
- As the angle of incidence increases, the
distribution of SEE shifts radially outward along
the detector surface
- Aperture opening in the detector may be observed
- 0o 15o incidence - most SEE lost to the
aperture opening
- Aperture masks the SEE spatial distribution
allowing for study of the tail ends of the
momentum distribution.
- 30o Center of Gravity (CG) of SE distr. and
standard deviation (SD)
18DETAILS SEE FROM 1 keV PRIMARY ELECTRON BEAM,
30O EP SAMPLE
19MONTE CARLO SIMULATION RESULTS
- Monte Carlo Code
- Original Version (valid 50 eV)
- Dr. David Joy, Univ. of Tenn.
- Modified Vers. (added near surf. Effects tracks
of all SE generations)
- Dr. Richard Kant, UNLV
- Microscopic, single scatterer approach to follow
the primary and all generations of secondaries
through the collision cascade
- Output - Initial energy/mom. dir. cos.
- Logistics
- 100,000 primary electr. launched
- 100 eV large concentration between 40-50 eV
- 1keV large concentration between 0.9 and 1 keV,
and structure around 50 eV
0.1 keV Primary
30o Beveled Surf.
1 keV Primary
20SIMULATION vs EXPERIMENT
- Logic
- The SE Monte Carlo code predicts BSE
- Based on specular arguments, exp. data has been
masked to observe the BSE
- Anticipate- SEs favor emission in specular dir.
- All initial particle trajectory conditions
(energy/ mom. dir. cos.) for the standard
deviation extrema from the average final position
of the SEE distr. as measured on the detector are
determined with a particle tracking code. - Initial conditions of final extrema positions are
plotted. All possible initial conditions should
lie in between these curves. If SEE is uniformly
distributed about the detected specular electron,
the ave. initial conditions of the Monte Carlo
BSE distri. should be central to experimental
curves. - Good agreement shown
30o Beveled Surf.
EP (similar for BCP)
Ave. initial condition stand. deviation from
Monte Carlo Sim.
EP
21ANTENNA ANALYSIS
- Dielectric encapsulated antenna 2.45 GHz. at 10
bandwidth 30 x 30 x 15 mm
- Theory - Near and far fields with dielectric
material
- Computational modeling
22MODELING SOFTWARE
SEE Matlab
- LSP MAGIC
- WAVICA RAYICA (Optica Inc.)
- MICROWAVE OFFICE - New
- ELECTRONIC WORKBENCH
- MONTE CARLO SECONDARY ELECTRON EMISSION
- MATLAB
- FIELD PRECISION EM SOFTWARE
30 million Incident Primary Electrons
Magic 3D
Wavica
Matlab Data Acquisition Software of Detector
RGA on, ion gauge off, grid 150 V
RGA off, ion gauge off, grid 150 V
RGA off, ion gauge on, grid 150 V
23Energy Material Interaction Technology Initiative
of Nevada Center - EMITION Center
- Focal Areas
- Pulsed power device technology
- Applications of pulsed power Materials science,
Biological/Medical science, Environmental
science
- The EMITION Center is dedicated to the study of
pulsed power (both the electromagnetic type and
the particle beam type) and its interaction on
materials with these focal interests in mind. - It is anticipated that a modest, dynamic, user
research facility with unique capabilities will
attract on-site experimentation of non-university
entities while simultaneously enhancing the
centers expertise and usefulness to the pulsed
power community.
24RESEARCH COLLABORATION OPPORTUNITIES?
- Pulsed power computing and communication
- Burst of information condensed in a single pulse
- Optical and Pulsed Wideband Microwave Imaging
- Charged particle imaging
- Optical Computing
25CONCLUSION
- Cool Page (Motivation, Target, Strategy)
- Gen. community, Grade High School (HS)
College
- Story Line -
- Xenon (from Zaro II) visits UNLV EM Lab
- Tools for Travel
- Four fundamental forces introduced
- HS phys. - calculations conversions
- Microwave, Visible, and EM spectrums
- Plasmas, Lightning in Box (Nevada Shocker),
Materials, and Sensors
- Tour the EM and Pulsed Power Labs
- Community Service
- Webpage
- http//EMandPPLabs.nscee.edu , http//emandpplabs.
nscee.edu/cool/coolpage.htm
26COMMUNITY SERVICE / TEACHING
- Scouts
- Childrens Leid Museum
- Interesting Web Page with Cool Stuff
http//EMandPPLabs.nscee.edu , http//emandpplabs.
nscee.edu/cool/coolpage.htm
27National Visibility
- Seven-minute news clip on Academic Café regarding
the Nevada Shocker pulsed power device. Academic
Café broadcasts high profile research and events
on public television to the community Robert A.
