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ADP1111 Datenblatt(PDF) 12 Page - Analog Devices |
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ADP1111 Datenblatt(HTML) 12 Page - Analog Devices |
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12 / 16 page ![]() ADP1111 –12– REV. 0 This occurs in the step-up mode when the following condition is met: VOUT + VDIODE VIN − VSW < 1 1 − DC where DC is the ADP1111’s duty cycle. When this relationship exists, the inductor current does not go all the way to zero during the time that the switch is OFF. When the switch turns on for the next cycle, the inductor current begins to ramp up from the residual level. If the switch ON time remains constant, the inductor current will increase to a high level (see Figure 24). This increases output ripple and can require a larger inductor and capacitor. By controlling switch current with the ILIM resistor, output ripple current can be maintained at the design values. Figure 25 illustrates the action of the ILIM circuit. Figure 24. Figure 25. The internal structure of the ILIM circuit is shown in Figure 26. Q1 is the ADP1111’s internal power switch that is paralleled by sense transistor Q2. The relative sizes of Q1 and Q2 are scaled so that IQ2 is 0.5% of IQ1. Current flows to Q2 through an internal 80 Ω resistor and through the R LIM resistor. These two resistors parallel the base-emitter junction of the oscillator- disable transistor, Q3. When the voltage across R1 and RLIM exceeds 0.6 V, Q3 turns on and terminates the output pulse. If only the 80 Ω internal resistor is used (i.e. the I LIM pin is connected directly to VIN), the maximum switch current will be 1.5 A. Figure 6 gives RLIM values for lower current-limit values. 72kHz OSC VIN POWER SWITCH SW2 SW1 RLIM DRIVER 80 Ω (INTERNAL) ILIM IQ1 200 VIN (EXTERNAL) Q2 ADP1111 Q1 Q3 R1 Figure 26. ADP1111 Current Limit Operation The delay through the current limiting circuit is approximately 1 µs. If the switch ON time is reduced to less than 3 µs, accuracy of the current trip-point is reduced. Attempting to program a switch ON time of 1 µs or less will produce spurious responses in the switch ON time; however, the ADP1111 will still provide a properly regulated output voltage. PROGRAMMING THE GAIN BLOCK The gain block of the ADP1111 can be used as a low-battery detector, error amplifier or linear post regulator. The gain block consists of an op amp with PNP inputs and an open-collector NPN output. The inverting input is internally connected to the ADP1111’s 1.25 V reference, while the noninverting input is available at the SET pin. The NPN output transistor will sink about 300 µA. Figure 27a shows the gain block configured as a low-battery monitor. Resistors R1 and R2 should be set to high values to reduce quiescent current, but not so high that bias current in the SET input causes large errors. A value of 33 k Ω for R2 is a good compromise. The value for R1 is then calculated from the formula: R1 = V LOBATT − 1.25 V 1.25 V R2 where VLOBATT is the desired low battery trip point. Since the gain block output is an open-collector NPN, a pull-up resistor should be connected to the positive logic power supply. ADP1111 1.25V REF GND AO 5V RL 47k TO PROCESSOR R1 R2 VBAT VIN SET 33k R1= ––––––––– VLB–1.25V 35.1µA VLB = BATTERY TRIP POINT Figure 27a. Setting the Low Battery Detector Trip Point 200mA/div 200mA/div |
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