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MLP2012S датащи(PDF) 16 Page - Seiko Instruments Inc |
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MLP2012S датащи(HTML) 16 Page - Seiko Instruments Inc |
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16 / 50 page ![]() STEP-UP, SUPER-SMALL PACKAGE, 1.2 MHz PWM/PFM SWITCHABLE SWITCHING REGULATOR S-8363 Series Rev.2.0_01 16 1. Continuous current mode The following explains the current that flows into the inductor when the step-up operation stabilizes in a certain status and IOUT is sufficiently large. When the Nch power MOS FET is turned on, current (I1) flows in the direction shown in Figure 14. The inductor current (IL) at this time gradually increases in proportion with the ON time (tON) of the Nch power MOS FET, as shown in Figure 15. Current change of inductor within tON : ΔIL(ON) = IL max. − IL min. = VIN L × tON When the Nch power MOS FET is turned off, the voltage of the CONT pin is stepped up to VOUT + VD and the voltage on both ends of the inductor becomes VOUT + VD − VIN. However, it is assumed here that VOUT >> VD and VD is ignored. Current change of inductor within tOFF : ΔIL(OFF) = VOUT − VIN L × tOFF The input power equals the output power in an ideal situation where there is no loss by components. IIN(AV) : PIN = POUT IIN(AV) × VIN = IOUT × VOUT ∴IIN(AV) = VOUT VIN × IOUT ........................ (1) The current that flows in the inductor consists of a ripple current that changes due to variation over time and a direct current. From Figure 15 : IIN(AV) : IIN(AV) = IIN(DC) + Δ IL 2 = IIN(DC) + VOUT − VIN 2 × L × tOFF = IIN(DC) + VIN 2 × L × tON ............... (2) Above, the continuous mode is the operation mode when IIN(DC) > 0 as shown in Figure 15 and the inductor current continuously flows. While the output current (IOUT) continues to decrease, IIN(DC) reaches 0 as shown in Figure 16. This point is the critical point of the continuous mode. As shown in equations (1) and (2), the direct current component (IIN(DC)) depends on IOUT. IOUT(0) when IIN(DC) reaches 0 (critical point) : IOUT(0) = tON × VIN2 2 × L × VOUT When the output current decreases below IOUT(0), the current flowing in the inductor stops flowing in the tOFF period as shown in Figure 17. This is the discontinuous mode. |
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