Current Research and Development of Wireless Power ... · 2. Overview of Wireless Power Transfer...
Transcript of Current Research and Development of Wireless Power ... · 2. Overview of Wireless Power Transfer...
Current Research and Development ofWireless Power Transfer via Radio Waves
and the Application [DML]
Jan 25, 2018
@ University of Perugia
Naoki Shinohara, Professor,
Research Institute for Sustainable Humanosphere, Kyoto University
Contents1. Introduction2. Overview of Wireless Power Transfer via Radio Waves3. Wireless Power Transfer via Radio Waves in Far Field4. Toward New Radio Wave Regulation of WPT5. Introduction of Activities of WPT in IEEE and IEICE6. Conclusion
2
SHARP Airplane exp.1987@Canada
MPT to helicopterBy W. Brown 1964, 1968
MPT rocket exp.1983 by Kyoto Univ., ISAS
Island-Island MPT (150km)in Hawaii2008 by Kobe Univ., NASA
3
Introduction
Kyoto and Kyoto University
4
KyotoWinter
Autumn
Spring APMC2018 will be held at Kyoto.
- Kyoto Univ. Data (2015) -
Professors : 1,032 (5,445 Employees)
Students : 13,569 (Under Graduate)
4,773 (Master), 3,671 (Ph.D)
Novel Prizes (Prof. Yamanaka, Prof. Yukawa,
Prof. Tomonaga, Prof. Tonegawa, Prof. Fukui..)
Main Campus
Uji Campus
Kyoto Univ.
Kyoto Univ.
Tokyo
5
What is ‘Wireless Power Transfer’?
Power Transmission
・Power transfer frompower station to homevia wire
Wireless Communication
TV
Mobile
Radio
・Information transfer frombase station to uservia radio wave
+ =Wireless PowerTransfer (WPT)
・Power transfer fromtransmitter to uservia electromagnetic fieldor radio wave
Various Wireless Power Transfer
I
I
H
Supply
User
I
I
H
Supply
User
L
L
C
C
Resonance of L and C
Transmitter
Transmitted
Power
Receiver
→PowerOnly Carrier for WPT
Very Narrow
Electric Power
To User
Frequency
Time and
Space
Inductive
Coupling
(Magnetic)
Resonance
Coupling
Capacitive
Coupling
6
E
V
V
Radio Waves
(Microwaves)
RISH, Kyoto Univ.
Microwave Power Transmission Field Experiment in Kyoto Univ.
1993
Second MPT Rocket
Experiment
- ISY-METS -
1994-95
Ground-to-Ground
MPT Experiment
1996
Retrodirective
MPT System
Open Experiment
1983
First MPT Rocket Experiment
In the World - MINIX-1992
MPT Experiment to
Fuel-free Airplane
- MILAX -
2001
Solar Power
Radio Integrated
Transmitter
- SPRITZ -
2009
Airship-to-Ground
MPT Experiment
7
8
Jan., 1983, by Kyoto Univ.. and ISAS
9
Aug., 1992, by Kyoto Univ., Kobe Univ., CRL, etc
10
Power from Airship (50m above, 2.45GHz, phased array with two magnetrons)
March, 2009, at Uji, Kyoto, Japan
11
Overview of Wireless Power Transfer
via Radio Waves
Brief History of WPT• 1864 Prediction of Radio Waves by establishment of
Maxwell’s Equation based on Ampere’s law and Faraday’s law. (Radio waves was found in 1888 by Hertz’s experiment)
• Around 1900 Tesla carried out WPT experiment of both inductive WPT and WPT via radio wave (150kHz), -> faired
• 1960s W. Brown carried out beam-type WPT via microwave (2.45GHz) -> succeeded
• 1980s Commercial Products of inductive WPT (Shaver, IC card..)
