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Examining Wireless Power Transfer
John Rice
Agenda
3-2 Texas Instruments – 2014/15 Power Supply Design Seminar
• Introduction 5 min. – Foundational principles of electromagnetics – Power transfer - near and far field
• Existing and Emerging Wireless Power Standards 5 min. – WPC, PMA, A4WP comparison – Electromagnetic field safety implications of WPT
• Theory of Operation 20 min. – Considering loosely coupled coils – Modeling resonant power transfer – Magnetic link efficiency – Topological analysis with SPICE and FEA
• Design Considerations 20 min. – RX to TX communication – Intelligent voltage positioning and load response – EMI, efficiency/loss measurement – Foreign object detection – eddy loss detection – Single coil, 5 W WPC design example
Notable Dates in Wireless Power Transfer
3-3 Texas Instruments – 2014/15 Power Supply Design Seminar
• 1820: Biot–Savart / André-Marie Ampère / H. Oersted discover and quantify relationship between electric current and magnetic fields
• 1831: Michael Faraday / H. Hertz discover electromagnetic induction
• 1834: Lenz (Lenz‘s law) à N. Callan invents the electrical transformer
• 1864: James Clerk Maxwell synthesizes previous observations and mathematically models electromagnetic radiation
• 1891-1917: Nicola Tesla – enormous contribution to the practical application of resonant power transfer and electromagnetic induction; numerous discoveries and patents
• 2007: WiTricity research group, led by Professor Marin Soljacic advances magnetic
resonance to wirelessly power a 60 W light bulb with 40% efficiency at 2 m using 60 cm-diameter coils
• 2008/9: A consortium of companies called the Wireless Power Consortium (WPC) announces the evolution of a industry standard for low-power (5 W) inductive charging
0.1 1 10
Wave Impedance104
1x103
100
10
Near Field
Magnetic Field Electric Field
Far Field
Wireless EnergyTransfer
ElectromagenticRadiation
ElectromagneticInduction
ElectrodynamicInduction
ElectrostaticInduction
Microwave/RFPower
Light/LaserPower
MagneticInduction
Magnetic ResonantInduction
ZDC ZLC
Electromagnetic Wave Propagation
Texas Instruments – 2014/15 Power Supply Design Seminar 3-4
E ∝1/r3, H ∝1/r2 E ∝1/r, H ∝1/r
E ∝1/r2, H ∝1/r3
ZO = 377 Ω, Plane Wave
rc ⋅β
• Field defined by antenna and distance from source
• Dipole(red) and loop(blue) antennas shown
• Wave impedance = E/H, converges at λ >>1
• Reactive near field below λ/2π is non-radiative
Alliance for Wireless Power
3-5 Texas Instruments – 2014/15 Power Supply Design Seminar
Race for a Wireless Charging Standard Safety, Performance, Reliability and Interoperability
Protocols Power Frequency Band
Communication Frequency Band
Range of Coupling
Wireless Power Consortium (WPC) 105-205 kHz Same as power
transfer band 0.4 to 0.7
Powermat (PMA) 277-357 kHz Same as power transfer band 0.6 to 0.8
Alliance for Wireless Power (A4WP) 6.78 MHz 2.4GHz ISM
(ZigBee or BLE) 0.1 to 0.5
BatteryMagnetic Shield
AC MagneticFlux
RX CoilRX Coil
TX CoilTX Coil
Magnetic (Ferrite) Shield
DCAlignment
Magnet
3-6
Safety Considerations Electromagnetic Radiation Effect
