參數(shù)資料
        型號: DCP011512DBP-U
        英文描述: Miniature, 1W Isolated UNREGULATED DC/DC CONVERTERS
        中文描述: 微型1W隔離未穩(wěn)壓DC / DC轉(zhuǎn)換器
        文件頁數(shù): 12/20頁
        文件大?。?/td> 453K
        代理商: DCP011512DBP-U
        DCP01B SERIES
        SBVS012B
        DECEMBER 2000
        REVISED OCTOBER 2004
        www.ti.com
        12
        Decoupling Ceramic Capacitors
        All capacitors have losses due to their internal equivalent
        series resistance (ESR), and to a lesser degree their
        equivalent series inductance (ESL). Values for ESL are
        not always easy to obtain. However, some manufacturers
        provide
        graphs
        of
        Frequency
        Impedance. These will show the capacitors
        impedance
        falling as frequency is increased (see Figure 4). As the
        frequency is increased, the impedance will stop
        decreasing and begin to rise. The point of minimum
        impedance indicates the capacitors
        resonant frequency.
        This frequency is where the components of capacitance
        and inductance reactance are of equal magnitude. Beyond
        this point, the capacitor is not effective as a capacitor.
        versus
        Capacitor
        0
        f
        O
        Frequency
        X
        L
        Z
        Where:
        XC is the reactance due to the capacitance,
        XL is the reactance due to the ESL
        f
        O
        the resonant frequency
        Z =
        (XC
        XL)
        2
        + (ESR)
        2
        Figure 4. Capacitor Impedance vs Frequency
        At f
        O
        , X
        C
        = X
        L;
        however, there is a 180
        °
        phase difference
        resulting in cancellation of the imaginary component. The
        resulting effect is that the impedance at the resonant point
        is the real part of the complex impedance; namely, the
        value of the ESR. The resonant frequency must be well
        above the 800kHz switching frequency of the DCP and
        DCVs.
        The effect of the ESR is to cause a voltage drop within the
        capacitor. The value of this voltage drop is simply the
        product of the ESR and the transient load current, as
        shown in Equation (1):
        V
        IN
        V
        PK
        (ESR
        I
        TR
        )
        Where:
        V
        IN
        is the voltage at the device input.
        V
        PK
        is the maximum value of the voltage on the
        capacitor during charge.
        I
        TR
        is the transient load current.
        The other factor that affects the performance is the value
        of the capacitance. However, for the input and the full wave
        outputs (single-output voltage devices), the ESR is the
        dominant factor.
        Input Capacitor and the effects of ESR
        If the input decoupling capacitor is not ceramic with
        < 20m
        ESR, then at the instant the power transistors
        switch on, the voltage at the input pins will fall momentarily.
        Should the voltage fall below approximately 4V, the DCP
        will detect an under-voltage condition and switch the DCP
        drive circuits to the off state. This is carried out as a
        precaution against a genuine low input voltage condition
        that could slow down or even stop the internal circuits from
        operating correctly. This would result in the drive
        transistors being turned on too long, causing saturation of
        the transformer and destruction of the device.
        Following detection of a low input voltage condition, the
        device switches off the internal drive circuits until the input
        voltage returns to a safe value. Then the device tries to
        restart. If the input capacitor is still unable to maintain the
        input voltage, shutdown recurs. This process is repeated
        until the capacitor is charged sufficiently to start the device
        correctly. Otherwise, the device will be caught up in a loop.
        Normal startup should occur in approximately 1ms from
        power being applied to the device. If a considerably longer
        startup duration time is encountered, it is likely that either
        (or both) the input supply or the capacitors are not
        performing adequately.
        For 5V to 15V input devices, a 2.2
        μ
        F low-ESR ceramic
        capacitor will ensure a good startup performance, and for
        the remaining input voltage ranges, 0.47
        μ
        F ceramic
        capacitors are good. Tantalum capacitors are not
        recommended, since most do not have low-ESR values
        and will degrade performance. If tantalum capacitors must
        be used, close attention must be paid to both the ESR and
        voltage as derated by the vendor.
        Output Ripple Calculation Example
        DCP020505: Output voltage 5V, Output current 0.4A. At
        full output power, the load resistor is 12.5
        . Output
        capacitor of 1
        μ
        F, ESR of 0.1
        . Capacitor discharge time
        1% of 800kHz (ripple frequency):
        t
        DIS
        = 0.0125
        μ
        s
        t = C
        ×
        R
        LOAD
        t = 1
        ×
        10
        6
        ×
        12.5 = 12.5
        μ
        s
        V
        DIS
        = V
        O
        (1
        EXP(
        t
        DIS
        /
        τ
        ))
        V
        DIS
        = 5mV
        By contrast the voltage dropped due to the ESR:
        V
        ESR
        = I
        LOAD
        ×
        ESR
        V
        ESR
        = 40mV
        Ripple voltage = 45mV
        Clearly, increasing the capacitance will have a much
        smaller effect on the output ripple voltage than reducing
        the value of the ESR for the filter capacitor.
        (1)
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