• 1990s 1) RF-ID, 2) RF WPT toward Solar Power Satellite in Japan
• 2006 MIT group proposed resonance coupling WPT (revised inductive coupling)
• 2010s Various WPT – Standardization of inductive WPT, wireless charger for EV, energy harvesting from broadcasting waves, ubiquitous RF-WPT…
12
Various Wireless Charger Products
13
Inductive WPT (kHz-MHz) Radio Waves (Microwaves, GHz)
Silicon Valley’s Rumor (Nov., 2016)
• iPhone8 will install chip of Wireless Charging via Radio Wave by Energous
“With an Energous transmitter in your office, your phone will constantly be charging even while it’s in your pocket as you sit at your desk and work.”
14
https://www.bloomberg.com/news/articles/2016-01-29/apple-said-developing-wireless-charged-phone-for-as-soon-
as-2017-ijz3i4si
http://www.phonearena.com/news/Upcoming-iPhone-8-could-feature-wireless-charging-unlike-anything-weve-
seen-yet_id87639
Energous Receives Industry-First FCC Certification for Over-the-Air, Power-at-a-Distance Wireless Charging (2017/12/26)
The company's WattUp Mid Field transmitter can deliver power via radio frequency (RF) energy to WattUp-enabled electronic devices at a distance of up to three feet.
15
https://ir.energous.com/press-releases/detail/596/energous-
receives-industry-first-fcc-certification-for
t t
RF Amplifier Rectifier
(+ Antenna = Rectenna)
Transmitting
AntennaRF Choke
(DC Bias)
RF Choke
(DC Bias) DC
Block
VDD-VG
R0
Imp
ed
an
ce
Ma
tch
ing
Circ
uit (N
o
Lo
ss)
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
FET,
HEMT,
etc.
Imp
ed
an
ce
Ma
tch
ing
Circ
uit
an
d L
ow
Pa
ss
Filte
r
RL
DC
Block
Receiving
Antenna
Electromagnetic
ally
Uncoupled
Source
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
Diode
User
DC
I V I V I V I V I V I V
Wireless Power Transfer via Radio Waves
16
Field of Radio Waves
17
2
2
2
2
Dd
Dd
d
I : Reactive Near Field
II : Radiative Near Field (Fresnel Region)
III : Far Field (Fraunhofer Region)
[Antenna Element] [Aperture Antenna]
Electric Field from Aperture Antenna
in Near Field and Far Field
II : Radiative Near Field (Fresnel Region)
= Sphere Wave (Beam-type WPT)
III : Far Field (Fraunhofer Region)
= Plane Wave (approximation) (Ubiquitous WPT)
I : Reactive Near Field = Inductive WPT
Various Wireless Power Transfer via Radio Waves(a) Beam-type
(High efficiency with higher frequency)
(b)Ubiquitous-type (Low efficiency, like RF-ID)
(c) Energy Harvesting
(No power source)
Transmitter
Receiver
→Power
Time and Space
Information
Frequency
Wide
Electric Power
to User Receiver
→Power
Transmitted
Power
Transmitted
Power
Transmitted
Power
Transmitter
Transmitted
Power (Broad)
→ Electric
PowerOnly Carrier for WPT
Very Narrow
Frequency
Time and
Space
→ Electric
Power→ Electric
Power
18
(d) In Closed Area (like Waveguide)
Transmitter
Transmitted Power
Receiver→
Power
19
Future Dream of MPT:
Solar Power Satellite (SPS)
1GW Solar Power Station
2kmf Solar Cells
2kmf Microwave Antenna
< 10,000 ton weight
36,000km
Wireless Power
Transmission
via Microwave
2kmf
Receiving Antenna
Energy Availability Factor
Ground PV
: < 15% (Night, Rain…)
Space PV (SPS)
: >90% (No Night in 36,000km Orbit,
No Rain by Microwave Propagation)
-> SPS is huge, stable, and CO2-less
Power Station
Power Density~350W/ /㎡at rectenna center
~10W/ /㎡at rectenna edge
WPT Ground Test
Microwave
Beam
MPT Experiment on Feb. 2015Thin-High Efficiency Phased Array with GaN MMIC
55m
2.5cm thickness phased array
GaN MMIC Amplifiers
5.8GHz, 1.8kW
Developed by Mistubishi Electric Corp. (Phased Array), IHI Aerospace (Rectenna Array), Supported by METI 20
Nobel winner Hiroshi Amano and his team tap gallium nitride technology in bid to transmit power wirelessly from a distance (2018)
21
https://www.japantimes.co.jp/news/2018/01/15/national/nobel-winner-hiroshi-amano-team-tap-
gallium-nitride-technology-bid-transmit-power-wirelessly-distance/#.Wl0yf2cUmUl
“Our first target is to create a wirelesssystem to supply electricity to drones withinthree years,” Amano said.
