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    型號: 74HCT9046A
    廠商: NXP Semiconductors N.V.
    英文描述: PLL with bandgap controlled VCO
    中文描述: 鎖相環(huán)控制VCO的帶隙
    文件頁數(shù): 9/40頁
    文件大?。?/td> 240K
    代理商: 74HCT9046A
    1999 Jan 11
    9
    Philips Semiconductors
    Product specification
    PLL with bandgap controlled VCO
    74HCT9046A
    The pump current I
    P
    is independent
    from the supply voltage and is set by
    the internal bandgap reference of
    2.5 V.
    R
    b
    is the external bias resistor
    between pin 15 and ground.
    The current and voltage transfer
    function of PC2 are shown in Fig.9.
    The phase comparator gain is:
    I
    2
    π
    Typical waveforms for the PC2 loop
    locked at f
    c
    are shown in Fig.10.
    When the frequencies of SIG
    IN
    and
    COMP
    IN
    are equal but the phase of
    SIG
    IN
    leads that of COMP
    IN
    , the up
    output driver at PC2
    OUT
    is held ‘ON’
    for a time corresponding to the phase
    difference (
    Φ
    PCIN
    ). When the phase of
    SIG
    IN
    lags that of COMP
    IN
    , the down
    or sink driver is held ‘ON’.
    When the frequency of SIG
    IN
    is higher
    than that of COMP
    IN
    , the source
    output driver is held ‘ON’ for most of
    the input signal cycle time and for the
    remainder of the cycle time both
    drivers are ‘OFF’ (3-state). If the
    SIG
    IN
    frequency is lower than the
    COMP
    IN
    frequency, then it is the sink
    driver that is held ‘ON’ for most of the
    cycle. Subsequently the voltage at the
    capacitor (C2) of the low-pass filter
    connected to PC2
    OUT
    varies until the
    signal and comparator inputs are
    equal in both phase and frequency. At
    this stable point the voltage on C2
    remains constant as the PC2 output is
    in 3-state and the VCO input at pin 9
    is a high impedance. Also in this
    condition the signal at the phase
    comparator pulse output (PCP
    OUT
    )
    has a minimum output pulse width
    equal to the overlap time, so can be
    used for indicating a locked condition.
    I
    P
    17
    R
    b
    2.5
    ( )
    ×
    =
    K
    p
    ------- A r
    )
    =
    Thus for PC2 no phase difference
    exists between SIG
    IN
    and COMP
    IN
    over the full frequency range of the
    VCO. Moreover, the power
    dissipation due to the low-pass filter is
    reduced because both output drivers
    are OFF for most of the signal input
    cycle. It should be noted that the PLL
    lock range for this type of phase
    comparator is equal to the capture
    range and is independent of the
    low-pass filter. With no signal present
    at SIG
    IN
    the VCO adjust, via PC2, to
    its lowest frequency.
    By using current sources as charge
    pump output on PC2, the dead zone
    or backlash time could be reduced to
    zero. Also, the pulse widening due to
    the parasitic output capacitance plays
    no role here. This enables a linear
    transfer function, even in the vicinity
    of the zero crossing. The differences
    between a voltage switch charge
    pump and a current switch charge
    pump are shown in Fig.11.
    The design of the low-pass filter is
    somewhat different when using
    current sources. The external resistor
    R3 is no longer present when using
    PC2 as phase comparator. The
    current source is set by R
    b
    . A simple
    capacitor behaves as an ideal
    integrator now, because the capacitor
    is charged by a constant current. The
    transfer function of the voltage switch
    charge pump may be used. In fact it is
    even more valid, because the transfer
    function is no longer restricted for
    small changes only. Further the
    current is independent from both the
    supply voltage and the voltage across
    the filter. For one that is familiar with
    the low-pass filter design of the
    4046A a relation may show how R
    b
    relates with a fictive series resistance,
    called R3'.
    This relation can be derived by
    assuming first that a voltage
    controlled switch PC2 of the 4046A is
    connected to the filter capacitance C2
    via this fictive R3' (see Fig.8b). Then
    during the PC2 output pulse the
    charge current equals:
    V
    V
    With the initial voltage V
    C2(0)
    at:
    1
    2
    V
    CC
    = 2.5 V,
    As shown before the charge current
    of the current switch of the 9046A is:
    R
    b
    Hence:
    Using this equivalent resistance R3'
    for the filter design the voltage can
    now be expressed as a transfer
    function of PC2; assuming ripple
    (f
    r
    = f
    i
    ) is suppressed, as:
    4
    π
    Again this illustrates the supply
    voltage independent behaviour of
    PC2.
    Examples of PC2 combined with a
    passive filter are shown in Figs 12
    and 13. Figure 12 shows that PC2
    with only a C2 filter behaves as a
    high-gain filter. For stability the
    damped version of Fig.13 with series
    resistance R4 is preferred.
    Practical design values for R
    b
    are
    between 25 and 250 k
    with
    R3' = 1.5 to 15 k
    for the filter design.
    Higher values for R3' require lower
    values for the filter capacitance which
    is very advantageous at low values
    the loop natural frequency
    ω
    n
    .
    I
    P
    -------------R3'
    =
    I
    P
    R3'
    2.5
    =
    I
    P
    17
    2.5
    ×
    =
    R3'
    R
    b
    17
    ------
    (
    )
    =
    K
    PC2
    --5
    (
    )
    =
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