Texas Instruments – 2014/15 Power Supply Design Seminar
Frequency Range
E-field (V/m)
H-field (A/m)
B-field (µT)
0.025-‐0.8 kHz 250/f 4/f 5000/f
0.15-‐1 MHz 87 0.73/f 0.92/f 1-‐10 MHz 87/f^0.5 0.73/f 0.92/f
3-7 Texas Instruments – 2014/15 Power Supply Design Seminar
Theory of Operation
E • dA =Q∑
ε0
∫
B• dA = 0∫E • dl = −
ddt
B• dAS∫∫
B• dl = µ0Ienc∫ + µ
0ε0
dϕE
dt
µ0= Vacuum _ permeability
ε0= Vacuum _ permittivity
D2
D1
RX
TX
Z
3-8 Texas Instruments – 2014/15 Power Supply Design Seminar
Loosely Coupled Coils Self and Mutual Inductance
V1(t) = R
1i1(t) + L
1
di1(t)
dt+ / −M
di2(t)
dt
V2(t) = R
2i2(t) + L
2
di2(t)
dt+ / −M
di1(t)
dt
Ρ =φ
Ni=µA
l,φ = ΡNi
Vc= N
dφ
dt= N
d(ΡNi)
dt= N2
µA
l
di
dt= L
di
dt
L =Nφ
i,φ1= φ
11+ φ
21
V2= N
2N1Ρ21
di1
dt→ M = N
2N1Ρ21
Physical representaion of flux coupling Electrical representation of flux coupling
V2 (t)V1 (t)i1 (t)
N2N1
21
11R1 I1(t) R2
V2L1 L2
M, k
V1
I2(t)
TXRX
IoutVP
IPRL
RLVS
Ideal Transformer k = 1
Cantilever Transformer Model
Leakage Impedance Cancelation
Non-Ideal Transformer k<<1
Load Reflected to Primary is Propotional to k2
IS
N
N2N1
IP IS
R1k LSLP RL
N:1
LIkg LIkgLm RL’ LmC2
C3C1
RL’
3-9 Texas Instruments – 2014/15 Power Supply Design Seminar
Power Transfer, Wired and Wireless
Wired/ Tightly Coupled
Loosely Coupled WPT
Load Reflected to Primary
RL' = N2 •RL = RL • k2 •LPLS
N = k •LPLS
Pout =VP
2
RL•NSNP
⎡
⎣⎢⎢
⎤
⎦⎥⎥
2
Llkg = (1− k2 )•LP
Lm = k2 •LP
VPVS
=ISIP
=NPNSPout =
V2
RL
T
Frequency (Hz)
89.51k 102.17k 116.63k
Ga
in (
dB
)
10.00
20.00
30.00
40.00
Series Resonant Tank
Parallel Resonant Tank
RL
RL
3-10 Texas Instruments – 2014/15 Power Supply Design Seminar
Considering Resonance
3dB
fr = 1/ 2π LCQ =
frΔf3dB
fr
Δf3dB
XC = 1ωC
XC = 1ωC
I = VZeqp
I = VZeqs
XL = ωL Rω
XL = ωL Rω
3-11 Texas Instruments – 2014/15 Power Supply Design Seminar
Coil Skin and Proximity Losses (Eddy Induced Losses)
Rpac =ωLpQp Rsac =
ωLsQs
R' = k2 i
LpLs
Rs+RL( )
IeIeL-IDEAL
RAC
RDC
RL
H-Field
Current Flow
TX
RX
VS
VS
RP
LP LS
R’
k<<1
Non-Ideal TX/RX Inductor Skin Effect Proximity Effect
3-12 Texas Instruments – 2014/15 Power Supply Design Seminar
Typical WPC TX/RX Coil Q and Skin/Proximity Effect
RX: 40 x 30 mm with shield Litz wire, 2 strands 14 turns, 1 layer Q = 2.3 @ 130 kHz Rac = 515 mΩ @ 130 kHz
TX: 43 mm diameter with shield Litz wire, 105 strand 20 turns, 2 layers Q = 100 @ 130 kHz Rac = 176 mΩ
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0
50
100
150
200
100K 150K 200K 250K 300K
TR1/Ohm
TR2/Q
f/Hz
TR1: Real(Impedance) RX : Real(Impedance)TR2: Q(Impedance) RX : Q(Impedance)
3-13 Texas Instruments – 2014/15 Power Supply Design Seminar
Primary Current vs. Frequency and Coupling Coefficient
ZIN f,k( ) = RP +R k( ) i QP f,k( )2
1+QP f,k( )2+ j(XLS f,k( )− XCr f( ) +R k( ) i QP(f,k)
1+QP(f,k)2 )
ir(f, k) =VfundamentalZIN(f, k)
2)()()( knRLRSkR +=
VIN
Cr Rp
Cr Rp
RS CS
RS
R
CS
C
RL
RL
Io
Iot
L2Ir
Ir
L1
LS
Lp
Cr Rp
Ir
LS
Lp
n 1
VIN
IDEAL
6
4
2
0
0 5x104 1x10
5 1.5x10
5 2x10
5
Frequency (Hz)
Re
so
na
nt
Cu
rre
nt
(A)
k = 0.3
k = 0.4
k = 0.5
k = 0.6
3-14 Texas Instruments – 2014/15 Power Supply Design Seminar
Coupling Efficiency