The team has begun by developing a systemfor drones. With the cooperation ofJapanese electronic manufacturers anddrone developers, they are currentlybuilding a system with an electric circuit andembedded antenna.
22
Wireless Power Transfervia Radio Waves
in Far Field
Transmitter
Transmitted
Power (Broad)
→ Electric
PowerOnly Carrier for WPT
Very Narrow
Frequency
Time and
Space
→ Electric
Power→ Electric
Power
Transmitter
Receiver
→Power
Time and Space
Information
Frequency
Wide
Electric Power
to UserReceiver
→Power
Transmitted
Power
Transmitted
Power
Transmitted
Power
t t
RF Amplifier Rectifier
(+ Antenna = Rectenna)
Transmitting
AntennaRF Choke
(DC Bias)
RF Choke
(DC Bias) DC
Block
VDD-VG
R0
Imp
ed
an
ce
Ma
tch
ing
Circ
uit (N
o
Lo
ss)
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
FET,
HEMT,
etc.
Imp
ed
an
ce
Ma
tch
ing
Circ
uit
an
d L
ow
Pa
ss
Filte
r
RL
DC
Block
Receiving
Antenna
Electromagnetic
ally
Uncoupled
Source
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
Diode
User
DC
I V I V I V I V I V I V
Wireless Power Transfer via Radio Waves
23
Field of Radio Waves
24
2
2
2
2
Dd
Dd
d
I : Reactive Near Field
II : Radiative Near Field (Fresnel Region)
III : Far Field (Fraunhofer Region)
[Antenna Element] [Aperture Antenna]
Electric Field from Aperture Antenna
in Near Field and Far Field
II : Radiative Near Field (Fresnel Region)
= Sphere Wave (Beam-type WPT)
III : Far Field (Fraunhofer Region)
= Plane Wave (approximation) (Ubiquitous WPT)
I : Reactive Near Field = Inductive WPT
25
Theoretical Beam Efficiency in Far Field (Plane Wave)
24 d
PP t
r
Simple Surface
Area of Sphere
Sourcet
rtr P
d
AGP
24
Friis Transmission
Equation
)(
02
)(
01
kztjkztj
x eEeEE
In far field (at long distance),
radio wave can be assumed as plane wave.
2224 d
AA
d
AG
P
P rtrt
t
r
Beam
Efficiency
Field of Radio Waves
26
2
2
2
2
Dd
Dd
d
I : Reactive Near Field
II : Radiative Near Field (Fresnel Region)
III : Far Field (Fraunhofer Region)
[Antenna Element] [Aperture Antenna]
Electric Field from Aperture Antenna
in Near Field and Far Field
II : Radiative Near Field (Fresnel Region)
= Sphere Wave (Beam-type WPT)
III : Far Field (Fraunhofer Region)
= Plane Wave (approximation) (Ubiquitous WPT)
I : Reactive Near Field = Inductive WPT
Measured Data in Near Field
27
mmD
mmD
421472
1224.0,3
2
@ Yamasaki,
Japan, 1996
28
Formula of Efficiency of WPT via Radiowavesfor Beam-type WPT (in Radiative Near Field)
t parameter
0 0.5 1 1.5 2 2.5 30
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Tau
Eta
t
rrt
P
P
d
AA
e
22
2
2
1
t
t
t parameter and beam collection efficiency
•W. C. Brown, The history of power transmission by radio waves, IEEE Trans.
Microwave Theory and Techniques, MTT-32, pp.1230-1242, 1984.
t
Rt Rr
D
Antenna
ApertureRectenna
Aperture
‘
–3 –2 –1 0 1 2 30
2
4
–1 0 10
1
Radius
Electric Field on Tx Ant. Electric Field in Far Field.