Schill, Jr. and William Culbreth. Filmstrip
may be viewed at the bottom of the webpage
http//emandpplabs.nscee.edu/communtyservice/pro/p
resenats/realpresentons.htm - High Profile National Visibility - UNLV
visibility in a Multidisciplinary University
Research Initiative (MURI) program, ranking UNLV
with MIT, Berkeley, and the University of
Wisconsin Madison. Please refer to the webpage
at http//cathwinmuri.ece.wisc.edu .
28NEVADA SHOCKER - PROBES UPGRADES
- Sensor Locations
- Machine Upgrades
- Water switch
- Diode electrodes
Fiber Sensor B/D-Dot
Resistive Probe Upgrades
29NS CHARGING/DISCHARGING DIODE PHYS.
- Resistive Coil (Displays 4 distinct stages)
- Charging stage (Low Freq.)
- Transition stage (Increase Freq.)
- Firing stage (Relatively Const.)
- Recover stage (High Freq. - reflections)
- Sums Diff. Dot (Rate of change ROC)
30NULL TEST
NULL TEST
2 SAMPLE
D
D
H
D
H
H
H
- Null Test
- A 0.185 thick aluminum plate covers anode.
- 2 long, 1 dia. Rexolite sample betw. cathode
null cover
- Compare Null Test to 2 Sample Test
- Overall ampl. of D H decreased by a factor
betw. 4 8.
31CONCLUSIONS
- Based on electrical diagnostics, flashover has
been observed.
- Gross 10s to 100s ns resolutions show
tendencies
- Nanoseconds and subnanoseconds resolutions will
offer information on relative time displacements
of signals
- This provides more localized information of the
flashover event lending itself to statistical
analysis of the position and time of the event.
32EXPERIMENTAL PROCEDURE
- Sample placement
- Crudely by hand
- Pumps on
- Finer placement with manipulator arm, electron
gun (EG) Faraday cup at 5e-9 Torr
- Cryostat on at 5e-9 Torr
- Diagnostic measurement on primary electron beam
- RGA measurements pressure measurements
- RGA pres. gauges off - particle position
detector (PPD) on
- Determined location of each bevel surface using
PPD EG - position recorded
- Perform exp. on virgin sample surf. at particular
beam energy
- Between each change in primary beam energy - PPD
turned off and RGA, pressure, and beam
characteristics recorded
33LUMPED CIRCUIT PARAMETERS
34TYP. OPEN AND SHORT-CIRCUITED DIODE SIGNATURES
FIRST 1.75 mS
2 long, 1 dia. Cyl. Al short
OPEN
SHORT
D
D
H
H
2 Gap
- 8 samples 32 field histories
- High freq. riding on low freq. (water switch
fired early electrodes too close)
- Shark tooth signature observed for D
- Definite phase relation
- Const. charging/discharging pattern t310ns
- Short surf. current order of mag. larger open
- Ave. charge density for open short same
- Note opposite polarity for surf. currents
- 6 samples - 24 field histories
- Surf. charge builds up 1.6 ms
- Small diode capacitor charges faster than
Blumlein coil discharges
- Marx bank supplying sign. amount of energy
water switch fired early
- Surface current max 5e5 to 1.75e6 A/m
- Low freq. signal vs high freq. signal
35TYP. OPEN AND SHORT-CIRCUITED DIODE SIGNATURES
AT TRANSITION
- Electric Flux Density
- Zero until MB fires (circled region) - transition
to rel. constant charge
- At transition pnt, large energy surge from BL to
MB by passing BL coil
- Radial Magnetic Field Intensity
- MB and BL transition points obvious
- Electric Flux Density
- Slow init. charging leads to const. rs
- 270 ns large D rs (20 ns fall time)
- Radial Magnetic Field
- From 0 to 100ns Approx. zero
- 100 to 280 ns Grows slowly
- 280 to 500 ns Rel. rapid growth
36OPEN CIRCUITED DIODE - RESISTIVE PROBE
H
D
RP
RP
- As MB charges, diode appears to charge
- MB fires - Blumlein (BL) charges the diode
charge density remains approximately constant
- Water switch fires Coil blocks forefront of
pulse
- Roughly 5-6 ns later - large Drs on diode
constant change in radial surface current
density
- About 20 ns later (transition point) the surface
current density grows faster
371 LONG REXOLITE SAMPLE SHORT-CIRCUITED DIODE
SIGNATURES-WATER SWITCH SHORTED
1 SAMPLE
SHORT
D
D
D
D
H
H
H
H
- One Inch Sample
- The diode cap. is small enough to charge to the
level of the discharge through the inductor in
series with the resistor probe as if it (CD)
where not present on the time scale of the
discharge of the MB through the BL coil. - Short
- Resistance of the diode short is much smaller
than that of the resistor probe such that the MB
is discharging directly through the diode
- The dist. of sep. of the water switch electr. in
normal position is far from optimal. Low freq.
signal content in earlier figs. is due to the MB.
