t2 f wireless power transfer
TRANSCRIPT
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Wireless PowerTransfer
John M. Miller
Matthew B. Scudiere
John W. McKeeverCliff White
for:
Oak Ridge National Laboratory's Power Electronics SymposiumFriday, July 22, 7:30 AM3:30 PM (EDT)Oak Ridge National Laboratory (ORNL) Conference Center,Oak Ridge, Tennessee
Patents Pending
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Introduction What is the Need?
There is need for an efficient method for transferringlarge power levels over moderate distances to hybridelectric vehicles (HEVs) in the near future:
First to parked vehicles,
Then expand to opportunity charging, and
Eventually to highway charging while driving.
Loosely coupled resonant mode transformers have the
potential to accomplish this. Magnetic resonance coupling for wireless power
transfer is termed WPT.
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Introduction Near Term Vision for WPT Electric vehicle charging must be:
Safe, compact and efficient in order to be convenient for customers Power levels commensurate with application:
3 kW to 7 kW residential and garage; 60 kW to >100 kW on-road dynamic
WPT alignment tolerance should be under closed loop DSRC control between
the transmit coil and vehicle mounted capture coil.
Graphics Left: J.M. Miller, Wireless Power Transfer for Electric Vehicles, PREA meeting, Utah State Univ, Energy Dynamics
Laboratory, Ogden, UT, 7 Feb. 2011
Right: J.M.Miller, ORNL internal presentation.
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Background: Barriers to Success
Efficiency
across cascade of components >90%
coil-to-coil ~98%
Meet international field emission standards (ICNIRP and
ARPANSA)* Efficient high frequency power inverter (20140 kHz)
Implement vehicle to infrastructure (V2I)communications compliant with DOT recommendationsfor DSRC
* International Commission on Non-Ionizing Radiation Protection N RP, Secretariat, c/o Gunde Ziegelberger, c/oBundesamt fur Strahlenschutz, Ingolstaedter Landstrasse 1, 85764 Oberschleissheim, Germany.
* The Radiation rotection Series is published by the Australian Radiation Protection and Nuclear Safety Agency(ARPANSA)
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Background: Measures of Success
Interoperability Any OEM vehicle with any WPT charger
Means coil size fixed, operating frequency fixed, alignmenttolerance & emissions fixed and communications fixed.
Safety and emissions
Transparent to vehicle occupants
Communications
DSRC following U.S. DOT recommendations for V2I
Private and secure
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Objective: PEV Stationary WPT Charging
Solution demands a system design that focuses on utility tovehicle battery terminal overall efficiency
SAE J2954 targets plug-battery efficiency >90%
Zone 1: Active field, ~1m2,
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Objective: Integrating WPT into a PEV
Solution: Design and develop coupling coil system suitablefor vehicle integration for stationary and on-road stationary at
high power levels (SAE Level 2: 3 kW to 7 kW) & high eff.Technically: a non-radiating, near field reactive zone power transfer method
Practically: a convenient, safe and flexible means to charge electric vehicles.
Vehicle to WPT communications
RFID localizer for positioning
Use existing on-board charger,
or dedicated fast-charge and
energy management strategy
Active zone field meetsinternational standards (ICNIRP)
Smart grid compliant utility feed
and modern power electronics
Graphic: Lindsey Marlar ORNL graphics services
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Approach: ORNL WPT System
Synthesize the driving point high power waveform, magnetically couple, rectify
and deliver charging power to the vehicle on-board energy storage system.
Isupply
Vdc_linkItransmitter
Vcapacitor
Vload
Iload
HALF-BRIDGE INVERTER
Vtransmitter_in
CONSTANT
VOLTAGE
LOAD
RECEIVERTRANSMITTER
Ireceiver_
loop
Rectifier
Series-parallel L-C magnetic resonant coupling
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Approach: Analytical PerspectiveWireless power transfer to unloaded vs. loaded coupling
Maximum impedance
frequency unloaded:
fo1 = 24.8 kHz
fo2= 25.6 kHz
fzmx~ fo1
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Approach: Analytical Perspective
For S-P resonant coil system the operating frequencies shift due to:
Degree of receiver coil loading (charging power demanded)
Coefficient of coupling between coils (vehicle receiver coil to transmit pad gap)
Tuning of various receiver coils relative to transmit coil tuning.
Coupling mode theory facilitates
understanding the fundamentals of WPT
and what parameters are key to optimized
performance.
During vehicle ESS charging the presence
of a dc potential at the secondary forces the
current and voltage responses to be very
nonlinear: fzmxto fzmntransitions
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Approach: Analytical Perspective
Resonance shifting is not an issue for stationary wireless charging, but
For on-road dynamic charging is an issue
Will require dynamic load tracking and inverter control using DSRCIllustration of ideal cases: k= 0.3, 0.22, 0.15, 0.1 and RL=2.5
Then, k=0.22 and RL= 5, 2.5, 1.8, 0.8
For a given value of coupling coefficient, k, the maximum power transfer occurs
when the reflected load matches the surge impedance of the system.
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Timeline and Milestones
Duration
(mo)
Task Milestone
2 Resolve instrumentation issues on laboratory sensorsand monitoring equipment. Validate accuracy at
WPT operating frequency
Manufacturer contacted, sensor/equipment
calibration validated and documented.