Radius
Fraunhofer’s Diffraction (|r0|, |r| <<d)
00 rrr dvyuxd
kf
d
k
d
kdg
jexp )(
2
jexp
)exp(j)(
d:distance, At,r : effective area of Tx, Rx antenna
2t
Friis'
Formula
Near distance or
Higher frequencyFar distance or
Lower Frequency
d
29
Theoretical 100% Receiving Efficiency at Infinite Array
伊藤他, “磁流アンテナを用いたレクテナの受電効率”, 信学技報AP84-69, pp.9-14, 1984
xJxJxB
xJxJxB
akx
GZ
akD
dxBxBZ
akG
DG
GA
LL
A
m
p
rad
pmrad
d
rade
yx
e
20
20
0
0
2
0
2
0
222
0
2
0
2
sin
sincos4
4
cos
Gd : operating conductance of array with antenna
position in previous page
Grad : radiation conductance of one element
D : antenna gain of one element
Grad, D is only TM110 mode by Derneryd
A : equivalent radius of CMSA
V0 : suplly voltage
K0 : propagation constant in free space
[Theory of microstrip antenna (magnetic current antenna)]
Receiving Efficiency η
HFSS Simulation ResultC
ell n
um
ber
of
z ax
is
Cell number of y axis
𝐻x [A/m]
Cel
l nu
mb
er o
f z
axis
Cell number of y axis
Receiving Efficiency: 99.9%
Magnetic field distribution Reflected magnetic field distribution
(After 15 cycles of Plane Wave input)
ReflectorAntenna ReflectorAntenna
Yu Tsukamoto, et al. “Study on a Dipole Array Antenna with Reflector for Non-Leak MPT System to Vehicles”, Proc. of 2015 Asian Wireless Power Transfer Workshop, 14.pdf 30
RF Harvesting ScenariosTokyo, Atlanta and London
R. Vias, H. Nishimoto, M. Tentzeris, Y. Kawahara, T. Asami, “A Battery-Less, Energy Harvesting Device for Long Range Scavenging of Wireless Power from Terrestrial TV Broadcasts,” IEEE 2012 IMS Digest, Montreal, June 2012.
31
M. Pinuela, P. Mitcheson, S.
Lucyszyn, “Ambient RF Energy
Harvesting in Urban
and Semi-Urban Environments,”
IEEE T-MTT, July 2013.
Energy Harvesting from TV Tower Signal by Univ. of Tokyo and Georgia Inst. of Tech.
32
Battery-Free Cellphone (Univ. of Washington)
33V. Talla, et al., “Ba‚ttery-Free Cellphone”, Proc. of the ACM on Interactive, Mobile, Wearable and
Ubiquitous Technologies, Vol. 1, No. 2, Article 25. Publication date: June 2017.
Wireless-Powered ZigBee in Same Frequency Band
34
ON ONON
OFF OFF
ZigBee
Rectenna
Mic
row
ave P
ow
er
Zig
Be
e C
om
mu
nic
atio
n
Mic
row
ave P
ow
er
Zig
Be
e C
om
mu
nic
atio
n
Mic
row
ave P
ow
er
Zig
Be
e C
om
mu
nic
atio
n
Time
• We propose MPT-ZigBee system at
same frequency of MPT and ZigBee (at
2.45GHz) with scheduling algorism.
• We can increase a limit power without
any interference (5pW/cm2 (CW)
-> 1.91mW/cm2 (pulse, no scheduling)
- > 2.61mW/cm2 (pulse, scheduling)
Intermitted
(Pulse) MPTDevice Type
As join in network
As not join in network
End device 9.46 mW 61.8 mW
Ichihara, T, et al., “Study and Development of an Intermittent Microwave Power Transmission System for a ZigBee
Device”, Proc. of 2014 IEEE Wireless Power Transfer Conference (WPTc2014), 2014, pp.40-43
Wireless Power Transfer to IoT Sensors in Hospital
(Project of ‘Center of Innovation’ supported by JST)
35
Transmitter
(927MHz, 5W)
Receivers(Sensors)
Sensing Data
Present : 920MHz-band, <1W, >5m distance
Future in ‘special Region’
: 920MHz-band, <5W, >10m distance
by Kyoto University
with Panasonic co.
in 2015
Field Experiment of Battery-less Sensor with Organic IC (Kyoto Univ., Panasonic, and Yamagata Univ.)
