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DCP01B Datasheet(PDF) 13 Page - Texas Instruments |
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DCP01B Datasheet(HTML) 13 Page - Texas Instruments |
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13 / 21 page ![]() DCP01B SERIES SBVS012C − DECEMBER 2000 − REVISED AUGUST 2005 www.ti.com 13 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 versus Capacitor 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. 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 fO, XC = XL; 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: VIN is the voltage at the device input. VPK is the maximum value of the voltage on the capacitor during charge. ITR 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 Ω 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 µF low-ESR ceramic capacitor will ensure a good startup performance, and for the remaining input voltage ranges, 0.47 µF 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 Ω. Output capacitor of 1 µF, ESR of 0.1Ω. Capacitor discharge time 1% of 800kHz (ripple frequency): tDIS = 0.0125µs t = C × RLOAD t = 1 × 10−6 × 12.5 = 12.5µs VDIS = VO(1 − EXP(−tDIS/τ)) VDIS = 5mV By contrast the voltage dropped due to the ESR: VESR = ILOAD × ESR VESR = 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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