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  • 參數(shù)資料
    型號(hào): LTC1773
    廠商: Linear Technology Corporation
    英文描述: Synchronous Step-Down Regulator Controller(同步步降穩(wěn)壓器)
    中文描述: 同步降壓穩(wěn)壓控制器(同步步降穩(wěn)壓器)
    文件頁(yè)數(shù): 8/20頁(yè)
    文件大?。?/td> 274K
    代理商: LTC1773
    LTC1773
    8
    inductor ripple current and consequent output voltage
    ripple. Do not allow the core to saturate!
    Molypermalloy (from Magnetics, Inc.) is a very good, low
    loss core material for toroids, but it is more expensive than
    ferrite. A reasonable compromise from the same manu-
    facturer is Kool M
    μ
    . Toroids are very space efficient,
    especially when you can use several layers of wire. Be-
    cause they generally lack a bobbin, mounting is more
    difficult. However, new designs for surface mount are
    available which do not increase the height significantly.
    Power MOSFET and Schottky Diode Selection
    Two external power MOSFETs must be selected for use
    with the LTC1773: a P-channel MOSFET for the top (main)
    switch, and an N-channel MOSFET for the bottom (syn-
    chronous) switch.
    The peak-to-peak gate drive levels are set by the V
    IN
    voltage. Therefore, for V
    IN
    > 5V, logic-level threshold
    MOSFETs should be used. But, for V
    IN
    < 5V, sub-logic
    level threshold MOSFETs (V
    GS(TH)
    < 3V) should be used.
    In these applications, make sure that the V
    IN
    to the
    LTC1773 is less than 8V because the absolute maximum
    V
    GS
    rating of the majority of these sub-logic threshold
    MOSFETs is 8V.
    Selection criteria for the power MOSFETs include the “ON”
    resistance R
    DS(ON)
    , reverse transfer capacitance C
    RSS
    ,
    input voltage, maximum output current, and total gate
    charge. When the LTC1773 is operating in continuous
    mode the duty cycles for the top and bottom MOSFETs are
    given by:
    Main Switch Duty Cycle = V
    OUT
    /V
    IN
    Synchronous Switch Duty Cycle = (V
    IN
    – V
    OUT
    )/V
    IN
    The MOSFET power dissipations at maximum output
    current are given by:
    P
    V
    V
    I
    R
    )
    K V
    I
    C
    f
    MAIN
    OUT
    IN
    MAX
    DSON
    IN
    MAX
    RSS
    =
    (
    )
    +
    (
    +
    ) (
    )(
    )( )
    2
    2
    1
    δ
    APPLICATIO
    S I
    N
    FOR
    ATIO
    U
    The operating frequency and inductor selection are inter-
    related in that higher operating frequencies allow the use
    of smaller inductor and capacitor values. However, oper-
    ating at a higher frequency generally results in lower
    efficiency because of external MOSFET gate charge losses.
    The inductor value has a direct effect on ripple current. The
    ripple current,
    I
    L
    , decreases with higher inductance or
    frequency and increases with higher V
    IN
    or V
    OUT
    .
    W
    U
    Kool M
    μ
    is a registered trademark of Magnetics, Inc.
    I
    f L
    V
    V
    V
    L
    OUT
    OUT
    IN
    =
    ( )( )
    1
    1–
    (1)
    Accepting larger values of
    I
    L
    allows the use of lower
    inductances, but results in higher output voltage ripple
    and greater core losses. A reasonable starting point for
    setting ripple current is 30% to 40% of I
    MAX
    . Remember,
    the maximum
    I
    L
    occurs at the maximum input voltage.
    The inductor value also has an effect on Burst Mode
    operation. The transition to low current operation begins
    when the inductor current peaks fall to approximately 1/3
    its original value. Lower inductor values (higher
    I
    L
    ) will
    cause this to occur at lower load currents, which can cause
    a dip in efficiency in the upper range of low current
    operation. In Burst Mode operation, lower inductance
    values will cause the burst frequency to increase.
    Inductor Core Selection
    Once the value for L is known, the type of inductor must be
    selected. High efficiency converters generally cannot af-
    ford the core loss found in low cost powdered iron cores,
    forcing the use of more expensive ferrite, molypermalloy,
    or Kool M
    μ
    cores. Actual core loss is independent of core
    size for a fixed inductor value, but it is very dependent on
    inductance selected. As inductance increases, core losses
    go down. Unfortunately, increased inductance requires
    more turns of wire and therefore copper losses will in-
    crease. Ferrite designs have very low core losses and are
    preferred at high switching frequencies, so design goals
    can concentrate on copper loss and preventing saturation.
    Ferrite core material saturates “hard”, which means that
    inductance collapses abruptly when the peak design cur-
    rent is exceeded. This results in an abrupt increase in
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