36at Special Permitted WPT City (Area) in South of Kyoto (2017.12)
Commercial Products of WPT via Radio Waves
• Venture Companies of Wireless Charger of Smart Phone* ‘Cota’ by Ossia inc. (WiFi-Band) http://www.ossiainc.com/
* ‘Wattup’ by Energous corp. (2.45GHz and 5.8GHz Band)
http://www.energous.com/
• Japanese Company (Dengyo)of Battery-less Sensor
(900MHz-Band) http://www.den-gyo.com/solution/solution10_b.html
UHF Band Transmitter
(920 MHz Band)
Re
ctifyin
gC
ircuit
Tran
s-M
itter
Sensor &Micro Computer
A few m
Wireless Power
DataTransmission315 MHz Band
Wireless Sensor
37
KDDI (One of Big 3 mobile
phone company
in Japan) supports them.
Delegate of US of ITU
AirFuel Group
‘Uncoupled WPT’
Based on FCC-15
t t
RF Amplifier Rectifier
(+ Antenna = Rectenna)
Transmitting
AntennaRF Choke
(DC Bias)
RF Choke
(DC Bias) DC
Block
VDD-VG
R0
Imp
ed
an
ce
Ma
tch
ing
Circ
uit (N
o
Lo
ss)
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
FET,
HEMT,
etc.
Imp
ed
an
ce
Ma
tch
ing
Circ
uit
an
d L
ow
Pa
ss
Filte
r
RL
DC
Block
Receiving
Antenna
Electromagnetic
ally
Uncoupled
Source
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
Diode
User
DC
I V I V I V I V I V I V
Wireless Power Transfer via Radio Waves
38
39
Rectenna – Rectifying Antenna –Radio Wave -> DC Power Converter
Brown&JPL Rectenna
(2.45GHz) 1970-75
Rectenna by Hokkaido Univ.
(2.45GHz) 1984
Rectenna byTexas A&M Univ.
(35GHz) 1992
Rectenna
byDENSO co.
(21GHz) 1997 Commercial Rectenna by DENGYO co. (2.45GHz) 2011
Rectenna
by Kyoto Univ.
(5.8GHz) 2001
Rectenna by Intel co.
(674 - 680 MHz) 2009
antenna
diode
antenna
diodeantenna
diode(backside)
antenna
diode
Radio Wave
DCTo Load
Imp
ed
an
ce
Ma
tch
ing
Circ
uit
an
d L
ow
Pa
ss
Filte
r
RL
DC
Block
Impedance M
atc
hin
g
Circ
uit
or H
igher H
arm
onic
s
Resonato
rs
Diode
User
Receivable Wireless Power
Receivable Wireless Power [W]
= Power Density @ Receiver [W/m2]
which depends on Transmitter and Distance
x Antenna Aperture [m2]
which is related with antenna gain and Directivity
x Antenna Efficiency [%]
x Rectifier Efficiency [%]
(x Time Factor)
40
41
Rectifier1. Half Wave (Theoretically 50%)2. Full Wave (Theoretically 100%)3. Bridge (Theoretically 100%)4. Single Shunt (Theoretically 100%)5. Double Voltage6. Charge Pump etc.
C
λ /4 line
Diode
“Theoretically 100%”
is most important
for WPT and harvesting.
Like Class-F Amplifier
Frequency Characteristics of Efficiency of Rectenna
42
2.45GHz 5.8GHz 14GHz 24GHz 35GHz
100%
50%
0%
10GHz
60%
70%
80%
90%
40%
30%
20%
10%
100GHz45GHz 62GHz 72GHz
Frequency
RF-
DC
Co
nve
rsio
n E
ffic
ien
cy
: Diode : CMOS
antenna
diode
by Brown&JPL
(2.45GHz) 1970-75
by Texas A&M Univ.