381 LONG, 1 DIA. REXOLITE SAMPLE WATER SWITCH
REMOVED
D
D
H
H
- Low Freq. MB Charging Removed
- Open Circuit Charging and Short Circuit Breakdown
Characteristics Observed
- Continued effort
39ACOUSTIC WAVE STUDIES
- Correlate flashover based on acoustic and dot
studies
40Optical Modeling Tools
- Optical Software
- Ray Optics - Geom. Optics
- Wave Optics - Physical Optics
- Diffraction modeling
- 3-Dimensional
- Ability to custom build components and system
- Spatial intensity profiles and more
41Light Intensity and ColorAnalysis
Intensity plot superimposed on image
- MATLAB
- Analyze both color and intensity results obtained
from experiment.
- MATLAB programming capabilities to analyze
Wavica/Rayica in different ways for clearer
understanding and interpretation
42THEORY
- Governing Eqs.
- Static approximation (dh/dt 0)
- Duration of experiment and acoustic wave
determines number of monolayers.
b - brass p - Rexolite plastic
mn mass of nth monolayer hn displacement of nth
layer FEM Electromagnetic force on top layer of b
rass
43SEE TEST STAND SCHEMATIC DRAWING
- Gun-Detector Geometry
- Electron beam passes through center of particle
detector via beam drift tube
- Grid (72 transmission)
- 75x200mm wire 1mm2 hole
- Covers MCP of detector
- Cryostat
- First stage of cryostat partially surrounded by a
second stage oxygen free high conductivity (OFHC)
copper shield
- Mounted on rotary table
- Transfer Engineering Inc.
- Built vacuum system manipulator arm with diagn.
44TYPICAL OPERATING CONDITIONS
- Pressure (RGA - 5e-9 Torr)
- Water Vapor- Abundant
- 1 H,16 O,17 HO,18 H2O
- Atm.Leak (4 x more N2 than O2)
- 16 O, 28 N2,32 O2,40 Ar
- UHV epoxy used on pin-hole in welded bellows
- 44 CO2 elastomeric O-rings
- Typ. Pres.-5e-9 to 9e-10Torr
- Cryostat Temp. (Grease)
- Side 9oK Top 23oK(no pressure)
- Electron Beam Parameters
- Energies 0.1-3 keV (1 keV typ.)
- Dia. / Duration - 150 mm / 100ms
- Current 80pA-3.7nA (2.2nA typ)
- Grid Potential 100 150 V
- Alignment and Sample Geom.
Cryostat axis 2 mm off beam axis
Cylindrical sample - 4 beveled surfaces
45Specular Backscattered Electron Location
- Motivation
- Quantum mechanics - electron is treated as a wave
function
- Wave function has properties of an
electromagnetic (EM) wave
- An EM wave obeys Snells law of reflection
- Backscattered electron (BSE) energy is nearly the
same as the incident primary electron
- Location of Specular BSE for Different Beveled
Surfaces
- 0o and 15o beveled surface
- Lost in aperture opening (r12 detector units or
6.8 mm for 15o)
- 30o beveled surface
- Location r26.6 detector units or 15 mm, nearly
in middle of cluster
Specular Reflection qr qi
46DATA PROCESSING PRESENTATION
- Scattered Plots - Color and Location
- Detected SE count over a 281mm x 281mm sq.
- Pixel color signifies the number of electrons
detected in a bin 1 pixel is 281 x 281 mm sq.
- Aperture opening visible in scattered plots
- Data Processing - Count
- One is subtracted from all bins bins with counts
less than one are omitted
- Enhance the visibility of the BSE
- Removes dark counts (sparse random)
- Negligible dark counts due to short pulse
duration (2 - 6 total count)
- Total count detected offers information on
relative change in SEE
- Other forms of measure
- Center of gravity (CG) of SEE spatial distr.