Coupling Efficiency in Relationship to Coil Separation (z) and the Ratio of Coil Diameters
Coil Vertical Displacement z/(D), Normalized
Mag
netic
Effi
cien
cy Coil Separation, Normalized
Rat
io o
f Coi
l Dia
met
ers
Q=100
0.01 0.1 1 100.0001
0.001
0.01
0.1
1Drx = DtxDrx = 0.3 DtxDrx = 0.1 DtxDrx = 0.03 DtxDrx = 0.01 Dtx
Magnetic Figure of Merit F(k,Q)
3-15 Texas Instruments – 2014/15 Power Supply Design Seminar
• Q = geometric mean of coil quality factors =
• Q influenced strongly by skin
and proximity effect
• High Q compensates for poor coupling
• High Q requires greater control bandwidth
Qp ×Qs
30 mm Planar Coils
λ k,Q( ) : = 2
k × Q( )2 × 1+ 1+ (k × Q)2⎡
⎣⎤⎦
0 0.2 0.4 0.6 0.8 1
Qsys=100Qsys=50Qsys=30Qsys=10
Coupling Coefficient, kEf
ficie
ncy
0 10 20 30 400
0.2
0.4
0.6
0.8
1
0
0.2
0.4
0.6
0.8
1k(2 mm)k(2.5 mm)k(5 mm)k(10 mm)
Center Displacement
Cou
plin
g, k
Vert
ical
Sep
arat
ion
Coil Displacement
Coupling Coefficient and Mutual Inductance from Transfer Gain
3-16 Texas Instruments – 2014/15 Power Supply Design Seminar
k =Lrx
Ltx•Vtx
Vrx=Gain
Lrx
Ltx
Ltx = 25 µH
k(gap = 0 mm) =0.516
LrxLtx
= 0.83, M = 13.6µ
k(gap = 8 mm) =0.208
LrxLtx
= 0.321, M = 5.27µ
Lrx = 10.8 µH M = k • Lrx • Ltx
Typical 5 W coils Connected to a VNA
zgap = 8 mm
zgap = 0 mmf = 125 kHz, Gain = 0.516
f = 125 kHz, Gain = 0.208
1
0.10.20.30.40.50.60.70.8
1.0x105 1.5x105 2.0x105
TR1
f/HzTR1: Mag(Gain) Memory 1 : Mag(Gain)
Intelligent WPT Digital Power, Resonant Battery Charger
3-17 Texas Instruments – 2014/15 Power Supply Design Seminar
• A transmitter (TX) driving a resonant coupled inductor
• A receiver (RX) with rectification, load modulation and post regulation
• A load, commonly a single cell, secondary battery pack
Resonant Circuit Analysis
3-18 Texas Instruments – 2014/15 Power Supply Design Seminar
• VG1 is a variable frequency AC signal in frequency domain
• VG1 is a 50% duty cycle, 19 V square wave in the time domain
• Power regulated by changing the frequency or voltage
20 × Log
VOUT
VIN
⎛⎝⎜
⎞⎠⎟= 20 × Log
7.65
19( )dB = − 7.902 dB
Resr_RX 641m Cr_RX 183n+
VG1
Cr 100n Resr_TX 452mVAC
LTX 25 µ LRX 10.8 µ
K = 0.8K
-
+Vcoil_TX
RLOAD 5
COUT 4.7 µ
VOUT 1
T
Frequency (Hz) 70.00 k 167.33 k 400.00 k
Gai
n (d
B)
-24.23
-2.48
19.26
a
Time (s) 300.00 µ 320.00 µ 340.00 µ
VOUT 4.60
4.80
VAC
5.25
VG10.00
19.00
Vcoil_TX -19.43
19.45
VAC[3]: k= 800 m, Q=34.7
f=170kHz, Gain = -7.9 dB
VAC[1]: k = 200 m
Examining Circuit Behavior in SPICE
3-19 Texas Instruments – 2014/15 Power Supply Design Seminar
Time (s)1.70m 1.71m 1.72m 1.73m 1.74m 1.75m 1.76m 1.77m
VOUT
4.00
6.00
Iprim-1.93
1.93
VSW-1.00
30.00
Vcoil_rx-20.00
20.00
Vcoil_tx-30.00
30.00
Vcoil_rx, RMS = 8.25V
Vcoil_tx, RMS = 18.7V
Isec, RMS = 1.2A
-+
-
+-
+
-
+
VgVset
U1
-
+ VCOSqr
GND
VDD
FM PHASEBoot
HGATE
GND LGATE
TPS28225 Rboot 1
Cboot 100n
T2
T1
C110 µ
C3100 µ
L8
R8
VSW K K = 0.55
L7
C62.2 m
OUTLISN
IN
M1
R650
M2
RACp
425 m
RACs
641 mIprimVcTX VcRX
CRx100 n
CRx220 n
LTX
25.4
µ
LRX
10.8
µ
VIN 19
VM1
RL 5VOUT
ISECCOUT4.7 µ
2-D FEA Plot of Magnetic Flux Between TX/RX Coils
3-20 Texas Instruments – 2014/15 Power Supply Design Seminar
• Receiver side shielding is important