(35GHz) 1992
Products by DENGYO co. (2.45GHz) 2011
by DENSO co.
(14GHz) 2000
MMIC by Kyoto Univ.
(24GHz) 2012
by École Polytechnique
Montréal (94GHz) 2015
antenna
diode
by Tel-Aviv University
(75-110GHz) 2014
532um x 910um
by Tsukuba Univ.
(94GHz) 2016
Input Poweror Connected Load
T.- W. Yoo and K. Chang, “Theoretical and Experimental Development of 10 and 35 GHz Rectennas”, IEEE Trans. MTT, Vol.40, No.6, 1992, pp.1259- 1266
Higher Order
Harmonics Effect
RF-DC conversion efficiency of rectifier
43
RF-DC conversion
efficiency
100%
V
I
VJ
(0.2-0.3V)
Vbr
(10-30V)
-VJ
Rdiode
“rectenna”region“detector”
region
VJ Effect
Vbr EffectDiode Maximum
Efficiency Curve
Maximum Eff. is
>90% at 2.45GHz
> 80% at 5.8GHz
How to increase efficiency of rectenna
• Choose theoretically 100% circuit
• Reduce number of diodes which include loss factor
– Recommend single shunt rectifier
• Choose diode with Low RC diode
• Match impedance at input and output
• Design circuit with higher harmonics combination (like class-F amplifier)
– Suppress higher harmonics re-radiation
• To add high voltage (almost breakdown)
• (Additionally) consider combination of antenna
44
Input Poweror Connected Load
T.- W. Yoo and K. Chang, “Theoretical and Experimental Development of 10 and 35 GHz Rectennas”, IEEE Trans. MTT, Vol.40, No.6, 1992, pp.1259- 1266
Higher Order
Harmonics Effect
RF-DC conversion efficiency of rectifier
45
RF-DC conversion
efficiency
100%
VJ Effect
Vbr EffectDiode Maximum
Efficiency Curve
Maximum Eff. is
>90% at 2.45GHz
> 80% at 5.8GHz
Low Power Rectenna – How to add high voltage at diode
• Charge Pump -> High Voltage but Low Efficiency
• Input Matching Network [e.g. Active] (MIT, US, 2015)
• Output Filter Matching (Kyoto Univ. etc., Japan)
- 50% @ 1mW, 5.8GHz (2004)
• Standing Wave by Reflection
(Okayama Univ., Japan, 2004)
• Rectifying Circuit with Resonator
(Tohoku Univ. (2006), Toyama Univ. (2013), Japan)
- 40% @ 100mW, 900MHz
• High Impedance Circuit and Antenna
(Kanazawa Inst. Tech. (2016), Japan)
- 40% @ 100mW, 900MHz
• Self-Biased Rectifier (Univ. of Cantabria, Spain, 2015)46
RISH, Kyoto Univ. 47
Toward New Radio Wave Regulation of WPT
47
ITU ActivitiesITU : International Telecommunication Union (Founded in 1865)
which cites the following purposes for the union: • to maintain and extend international cooperation between all members
of the union for the improvement and rational use of telecommunications of all kinds;
• to promote and to offer technical assistance to developing countries in the field of telecommunications;
• to promote the development of technical facilities and their efficient operation;
• to promote the extension of the benefits of the new telecommunication technologies to all the world's inhabitants;
• to harmonize the actions of members in the attainment of these ends; • to promote, at the international level, the adoption of a broader
approach to telecommunications issues, an approach that includes other world and regional organizations and nongovernmental organizations concerned with telecommunications.
48
Question Report Recommendation Regulation
Discussion Result is published as
Question ITU-R 210-3/1 (1997)Wireless power transmission
decides that the following information be gathered
1 What applications have been developed for use of WPTtechnologies?
2 What are the technical characteristics of the emission employed in or incidental to applications using WPT technologies?
