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3570 датащи(PDF) 13 Page - Linear Technology |
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3570 датащи(HTML) 13 Page - Linear Technology |
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13 / 20 page ![]() LT3570 13 3570fa into a tight local loop, minimizing EMI. The input capaci- tor must have low impedance at the switching frequency to do this effectively and it must have an adequate ripple current rating. The RMS input current is: IIN2(RMS) =IOUT2 • VOUT2 VIN2 –VOUT2 () VIN2 < IOUT2 2 and is largest when VIN2 = 2 • VOUT2 (50% duty cycle). Considering that the maximum load current is ~1.5A, RMS ripple current will always be less than 0.75A. The high frequency of the LT3570 reduces the energy storage requirements of the input capacitor, so that the capacitance required is often less than 10μF. The combi- nation of small size and low impedance (low equivalent series resistance or ESR) of ceramic capacitors makes them the preferred choice. The low ESR results in very low voltage ripple. Ceramic capacitors can handle larger magnitudes of ripple current than other capacitor types of the same value. Use X5R and X7R types. An alternative to a high value ceramic capacitor is a lower value along with a larger electrolytic capacitor, for example a 1μF ceramic capacitor in parallel with a low ESR tantalum capacitor. For the electrolytic capacitor, a value larger than 10μF will be required to meet the ESR and ripple current requirements. Because the input capacitor is likely to see high surge currents when the input source is applied, tantalum capacitors should be surge rated. The manu- facturer may also recommend operation below the rated voltage of the capacitor. Be sure to place the 1μF ceramic as close as possible to the VIN2 and GND pins on the IC for optimal noise immunity. A final caution is in order regarding the use of ceramic capacitors at the input. A ceramic input capacitor can combine with stray inductance to form a resonant tank circuit. If power is applied quickly (for example by plugging the circuit into a live power source), this tank can ring, doubling the input voltage and damaging the LT3570. The solution is to either clamp the input voltage or dampen the tank circuit by adding a lossy capacitor in parallel with the ceramic capacitor. For details, see Application Note 88. Boost Input Capacitor Selection The capacitor of a boost converter is less critical due to the fact that the input current waveform is triangular and does not contain large squarewave currents as found in the output capacitor. Capacitors in the range of 10μF to 100μF with an ESR of 0.3Ω or less work well up to the full 1.5A switch current. Higher ESR capacitors may be acceptable at low switch currents. Input capacitor ripple current for boost converters is: IRIPPLE = 0.3 • VIN1 • VOUT1 –VIN1 f•L • VOUT1 Buck Diode Selection The catch diode (D2 from Figure 1) conducts current only during switch off time. Average forward current in normal operation can be calculated from: ID(AVG) =IOUT1 • VIN1 –VOUT1 VIN1 The only reason to consider a diode with a larger current rating than necessary for nominal operation is for the worst-case condition of shorted output. The diode current will then increase to the typical peak switch current. Peak reverse voltage is equal to the regulator input voltage. Use a diode with a reverse voltage rating greater than the input voltage. Table 3 lists several Schottky diodes and their manufacturers. Table 3. Schottky Diodes PART NUMBER VR (V) IAVE (A) VF AT 1A (mV) On Semiconductor MBRM120E 20 1 530 MBRM140 40 1 550 Diodes Inc. B120 20 1 500 B130 30 1 500 International Rectifier 10BQ030 30 1 420 APPLICATIONS INFORMATION |
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