• Poorly designed shields expose battery and external circuits to magnetic field
• AC/DC winding losses of TX/RX coils correspond with empirical results = 0.32 W
Ferrite Shield (TX)
Litz Coil (RX)
Ferrite Shield (RX) Aluminum (Battery or Internals)
Litz Coil (TX)
Axisymmetric FEA Evaluated in FEMM
Control
Linear
Controller
Voltage
Regulation / OV
Protection
Control and
Modulation
Synchronous
Rectifier
Receiver
DC/
DC
Driv
er
Control &
Demodulation
+
-
100%
90%
80%
70%
60%
50%
40%
30%
20%
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
Eff
icie
nc
y (
%)
Tx Eff. Magnetics Eff. Rx Eff. System Efficiency
Output Power (W)
3-21 Texas Instruments – 2014/15 Power Supply Design Seminar
Quantifying Losses – Typical 5 W Wireless Power Transmitter/Receiver
η =POUT
POUT + PRX + PTX
PTX = PTXcoil + PBridge + Pcontrol + PDC−DC PRX = PRXcoil+ Prectifier+ PIdo + Pcomm
3-22 Texas Instruments – 2014/15 Power Supply Design Seminar
Design Considerations, WPC
• Feedback communication
• Loop response
• Foreign object detection
• Electromagnetic compatibility
• System efficiency
3-23 Texas Instruments – 2014/15 Power Supply Design Seminar
WPC 1.1 Compliant 5 W TX Reference Design
GND
PGND
GND
10.0kR19
10.0kR22
10.0kR23
J_CLK
J_DATA
DATA
CLK
GND
Vcc
PMBUS
JTAG
12345678910
J2
0.1µFC10
F
L1
0.1µFC18
0.1µF
0.1µF
C15
GND
76.8kR13
10.0kR14
0.1µFC3
GND
0.02
R18
1.00kR12
GND
PGND
0.1µFC12
10.0kR17
t°NTC1
GND
123456789101112131415 16 17 18 19 20 21 22 2 3 24 25 26 27
DRV
_EN
PWM
_CTR
L
AV
SS
AV
CC
PWM
1/CL
K_O
UT
PWM
2/U
P_D
N
I_SE
NSE
PEA
K_D
ET
V_S
ENSE
FOD
_GA
IN
LED
_GRN
LED
_RED
T_SE
NSE
MO
DE
BUZZ
N/C
JTA
G_C
LK
JTA
G_D
ATA
UA
RT/C
LK_I
N
COM
M1
COM
M2
SDA
SCL
V_C
ORE
DV
SS
DV
CC
LED
FOD
_TH
R28
U1
0.1µFC6
GND
DA
TA
CLK LED
FOD_THR
J_CL
K
J_D
ATA
1000pFC21
GND
C16
0.1µFC17
GNDGND GND
1
2
3
4
5
6789
1011
USB
J1
GNDGND
TANK
TANK
GNDGNDGND
FOD_THR LED
1.00kR3
1.00kR4
Place close to U2
GND
0.1µFC9
GNDPGND
PGND
10.0kR5
10.0kR6
10.0kR7
10.0kR8
10.0kR9
10.0kR10
10.0kR25
69.8kR24
523kR21
0.01µF
C20 1000pFC23
2700pFC22
GreenD2
RedD3
PWM1/CLK_IN1
PWM_CTRL2
EN3
BP34
AGND5
AGND6
DMOUT27
DMOUT18
CLK
_OU
T9
MO
DE
10
DM
IN1
11
DM
IN2
12
AG
ND
13
PVIN
214
PVIN
215
BOO
T216
SW2 17SW2 18SW2 19
PGND 20PGND 21PGND 22
SW1 23SW1 24
BOO
T125
SW1
26PV
IN1
27PV
IN1
28CS
-29
CS+
30CS
O31
PWM
2/U
P_D
N32
PWRP
AD
33
U2
Vcc
TP8
TP7
PGND
499R20
499R1
GND
TP9
TP11
TP2
TP3
TP14
TP15
TP4
TP5
0.47µFC8
TP12
TP10
0R15
0R16
TP6
0.01µFC7
10.0kR11
GND
TP13
523kR2
2700pFC1
TP1
D5D-1N4148WS
D1D-1N4148WS
GND
1 23 45 67 89 10
11 1213 14
J3
22µFC11
22µF
C13
22µFC24
PGND
0.01µFC19
0.01µFC14
2.2µFC5
0.47µFC4
22µFC2
PinkD4
NT1
Net-Tie
GND PGND
3-24 Texas Instruments – 2014/15 Power Supply Design Seminar
Qi Power Transfer Communication Protocol
• TX generates a shared magnetic field - TX coil creates magnetic field - Magnetic field induces current in RX coil
• Communication in power field
- TX waits until its field perturbed by RX
- TX sends seek energy “ping”
- TX waits for a digital response
- If digital response is valid, transfer power
• Power transferred at level needed
- RX reports power received/needed
