demonstration of year 1 prototypes and testing methods
TRANSCRIPT
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ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
SECURE Projectsponsored at UC Berkeley by the
California Energy Commission
Richard M. White, EECS Dept.
Sensor Team
15 August 2008
Berkeley Sensor &Actuator Center
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ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 660 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
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ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 240 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
Wireless passive proximity measurement of AC current, voltage, phase, power
BASIS:MEMS
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ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 240 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
Wireless passive proximity measurement of voltage, current, phase, power
Demand Response
Fault detection
Metering
System monitoring,
control
System monitoring,
controlAPPLICATIONS
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System monitoring,
control
ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 240 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
Wireless passive proximity measurement of voltage, current, phase, power
Demand Response
Fault detection
Metering
System monitoring,
control
Energy scavenging from energized circuit via sensor + efficient rectifier
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System monitoring,
control
ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 240 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
Wireless passive proximity measurement of voltage, current, phase, power
Demand Response
Fault detection
Metering
System monitoring,
control
Energy scavenging from energized circuit via sensor + efficient rectifier
Conductor temperature measurement
Line sag measurement
Vegetation growth detection
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System monitoring,
control
ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 240 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
Wireless passive proximity measurement of voltage, current, phase, power
Demand Response
Fault detection
Metering
System monitoring,
control
Energy scavenging from energized circuit via sensor + efficient rectifier
Conductor temperature measurement
Line sag measurement
Vegetation growth detection
Assessment of U/G
cable aging
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System monitoring,
control
ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
AC RMS VOLTAGE
120 240 V 4 69 KV 115 KV and up
Residential/Commercial Distribution Systems Transmission Systems
Wireless passive proximity measurement of voltage, current, phase, power
Demand Response
Fault detection
Metering
System monitoring,
control
Energy scavenging from energized circuit via sensor + efficient rectifier
Conductor temperature measurement
Line sag measurement
Vegetation growth detection
Assessment of U/G
cable aging
Remote (non-MEMS) field-based voltagemeasurement
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Specifics
Assessment of U/G
cable aging
Staffing: Giovanni Gonzalez, Michael Seidel, Bo Zhang; Igor Paprotny (Post-Doc with
MEMS experience joining Sept. 1)
Off-Site:
3 grad students and Prof. White visited and did experiments at Steven Boggs lab (U.
Conn.) in May, 2008.
Prof. White attended EPRI-NEETRAC meeting in Chicago in June 2008 (NEETRAC offerfrom Nigel Hampton to test our sensors there).
Review of Five Proposed Methods for Studying In-Service
Cables (from our Workshop held 25-26 February 2008)
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Five Methods for Studying In-Service Cables
1. Measure, with small probe, dependence on instantaneous appliedvoltage of permittivity of cable insulator, and determine nonlinearity
2. Probe electric fields or potentials just outside cable to infer insulator
permittivity, and determine nonlinearity as applied voltage changes
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COMSOL simulation (by Piero Marcolongo, Prof. Evans student) of
electric potential shows substantial AC potential exists just outside
jacket between adjacent concentric neutrals, and that its amplitude is
affected by permittivity of insulator there. Will attempt with a properly
shielded microsensor to detect this potential to measure insulator
properties at different times in applied voltage cycle looking for
nonlinearity.
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Five Methods for Studying In-Service Cables
1. Measure, with small probe, dependence on instantaneous appliedvoltage of permittivity of cable insulator, and determine nonlinearity
2. Probe electric fields or potentials just outside cable to infer insulator
permittivity, and determine nonlinearity as applied voltage changes
3. At cable end, measure currents in individual concentric neutrals to
identify open concentric neutrals (no current) and asymmetry (detectpossible degradation near concentric neutral wire)
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Five Methods for Studying In-Service Cables
1. Measure, with small probe, dependence on instantaneous appliedvoltage of permittivity of cable insulator, and determine nonlinearity
2. Probe electric fields or potentials just outside cable to infer insulator
permittivity, and determine nonlinearity as applied voltage changes
3. At cable end, measure currents in individual concentric neutrals to
identify open concentric neutrals (no current) and asymmetry (detectpossible degradation near concentric neutral wire)
AC current
sensor output
magnet
piezo cantilever
MEMS-based version of
passive proximity AC current
sensor. Permanent magnetcouples to AC magnetic field
to drive piezoelectric-coated
cantilever and produce proportional
AC voltage output
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Five Methods for Studying In-Service Cables
1. Measure, with small probe, dependence on instantaneous applied
voltage of permittivity of cable insulator, and determine nonlinearity
2. Probe electric fields or potentials just outside cable to infer insulator
permittivity, and determine nonlinearity as applied voltage changes
3. At cable end, measure currents in individual concentric neutrals to
identify open concentric neutrals (no current) and asymmetry (detectpossible degradation near concentric neutral wire)
4. Using pairs of concentric neutral wires as transmission line, from
reflections and/or loss infer insulator permittivity and loss as function of
instantaneous applied voltage to determine nonlinearity
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High-voltage pulsed source (electrostatic discharge tester, gift of
Kikusui Corp.) might launch usable pulse through jacketnon-destructively onto a concentric neutral wire transmission line.