3 What is the WPT’s standardization situation in the world?
decides that the following Questions should be studied
1 Under what category of spectrum use should administrations consider WPT: ISM, or other?
2 What radio frequency bands are most suitable for WPT?
3 What steps are required to ensure that radiocommunicationservices, including the radio astronomy service, are protected from WPT operations?
49
Discussion of WPT in ITU on June, 2016• Two Documents are submitted to ITU from Japan
– PROPOSED REVISION OF THE WORKING DOCUMENT TOWARDS A PRELIMINARY DRAFT NEW REPORT ITU-R SM.[WPT.BEAM]
-> Toward Draft New Report – WORK PLAN FOR WIRELESS POWER TRANSMISSION
VIA RADIO FREQUENCY BEAM-> For Discussion of Each Applications
• Following frequency bands are listed– 915MHz band (on ISM band except in region 2)– 2.45GHz-band (on ISM band)– 5.8GHz band (on ISM band)
50
Done!!!
“New Report” is published
from ITU Now!http://www.itu.int/pub/R-REP-SM.2392
Question Report Recommendation Regulation
Discussion of WPT in ITU on Nov., 2016
Meeting: ITU-R RG-WPT/WP1A/WP1BThere was no SG1 meeting and no formal approval of Report or Recommendation
Date: Nov. 22nd (Tue.), – Nov.20th (Wed.) , at ITU headquarter in GenevaResults:1) Discussion of role of WP1A and WP1B2) Toward Recommendation of 6.78MHz-band WPT・There was new proposal from Bosch about the other frequency for other WPT system. But it
was rejected because there was no impact study to the other wireless systems which must be.・There was document with concern about effect of 2nd harmonics from broadcasting company
and from radio astronomy
3) Discussion of EV-WPT・Drafting of revised ITU-R Report SM.2303-1 by new organization of DG-NON.BEAM under
WP1A was done.・Opinions of coexistence power level to AM radio both from WP6A/EBU and from Japan will be
on the above revised report to show there is the different approaches
4) Discussion of Beam WPT・DG-BEAM under WP1A revised work plan toward new report [WPT-BEAM.IMPACT] based on
documents from USA and Japan.
5) Proposal of new report “Frequency management method of WPT”・Toward WRC-19, frequency management method of WPT, e.g. spectrum category of EV-WPT
will be done. 6) Other topics : Safety Issue
• Discussion of safety issue of WPT, whether it is ITU matter of not. ICNIRP, IEEE, and the other safety standards are referred in WPT documents.
51
Work Plan for Wireless Power Transmission via Radio Frequency Beam
in ITU (International Telecommunication Union) (Revised on Nov., 2016)
52
Characteristics of beam WPT applications
Type
ID Applications Frequency band
Condition Distance Power Impact study
Remarks
a
a1Wireless PoweredSensor Network
915 MHz band,2.45 GHz band,5.8 GHz band
Indoor, outdoor Several meters –dozens of meters
< 50W Must
a2Wireless Charger ofMobile Devices
2.45 GHz band Indoor Several meters –dozens of meters
< 50W Must
b
b1Wireless PowerTransfer Sheet
2.45 GHz band In mesh-patternshielded sheet
Several meters(in sheet)
< 30W [N/A] ARIBSTD-T113
b2 MPT in Pipe 2.45 GHz band,5.8 GHz band
In shielded pipe 1 m – 100 m (inpipe)
< 50W N/A
b3Microwave Buildings 2.45 GHz band,
5.8 GHz bandIn shielded pipe 1 m – 100 m (in
pipe)50W –5kW
N/A
c
c1WPT to MovingFlying Target
2.45 GHz band,5.8 GHz band
Outdoor 10 m – 20 km 50W-1MW
Must
c2Point-to-Point WPT 2.45 GHz band,
5.8 GHz bandOutdoor 1 m – 20 km 100W –