- TX adjusts power based on RX feedback
- If feedback is lost, power transfer stops
Apply Power
Co
nta
ct
Es
tab
lish
ed
Ex
ten
de
d
Dig
ital P
ing
Ping
Identification and
Configuration
Power Transfer
No Response
Abort Digital Ping
Power Transfer (PT)
Complete
PT Contact Violation
Unexpected Packet
Time-out
Power Transfer
Complete
Reconfigure
Selection
No PT Contact
Unexpected Packet
Transmission Error
Time-Out
From WPC Qi System Description. Part 1
Control
Linear
Controller
Voltage
Regulation / OV
Protection
Control and
Modulation
Synchronous
Rectifier
Rectifier
Voltage Battery/ChargerResonant
Transmitter
Resonant
ReceiverDriv
er
Control &
Demodulation
+
-
3-25 Texas Instruments – 2014/15 Power Supply Design Seminar
WPC RX Load Modulation
Integrated Transmitter IC Integrated Receiver IC
3-26 Texas Instruments – 2014/15 Power Supply Design Seminar
Measurement
• Power transfer waveforms - Coil resonance - Harmonic content
• Load response
• Efficiency –
- Loss contributors - PCB coil vs. Litz
• RX/TX communication
• EMI, FOD
• Spatial freedom VNA – Bode 100 – Coil gain/impedance characteristics MDO4104 – Mixed domain oscilloscope Differential voltage probe capable of > 40 V, current probe, IR probe
3-27 Texas Instruments – 2014/15 Power Supply Design Seminar
Reference Design Waveforms at 5 W Time and Spectrum Domain
Misaligned coils force operation closer to resonance Vpp_tx = 40 V, fSW = 135 kHz
RMS gain = 0.509
Centered coils force operation further from resonance
Vpp_tx = 20 V, fSW = 170 kHz RMS gain = 0.56
TX
TX Coil Harmonics TX Coil Harmonics
RX TX RX
3-28 Texas Instruments – 2014/15 Power Supply Design Seminar
Intelligent Voltage Positioning
Maximum data rate package during transition
240 ms
Dynamic Voltage Positioning
Load current step = 250 mA-0 A
3-29 Texas Instruments – 2014/15 Power Supply Design Seminar
Transient Load Response IOUT = 0 to 1 A
5 V TX Supply Current
12 V TX Supply Current
Voltage Response
WPC Wireless Power RX Phone “Skin”
3-30 Texas Instruments – 2014/15 Power Supply Design Seminar
Transient Load Step Response Litz TX Coil / PCB RX Coil
0 to 250 mA load step at ~ 1 A/µs
bq51013B based RX design 2.65 in x 1.35 in x 0.02 in
45 mm TX coil with shield
Eff
icie
nc
y (
%)
Output Power (W)
Litz TX Coil w/o
SEPIC Converter
Litz TX Coil w/SEPIC
Triple PCB Coil w/o SEPIC
80%
70%
60%
50%
40%
30%
20%
10%
0
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
3-31 Texas Instruments – 2014/15 Power Supply Design Seminar
System Efficiency – DC Input to DC Output PCB Coil vs. 105 Strand Litz Coil
3-32 Texas Instruments – 2014/15 Power Supply Design Seminar
Designing for Spatial Freedom Efficiency Across Charging Area
• Efficiency map at a 5 W load measured over the PCB coil area • +/- 40 mm in x-direction and 30 mm in y-direction, 5 mm steps
0.00% 0.00% 0.00% 45.23% 0.00% 0.00% 0.00% 0.00% 0.00% 0.00% 0.00% 0.00% 44.95% 46.05% 0.00% 0.00% 0.00% 15
0.00% 0.00% 48.78% 51.77% 50.32% 45.38% 46.91% 50.38% 51.84% 50.05% 45.21% 46.49% 51.92% 52.46% 48.58% 0.00% 0.00% 10
0.00% 43.71% 51.37% 53.92% 52.23% 47.34% 52.23% 55.30% 56.12% 55.44% 51.05% 49.32% 53.11% 53.84% 51.24% 44.16% 0.00% 5