Source voltages adjustable from -30 kV to +30 kV, central spike
1 ns duration, pulse shoulder to 60 ns.
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Five Methods for Studying In-Service Cables
1. Measure, with small probe, dependence on instantaneous appliedvoltage of permittivity of cable insulator, and determine nonlinearity
2. Probe electric fields or potentials just outside cable to infer insulator
permittivity, and determine nonlinearity as applied voltage changes
3. At cable end, measure currents in individual concentric neutrals to
identify open concentric neutrals (no current) and asymmetry (detectpossible degradation near concentric neutral wire)
4. Using pairs of concentric neutral wires as transmission line, from
reflections and/or loss infer insulator permittivity and loss as function of
instantaneous applied voltage to determine nonlinearity
5. Using surface guided wave, from propagation velocity, reflectionsand loss as function of instantaneous applied voltage, infer insulator
permittivity, loss and nonlinearity
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RF SOURCE
Surface wave RF transmission line with waves guided by
dielectric coated conductor. Low loss at high frequencies
(Goubau line). Conventional insulated distribution cablewould guide it. Its propagation characteristics might be
affected by dielectric nonuniformities in the cable insulator.
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Specifics
Assessment of U/G
cable aging
1. Interdigital sensor to measure dependence of insulator permittivity on electric field:
a. Simulation of test device
b. Designed/submitted photomask for Microlab fabrication TEST with solid
dielectric; TEST with short length of cable; PLAN TEST with energizedcable
2. Electric field sticking out of cable
a. Materials Team did simulation showing detectable external field:
can this be detected and is that useful?
b. Design/build an electrostatic sensor for use at power frequency
(we have an inexpensive commercial E-field sensor but it works well
only at very high frequencies) TEST with short length of cable
at 5 kV (Material Team lab)
(continued)
Where do we stand on these proposed techniques?
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4. RF transmission lines that are integral to cable concentric neutral wires
a. Tested earlier using 8-foot cable measuring transmission/loss
b. Analyzed two-wire line large loss so use strong external drive
c. Two sources now in house: spark coil (7 kV?); ESD tester (30 kV,
few ns pulse length) TEST with existing cable (8-foot)
HELP! WE NEED MORE NEW OR OLD CABLE ~ 100 FEET?
Specifics
Assessment of U/G
cable aging
(continued)
3. Instrumentation for measuring uniformity of concentric neutral currents:
a. Current detection test at Prof. Boggs lab with short length of cable
b. PG&E gift of current transformer from San Ramon lab for current source
c. Holder for current sensors designed/built
d. Obtained/mounting very sensitive 2-axis commercial magnetometer chip to
TEST on short length of cable, along with Berkeley current sensor(piezoelectric-coated cantilever with magnet)
e. SIMULATE external magnetic fields for different drive conditions (noise
issue)
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ELECTRIC POWER INDUSTRY APPLICATIONS OF MEMS
SUMMARY
1. Many possible applications for wireless MEMS sensors
2. Progress on in-service U/G distribution cable assessment
a. Simulation/design/start of fabrication ofinterdigital sensorto
measure voltage dependence of insulator permittivity (nonlinear?)
b. Considering design of sensor to detect electric field leakage from
cable to compare with simulation
c. Instrumentation/preliminary test of ability to measure CN currentsd. Excitation of integral RF transmission lines to test cable irregularities
begun
3. Consideration of voltage, current, power sensing for distribution
voltages and higher