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LT1510CS8 Datasheet(PDF) 9 Page - Linear Technology |
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LT1510CS8 Datasheet(HTML) 9 Page - Linear Technology |
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9 / 16 page ![]() 9 LT1510/LT1510-5 APPLICATIONS INFORMATION capacity ceramic capacitor (5 µF to 10µF) from Tokin or United Chemi-Con/MARCON, et al., and the old standby, aluminum electrolytic, which will require more microfarads to achieve adequate ripple rating. OS-CON can also be used. The output capacitor COUT is also assumed to absorb output switching current ripple. The general formula for capacitor current is: I V V V Lf RMS BAT BAT CC = () − ()( ) 029 1 1 . For example, with VCC = 16V, VBAT = 8.4V, L1 = 30µH and f = 200kHz, IRMS = 0.2A. EMI considerations usually make it desirable to minimize ripple current in the battery leads, and beads or inductors may be added to increase battery impedance at the 200kHz switching frequency. Switching ripple current splits be- tween the battery and the output capacitor depending on the ESR of the output capacitor and the battery impedance. If the ESR of COUT is 0.2Ω and the battery impedance is raised to 4 Ωwithabeadofinductor,only5%ofthecurrent ripple will flow in the battery. Soft Start The LT1510 is soft started by the 0.1 µF capacitor on VC pin. On start-up, VC pin voltage will rise quickly to 0.5V, then ramp at a rate set by the internal 45 µA pull-up current and the external capacitor. Battery charging current starts ramping up when VC voltage reaches 0.7V and full current is achieved with VC at 1.1V. With a 0.1µF capacitor, time to reach full charge current is about 3ms and it is assumed that input voltage to the charger will reach full value in less than 3ms. Capacitance can be increased up to 0.47 µF if longer input start-up times are needed. In any switching regulator, conventional timer-based soft starting can be defeated if the input voltage rises much slower than the time-out period. This happens because the switching regulators in the battery charger and the com- puter power supply are typically supplying a fixed amount of power to the load. If input voltage comes up slowly compared to the soft start time, the regulators will try to deliver full power to the load when the input voltage is still well below its final value. If the adapter is current limited, it cannot deliver full power at reduced output voltages and the possibility exists for a quasi “latch” state where the adapter output stays in a current limited state at reduced output voltage. For instance, if maximum charger plus computer load power is 20W, a 24V adapter might be current limited at 1A. If adapter voltage is less than (20W/1A = 20V) when full power is drawn, the adapter voltage will be sucked down by the constant 20W load until it reaches a lower stable state where the switching regulators can no longer supply full load. This situation can be prevented by utilizing undevoltage lockout, set higher than the minimum adapter voltage where full power can be achieved. A fixed undervoltage lockout of 7V is built into the VCC pin. Internal lockout is performed by clamping the VC pin low. The VC pin is released from its clamped state when the VCC pin rises above 7V. The charger will start delivering current about 2ms after VC is released, as set by the 0.1µF at VC pin. Higher lockout voltage can be implemented with a Zener diode (see Figure 3 circuit). Figure 3. Undervoltage Lockout GND VCC VC VIN 1510 F03 LT1510 2k D1 1N4001 VZ The lockout voltage will be VIN = VZ + 1V. For example, for a 24V adapter to start charging at 22VIN, choose VZ = 21V. When VIN is less than 22V, D1 keeps VC low and charger off. Charging Current Programming The basic formula for charging current is (see Block Diagram): II V R BAT PROG PROG = ()( )= () 2000 2 465 2000 . |
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