WIRELESS POWER - Minimizes Interconnection Problems

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  • 8/12/2019 WIRELESS POWER - Minimizes Interconnection Problems

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    DESIGNfeature

    10 Power Electronics Technology| July2011 www.powerelectronics.com

    U

    se of wireless power involves themagnetic coupling of conductorsconfigured so that the change in

    current flow through one conduc-tor transfers a voltage in anotherconductor through electromagnet-

    ic induction. The amount of inductive couplingbetween two conductors is determined by theirmutual inductance.

    You can enhance wireless power transmis-sion with the application of resonance effects.This technique employs transmitter and receiverinductors tuned to a mutual frequency. This

    enables power to be transmitted over a distanceof up 1/4 or 1/3 times the size of the primarycoil. Transmitting and receiving coils are usuallysingle layer solenoids or flat spirals with seriescapacitors, which, in combination, allow thereceiving element to be tuned to the transmitterfrequency.

    Electromagnetic induction is a function of thefrequency and the intensity of the conductorscurrent and voltage that produces the fields. The

    higher the frequency, the greater the inductioneffect. Energy transfers from the conductor

    WIRELESS POWER ALLOWS THE

    TRANSMISSION OF ELECTRICAL

    ENERGY FROM A POWER SOURCETO AN ELECTRICAL LOAD WITH-

    OUT INTERCONNECTING WIRES.

    THIS PROCESS IS USEFUL WHERE

    INTERCONNECTING WIRES ARE

    INCONVENIENT, HAZARDOUS, OR

    IMPOSSIBLE.

    SAM DAVIS,Editor-In-Chief, PET

    WIRELESSPOWERMinimizes

    InterconnectionProblems

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    Fig. 1. Wireless transmitter uses a single layer winding array structure.

    that produces the fields (the primary) to any conductor

    on which the fields impinge (the secondary). You canincrease the coupling between two conductors by wind-

    ing them into coils and placing them close together on

    a common axis, so the magnetic field of one coil passes

    through the other coil. Coupling must be tight to achieve

    high efficiency. If the distance from the primary to the

    secondary increases some of the magnetic field will miss

    the secondary, lowering the coupling.

    Common uses of resonance-enhanced electrodynamic

    induction are charging the batteries of laptop computers

    and cell phones, medical implants and electric vehicles.

    A localized charging technique selects the appropriate

    transmitting coil in a multilayer winding array structure.Fig. 1shows a typical wireless transmitter. Resonance is

    used in both the wireless charging pad (the transmitter

    circuit) and the receiver module (embedded in the load)

    to maximize energy transfer efficiency. This approach hasbeen adopted as part of the Qi (pronounced chee) wire-

    less charging standard developed by the Wireless Power

    Consortium.

    LINK EFFICIENCY

    The effectiveness of the electrodynamic induction is called

    link efficiency, dlink

    . It is a measure of the primary and

    secondary coils ability, to transfer energy from one coil to

    the other:

    (1)

    Where:

    k = Magnetic coupling factor

    (2)

    = Unloaded quality factor of the primary circuit

    (3)

    = Unloaded quality factor of the secondary circuit

    RE= REopt

    opt

    kQ

    1 10 100 1 x 103

    1.2

    1.1

    1

    0.9

    0.8

    0.7

    0.6

    0.5

    0.4

    0.3

    0.2

    0.1

    Fig. 3 Magnetic flux lines from primary and secondary coils where z = 6 mm

    (vertical distance between coils) and k = magnetic coupling factor.

    Without ferromagnetic shielding

    r= 1 (relative permeability)

    k = 0.45

    With ferromagnetic shielding

    r= 3000 (relative permeability)

    k = 0.68

    Fig. 2. Optimum link efficiency as a function of the figure of merit for the coils.

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    (4)

    = QE= Effective Q

    Where:

    RE= Effective load resistance which models the rectifier

    including the output filter capacitor and the actual load

    resistance RL. The relationship between REand RLis

    (5)

    If series resonance is used on the secondary side

    t= Primary angular velocity (2f)

    t2 =Secondary angular velocity (2f2)

    L1= Primary inductance in Henriesr1= Primary dc resistance in Ohms

    L2= Secondary inductance in Henries

    r2=Secondary dc resistance in Ohms

    The loaded quality factor is:

    (6)

    For maximum efficiency:

    Tune the link to the secondary resonant frequency

    Set the effective load resistance to:

    (7)

    To maximize kQ (figure of merit):

    Q is called the system quality factor. It should be noted

    that a low magnetic coupling can be compensated by an

    increased system quality factor.

    WIRELESS POWERtransmission

    Quality factor (D47x1)

    Q

    350

    300

    250

    200

    150

    100

    50

    0

    Frequency (kHz)0 100 200 300 400

    Q

    350

    300

    250

    200

    150

    100

    50

    0

    Frequency (kHz)0 100 200 300 400

    Q

    350

    300

    250

    200

    150

    100

    50

    0

    Frequency (kHz)0 100 200 300 400

    D47 x 1-24

    Quality factor (P40x5) Quality factor (P52x6.75)

    P40 x 5-65P40 x 5-10P40 x 5-15

    P52 x 6.75-10P52 x 6.75-20P52 x 6.75-28

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    WIRELESS POWERtransmission

    ('# #!$"&'#"

    +"!+ (&'

    +&'! "'"

    %'+ %( +#(% &" +

    ( ##'$%"'

    *

    *

    ! !

    #(' ' '&' '#" '# & $#)% "

    ! " ! # ! ! $ "

    ! ! $ "& # #!

    # %! ! $ !""& !# ! " $ !!

    ! ! "#

    Fig. 2 plots the optimum link

    efficiency as a function of the figure

    of merit for the coils, which is doptvs. kQ.

    One way to manage a high k value

    is to use a ferromagnetic shield (core)

    enhances the magnetic coupling fac-

    tor and reduces the stray magnetic

    field. Fig. 3 shows the magnetic

    field resulting from a ferromagnetic

    shield with and without ferromag-netic shielding.

    Another way to manage a high

    efficiency inductive solution is maxi-

    mize the Q or Quality factor for the

    inductive coils. Table 1 lists typical

    wireless power core from RRC and

    Fig. 4 are plots of Q vs. Frequency

    for these cores.

    Generally, for any type of coil

    type the magnetic coupling factor, k,

    can be improved by reducing the ver-

    tical distance between the coils andaligning the coils vertically as shown

    in Fig. 5a, lateral misalignment (Fig.5b) and angular misalignment (Fig.

    5c) degrade efficiency.

    EVALUATION BOARD

    To help designers evaluate the feasi-

    bility of developing a wireless power

    transmission system, RRC Power

    Solutions Inc. has introduced a wire-

    less power evaluation kit to allow

    OEMs to become familiar with the

    inductive coupling technology. The

    kit (Fig. 6) consists of a 5W (5V,1A)

    Qi compatible wireless power trans-

    mitter and receiver in a self-contained

    testing module. Users can remove

    the board and coil from the module

    housing and embed them into a

    design for hands-on device evalua-

    tion. RRC will provide detailed

    instructions on embedding the kit

    into a device at www.rrc-ps.com.

    Therefore, optimum efficiency =

    (8)

    Fig. 6. Evaluation kit

    consists of a 5W (5V,1A)

    Qi-compatible wireless

    power transmitter and

    receiver in a self-con-

    tained testing module.

    http://cui.com/powerhttp://www.powerelectronics.com/http://www.rrc-ps.com/