10 Design, develop and fabricate a SAE level 2 WPTcharger rated 7 kW at PF and frequency level
dictated by vehicle systems team.
Demonstration and validation against program
targets using laboratory WPT apparatus. Verify
that 20 kHz < f < 140 kHz is attainable.
6 Analysis, model and simulation of level 2 WPTcharging system
Validate simulation against laboratory apparatus to
extent possible.
4 Extend WPT design to next generation coil andevaluate performance against targets.
Next generation coil design meets specifications
8 Develop vehicle integrate coils and install on mulevehicle.
Demonstrate WPT to vehicle mounted receiver coil
and passive load. Validate targets met.
8 Procure DSRC and integrate into mule vehicle andinterface to vehicle CAN (w/ OEM help)
Demonstrate WPT to mule vehicle battery pack
with grid converter regulation via DSRC.
3 Validation of stationary charging at 37 kW usingDSRC for regulation and messaging.
Must demonstrate that power, plug to battery
efficiency, magnetic field emissions and packaging
constraints are met.
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Summary of Accomplishments
Prior LDRD developed Evanescent Power Transfer apparatus is used for testing
Alternative coupling coil designs directed research activities into ac resistiveeffects contributing to coil losses: skin and proximity effects
Analytical work continues on both parasitic effects and on application ofmagnetic vector potential to the coupling field itself.
Coil designs aimed at vehicle integration are not covered in this presentation.
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Summary of Accomplishments
Validation of laboratory instrumentation accuracy
Current sensor calibration at high frequencyInstrumentation errors due to low power factor (Agilent LCR)
Error in losses due to current redistribution in conductors
Reconfigured the WPT apparatus for:Initial 120 Vdc lamp loads (series connected), to
240 Vdc (parallel connected), to
270 Vdc using new, higher power bulbs.
Refinement of DSP load voltage regulator.
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Summary of Accomplishments
Developing deeper understanding of transmit and receiver coil
electromagnetic behavior Experimental finding that multiple ribbon coils operating in parallel
offer no benefit in terms of loss reduction.Two such coils in close proximity (~15mm) exhibit virtually unchanged Racand Ls
Top: End on view of flux lines for 3 turn ribbon coil antenna. Bottom: end on view of ribbon coil conductor current density plots
shown extensive skin effect and proximity effects in two outside bars.:
:
Source: Field flux plot simulation: Dr. Pan-Seok Shin
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Summary of Accomplishments
Developing deeper understanding of transmit and receiver coil
electromagnetic behavior
Plot of coil field at 20kHz excitation in air
L and R of Ribbon Antennae
12
13
14
15
16
17
18
1 10 100
Frequency, kHz
Inductance
(L),
H
0
5
10
15
20
25
30
35
40
45
50
Resistance
(R),m
L_1_3-turn ribboncoil
L_3_3-turn ribboncoils
L_4_3-turn ribboncoils
L_4_3-turn Cu tubecoils
R_1_3-turn ribboncoil
R_3_3-turn ribboncoilscoils
R_4_3-turn ribboncoils
R_4_3-turn Cu tubecoils
untt:
u
u
r
.:
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n/
u
/
-.
-
/
-.
-
/
-.
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/
-.
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Anamolous Racbehavior at 12 kHz has been
resolved and found to be due to LCR meter
Source: coil CAD drawings courtesy: Dr. Matthew Scudiere, Laboratory test data: Dr. John McKeever
Field flux plot simulation: Dr. Pan-Seok Shin
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Summary of Accomplishments
Validated coefficient of coupling, coil spacing, and alignment sensitivity of WPT
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Future Work
Develop design for grid converter and communications (base side)
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Future Work: WPT Communications
Source: Walton Fehr, Mgr. Systems Engineering, U.S. Dept. Transportation, Layered
Communications Enabling V-I Applications: Connected Vehicle Core Systems, 12 June 2011
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Future Work: Design Considerations
Power inverter must match the WPT network
Analysis of efficiency considered inverter kVA/kW requirement
Off resonance kVA/kW rating can be excessive
Therefore, inverter must maintain close tracking of coupled power factor
Further study of secondary rectification and filtering stage mustbe performed.
ORNL internal power inverter development supports the WPTsystems project
Industrial partner would greatly accelerate progress in WPT forLevel 2 stationary charging case.
Transition from laboratory to in-vehicle
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Topics to be Addressed for WPTVehicle Integration
Interoperability with existing Electric Vehicle Supply Equipment
Recommend stationary charging demonstration as 1stin-vehicle appl.
Field shaping and shielding for vehicle mounted receiver
Minimize loading due to proximity with vehicle chassis, and
Insure WPT will not corrupt CAN network(s)
Comply with International Regulations (ICNIRP)
ORNL WPT has 15 from antenna at 4kW
ICNIRP requires
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Conclusions
Only need a simple design to efficiently transfer large power
levels over moderate distances.
Demonstrated >4 kW at 10 separation with 92% transferefficiency.
Can be constructed with commercial-off-the-shelf components(20 kHz IGBTs).
Challenges being addressed by the ORNL team:
Minimization of coupling coil ac resistance effects,
load tracking and compliance with interoperability, power inverter kVA/kW limits and
appropriate vehicle to grid side communications.