1MWMust
c3Wireless Charging forElectric Vehicle
2.45 GHz band,5.8 GHz band
Outdoor 0.1-10 m 100W-100kW
Must
c4 Solar Power Satellite TBD Space to ground 36,000 km 1.3GW Must
Edited by USA, Japan, and Israel (based on Japanese Document)
Target Year of Each Application of Beam.WPT toward New Report [WPT-BEAM.IMPACT]
53
Target years of making reports ID Applications
[2017-2020] a1 Wireless Powered Sensor Network
[2017-2020] a2 Wireless Charger of Mobile Devices
[2017 – 2020
(Short Distance)]
[2020- 2030
(Long Distance)]
c2 Point-to-Point WPT
[2025-2030] c1 WPT to Moving Flying Target
[2025-2030] c3 Wireless Charging for Electric Vehicle
TBD c4 Solar Power Satellite
RISH, Kyoto Univ. 54
Introduction of Activities of WPT
in IEEE and IEICE
54
IEEE Wireless Power Transfer Conference (WPTc)
1st IMWS-IWPT (2011)2nd IMWS-IWPT (2012)at Kyoto, Japan
1st WPTC (2013)at Perugia, Italy
2nd WPTC (2014)at Jeju, Korea
55
4th WPTC (2016)at Aveiro, Portugal
5th WPTC (2017)at Taipei, Taiwan
6th WPTW (2018)at Montreal, Canada
3rd WPTC (2015)at Boulder, USA
History of IEEE WPTc (IMWS-IWPT)
• 2011@Japan paper 59/ 69 (88%) from 8 countries,
142 attendees (pre), 176 (total)
• 2012@Japan paper 60/ 68 (88%) from 7 countries,
117 attendees (pre), 146 (total)
• 2013@Italy paper 62/ 77 (80%)
90 attendees (pre)
• 2014@Korea paper 73/103 (71%) from 19 countries,
187 attendees (pre), 203 (total)
• 2015@USA paper 93/166 (53%) from 29 countries,
164 attendees (pre), 199 (total)
• 2016@Portugal paper 97/147 (66%) from 31 countries,
146 attendees (total)
• 2017@Taiwan paper 106/132 (81%) from 20 countries
169 attendees (pre) 56
IEEE Wireless Power Transfer Conference (WPTc2018)
Montreal, Canada, June 3-7, 2018
www.wptc-ieee.org
57
Important Dates:
Submission Deadline: February 18, 2018
Notification of Acceptance: March 12, 2018
Final Paper Submission: April 30, 2018
Conference Dates: June 3-7, 2018Accepted papers will appear in the WPTC-2018 conference proceedings and will
be submitted for publication in IEEE Xplore.
Contacts: WPTC organizing committee
Asian Wireless Power Transfer Workshop by IEICE
2015 @ Taipei, Taiwan
Paper 31
Attendees app.50
2016 @ Chengdu, China
Paper 44
Attendees app.100
2017 @ Singapore
Paper 60
Attendees app.70
58
2018 in Tokoku University, Sendai, Japan
3rd Asian Wireless Power Transfer Workshop (AWPT)
Dec. 9-11, 2017
@ National University of Singapore, Singapore
59
RISH, Kyoto Univ. 60
Conclusion
60
SPS
Buildings
Vehicles
Smart Energy
Communications –Power Coexistence
Energy Security
Infrastructure of Communications –Power Coexistence
Power Storage
Ubiquitous Power Source
Saving Energy
Our Dream : Wireless Power Society
Ubiquitous Power Source in Emergency
61
WPT Books
Wireless Power Transfer via Radiowaves (Wave Series)
by Naoki ShinoharaISTE Publishing &
John Wiley & Sons, Inc., UK & USA, 2014.1
ISBN 978-1-84821-605-1
Wireless Charging Technology and the Future of
Electric Transportationed. In-Soo Suh
(Chapter Writing)SAE Books, 2015.6
ISBN 978-0-7680-8153-4
Wireless Power Transfer Algorithms, Technologies
and Applications in Ad Hoc Communication Networks
ed. Sotiris Nikoletseas, Yuanyuan Yang, and Apostolos Georgiadis,
(Chapter Writing), Springer, 2016.7, ISBN 978-3-319-46810-5
+ 2 WPT books edited by Shinohara will be published next year (River Publisher, IET Books) 62