- Standard deviation(SD) from CG
Before Processing Total Count 3137
NOTE 20 bins 10 det. units Dect. Length
45 mm
Approx. Det. Boundary
After Processing Proc. Count 1244
47SURFACE CONDITIONING BCP - PULSE WIDTHS NUMBER
SHOTS
- Pulse Width vs Rep. Rate
- Five 200 ms pulses yield a similar min.
conditioning effect as ten 100 ms pulses
- Ten 50 ns pulses yield a conditioning minimum
slightly higher than ten 100 ns pulses
- Fall and rise rates for a particular pulse width
is similar.
- EP Conditioning Rate is Slower than BCP but SEE
Minimum are Similar
1 keV Prim. Beam
200 ms
100 ms
50 ms
- Repeated beam impacts on
- single spatial location
- 30 s between each impact
- 1 keV primary beam, pulse current 2.2 nA
48SIMULATION LIMITATIONS
- SEE Monte Carlo Code-Limitations
- Model provides estimates for energies between 50
eV and 1 keV in the collision cascade
- Once below 50 eV, the charge is no longer
tracked
- If near the surface and the SE energy is betw. 20
eV and 50 eV, a random generator decides if the
particle is emitted from the surface
- Important Observations
- Literature suggests that true secondary electrons
typically have energies less than 50 eV
- SEE Monte Carlo Code in its present form may not
adequately predict the true secondary electron
emission
- Since the primary electron beam is low, tracking
results obtained from the SEE Monte Carlo code
should provide reasonable estimates for the
backscattered secondary electron (BSE) (Note BSE
have energies comparable to primary electron)
49OTHER INFRASTRUCTURE OF INTEREST
- Subnanosecond risetime pulser with pulse
sharpener
- Pulse widths 10 ns, 50 ns, 200 ns into 50 Ohm
load
- sharpener
- Shot log database
- Documentation is important
- Technician and scientist What are the real
environmental and experimental conditions?
- Secure Website for data transfer to offsite
location
- Polycold - more shots per day
- Safety Precautions
- New Hire
- Subcontract - K-Tech ?
50NEVADA SHOCKER DATA BASE LOG
51INVITED WORKING RELATIONSHIP
- To promote a long term research oriented working
relationship with proposal development roots.
- Talents exist and infrastructure is now in
place.
- EMITION pools multi-disciplinary researchers
under a single umbrella to push the state of the
art in a number of fields. Offers new ideas and
research resources. - Possible Funding Mechanism
- More cost effective to work as a consortium where
the funding agency would support each entity
independent of the other
- We would be the lead institution and all other
partners are subcontractors
- Overhead is charged for each subcontract up to
the first 25k, thereafter UNLV does not charge
overhead
52BUFFERED CHEMICAL POLISHED (BCP) - 1 keV Primary
Electron Beam
0O Beveled Surf.
15o Beveled Surf.
30o Beveled Surf.
Proc. Count 414
Proc. Count 164
Proc. Count 790
CG(-5.65,-20.32) SD(5.25,8.44)
- Observations - (Same trends as from the EP
sample)
- Significant loss of count for 15o incidence
compared to normal.
- 30o Beveled Surface
- On ave., proc. EP count is 2.3 times larger than
proc. BCP count
- Based on six BCP and five EP shots
- Lit. - rough surf. on a micro. level min. SEE.
Electr. emitted from the surf. inside of a micro.
groove may be recaptured by its walls.
53TRACKING SEE DISTR. VARYING GRID VOLT.
displacement
200 V
Approx. Aperture Boundary
1 keV Primary Beam 15o Beveled Surface BCP Samp
le
100 V
150 V
50 V
0 V
- Controlling Grid Properties - BCP
- Specular cal. indicate the CG of the SEE
distri. for the 100 V higher grid pot. is lost
to the detector aperture.
- At 50 V, the entire distribution is visible to
the detector.
- D200 V-displaced by 40 bin / 11.3 mm
- Controlling Grid Properties - EP
- Increasing the pot. displaces the center of
gravity of the distribution towards the detector
center.
- For a 150 V change, the distribution traverses 16
bins or 4.4 mm
54CONCLUSION
- A SEE test stand has been designed to study the
initial conditions of secondary electrons emitted
from niobium in cryogenic state.
- Secondary electron particle distributions have
been studied for 0o, 15o, and 30o beveled
surfaces
- BCP and EP samples have been compared showing
that the EP count is over twice as large as the
BCP count
- Electron beam surface conditioning was examined.
Conditioning appears to be sensitive to pulse
duration and the number of impacts
- Good comparison have been shown between
experiment and simulation
55INITIAL DIODE CHARGING
D
56NEVADA SHOCKER - TRANSIT TIME STUDY
57DIODE PHYSICS - JS AND rs
(ns)