0.00% 44.74% 52.23% 54.55% 52.69% 48.95% 53.64% 56.73% 57.54% 56.72% 52.95% 49.69% 53.59% 54.54% 51.75% 45.64% 0.00% 0
0.00% 43.99% 51.58% 53.85% 52.56% 47.95% 51.06% 54.79% 55.37% 55.00% 50.74% 49.44% 53.06% 53.63% 50.99% 44.34% 0.00% -5
0.00% 41.57% 49.44% 52.08% 50.50% 45.28% 46.08% 50.08% 51.84% 50.23% 44.44% 46.61% 50.05% 51.68% 48.26% 0.00% 0.00% -10
0.00% 0.00% 42.12% 44.93% 0.00% 0.00% 0.00% 0.00% 0.00% 0.00% 0.00% 0.00% 45.00% 44.81% 0.00% 0.00% 0.00% -15
-40 -35 -30 -25 -20 -15 -10 -5 0 5 10 15 20 25 30 35 40 (mm)
3-33 Texas Instruments – 2014/15 Power Supply Design Seminar
Design for Electromagnetic Compatibility
Optimized for EMC Non-Optimized Performance
GND Plane Under TX Coil TX Conductive Enclosure
WirelessReceiver
WirelessTransmitter
Common Mode Filter
Multilayer Electric Shield
3-34 Texas Instruments – 2014/15 Power Supply Design Seminar
Foreign Object Detection • Depending on specific heat capacity,
foreign object temp rise can be > 60°C
• Battery pack is especially sensitive
Where: → P = Power dissipated in FO → C = FO specific heat capacity → M = FO mass → t = time
• Metal objects between TX and RX can induce eddy current losses
• Field density of 5 W wireless chargers can result in significant eddy losses
ΔT= P× tC×m
1009080706050403020100
0.20 0.40 0.60 0.80 1.00 1.20 1.40 1.60
Tem
pera
ture
, deg
C
Power, W
AI Cu Fe Au
Temperature Rise for 1g of Material in 15s
TX 8,563
RX 5,000
04:00 04:20
04:40
05:00
10,000
8,000
6,000
4,000
2,000
0
Thr 1,900
Loss 1,316
04:00 04:20
04:40
05:00
2,000
1,500
1,000
500
0
Transmit & Receive Power (mW)
Loss vs. Threshold (mW)
3-35 Texas Instruments – 2014/15 Power Supply Design Seminar
Dynamic RX / TX Loss Accounting
45 mm FO placed adjacent to misaligned TX coil
TX & RX account for losses
Loss threshold set high
FO removed
FO placed next to TX coil, losses increase by > 1 W
FOD reaches 55 C in under 60 s
Transmit & Receive Power (mW)
Loss vs. Threashold (mW)
min:sec
min:sec
PDAn
Wired Model
Wireless Power Vision
Multi-ModeUniversal
WPT Transmitter
Charges All Compliant Devices
Intelligent WirelessPower Transfer
85% Efficient + Plus LowPower Shutdown Modes
Phone/PortableElectronic Device
~80%Full Load
Cha
rger
ICW
TPR
ecei
ver
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3-36 Texas Instruments – 2014/15 Power Supply Design Seminar
A Vision for Wireless Power Transfer
3-37 Texas Instruments – 2014/15 Power Supply Design Seminar
Summary
• Market studies project rapid growth in wireless power technology
• Wireless power transfer is useful when a wired solution is inconvenient, hazardous or impossible
• WPT standards have emerged to accelerate growth, reliability, acceptance and safety in consumer electronics
• Developing a wireless power solution does not require compliance to any standard other than those affecting consumer safety and EMC
• Standard compliance may provide advantages in marketability
(interoperability), performance, reliability and time to market • Achieving spatial freedom and good efficiency requires a deep
understanding of magnetic field theory
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