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LT1512CS8 Datasheet(PDF) 6 Page - Linear Technology |
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LT1512CS8 Datasheet(HTML) 6 Page - Linear Technology |
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6 / 12 page ![]() 6 LT1512 OPERATION current amplifier is set to a fixed gain of – 12.5 which provides a – 100mV current limit sense voltage. The error signal developed at the amplifier output is brought out externally and is used for frequency compen- sation. During normal regulator operation this pin sits at a voltage between 1V (low output current) and 1.9V (high output current). Switch duty cycle goes to zero if the VC pin is pulled below the VC pin threshold, placing the LT1512 in an idle mode. The LT1512 is an IC battery charger chip specifically opti- mized to use the SEPIC converter topology. The SEPIC topology has unique advantages for battery charging. It will operate with input voltages above, equal to or below the battery voltage, has no path for battery discharge when turned off and eliminates the snubber losses of flyback designs. It also has a current sense point that is ground referred and need not be connected directly to the battery. The two inductors shown are actually just two identical windings on one inductor core, although two separate inductors can be used. A current sense voltage is generated with respect to ground across R3 in Figure 1. The average current through R3 is always identical to the current delivered to the battery. The LT1512 current limit loop will servo the voltage across R3 to – 100mV when the battery voltage is below the voltage limit set by the output divider R1/R2. Constant current charging is therefore set at 100mV/R3. R4 and C4 filter the current signal to deliver a smooth feedback voltage to the IFB pin. R1 and R2 form a divider for battery voltage sensing and set the battery float voltage. The suggested value for R2 is 12.4k. R1 is calculated from: R RV RA BAT 1 2 1 245 1 245 2 0 3 = +µ (– . ) .( . ) VBAT = battery float voltage 0.3 µA = typical FB pin bias current A value of 12.4k for R2 sets divider current at 100 µA. This is a constant drain on the battery when power to the charger is off. If this drain is too high, R2 can be increased to 41.2k, reducing divider current to 30 µA. This introduces an addi- APPLICATIONS INFORMATION tional uncorrectable error to the constant voltage float mode of about ±0.5% as calculated by: V Error = 0.15 A(R1)(R2) 1.245(R1+ R2) BAT ±µ ±0.15µA = expected variation in FB bias current around the nominal 0.3 µA typical value. With R2 = 41.2k and R1 = 228k, (VBAT = 8.2V), the error due to variations in bias current would be ±0.42%. A second option is to disconnect the voltage divider with a small NMOS transistor as shown in Figure 3. To ensure adequate drive to the transistor (even when the VIN voltageis at its lowest operating point of 2.4V), the FET gate is driven wth a peak detected voltage via D2. Note that there are two connections for D2. The L1 A connection must be used if the voltage divider is set for less than 3.5V (fully charged battery). Gate drive is equal to battery voltage plus input voltage. The disadvantage of this connection is that Q1 will still be “on” if the VIN voltage is active and the charger is shut down via the S/S pin. The L1 B connection allows Q1 to turn off when VIN is off or when shutdown is initiated, but the reduced gate drive (=VBAT) is not adequate to ensure a Q1 on-state for fully charged battery voltages less than 3.5V. Do not substitute for Q1 unless the new device has adequate VGS maximum rating, especially if D2 is connected to L1A. C6 filters the gate drive and R5 pulls the gate low when switching stops. Disconnecting the divider leaves only D1 diode leakage as a battery drain. See Diode Selection for a discussion of diode leakage. |
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