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AN1330 датащи(PDF) 18 Page - STMicroelectronics |
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AN1330 датащи(HTML) 18 Page - STMicroelectronics |
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18 / 31 page ![]() Application information AN1330 18/31 Nevertheless, the ESR of the output capacitor introduces a zero in the open loop gain, which helps to increase the phase margin of the system. If the zero goes to a very high frequency, its effect is negligible. For this reason, ceramic capacitors and very low ESR capacitors in general should be avoided. Tantalum and electrolytic capacitors are usually a good choice for this purpose. Table 3 below provides a list of some tantalum capacitor manufacturers. ● Inductor The inductor value is very important because it fixes the ripple current flowing through output capacitor. The ripple current is usually fixed at 20-40% of IOmax, which is 0.2 - 0.4 A with IOmax = 1 A. The approximate inductor value is obtained using the following formula: Equation 19 where TON is the ON time of the internal switch, given by D · T. For example, with VOUT = 3.3 V, VIN = 12 V and ∆IO = 0.3 A, the inductor value is about 35 µH. The peak current through the inductor is given by: Equation 20 and it can be observed that if the inductor value decreases, the peak current (which must be lower than the current limit of the device) increases. So, when the peak current is fixed, a higher inductor value allows a higher value for the output current. In Table 4: Inductor selection, some inductor manufacturers are listed. Table 3. Output capacitor selection Manufacturer Series Cap value ( µF) Rated voltage (V) ESR (m Ω) AVX TPS 100 to 470 4 to 35 50 to 200 KEMET T494/5 100 to 470 4 to 20 30 to 200 Sanyo POSCAP (1) 1. POSCAP capacitors have characteristic very similar to tantalum capacitors. TPA/B/C 100 to 470 4 to 16 40 to 80 Sprague 595D 220 to 390 4 to 20 160 to 650 Table 4. Inductor selection Manufacturer Series Inductor value ( µH) Saturation current (A) Coilcraft DO1813HC 22 to 33 1 to 1.2 DO3316 33 to 47 1.6 to 2 L V IN V OUT – () I ∆ --------------------------------------- T ON • = I PK I O I ∆ 2 ----- + = |
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