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LT1769IGN Datasheet(PDF) 10 Page - Linear Technology |
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LT1769IGN Datasheet(HTML) 10 Page - Linear Technology |
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10 / 16 page ![]() 10 LT1769 APPLICATIONS INFORMATION R5 = R6(V – V ) V UV UV IN VUV = Rising lockout threshold on the UV pin VIN = Charger input voltage that will sustain full load power Example: With R6 = 5k, VUV = 6.7V and setting VIN at 12V; R5 = 5k (12V – 6.7V)/6.7V = 4k The resistor divider should be connected directly to the adapter output as shown, not to the VCC pin, to prevent battery drain with no adapter voltage. If the UV pin is not used, connect it to the adapter output (not VCC) and connect a resistor no greater than 5k to ground. Floating this pin will cause reverse battery current to increase from 3 µA to 200µA. If connecting the unused UV pin to the adapter output is not possible, it can be grounded. Although it would seem that grounding the pin creates a permanent lockout state, the UV circuitry is arranged for phase reversal with low voltages on the UV pin to allow the grounding technique to work. ally, batteries will automatically be charged at the maximum possible rate of which the adapter is capable. This is accomplished by sensing total adapter output current and adjusting the charge current downward if a preset adapter current limit is exceeded. True analog control is used, with closed-loop feedback ensuring that adapter load current remains below the limit. Amplifier CL1 in Figure 2 senses the voltage across RS4, connected between the CLP and CLN pins. When this voltage exceeds 100mV, the amplifier will override the programmed charge current to limit adapter current to 100mV/RS4. A lowpass filter formed by 500 Ω and 1µF is required to eliminate switching noise. If the input current limit is not used, both CLP and CLN pins should be connected to VCC. Charge Current Programming The basic formula for charge current is (see Block Diagram): IBAT = IPROG = 2.465V RPROG RS2 RS1 ()( ) RS2 RS1 () where RPROGisthetotalresistancefromPROGpintoground. For the sense amplifier CA1 biasing purpose, RS3 should have the same value as RS2 and SPIN should be connected directly to the sense resistor (RS1) as shown in the Block Diagram. For example, 2A charge current is needed. For low power dissipation on RS1 and enough signal to drive the amplifier CA1, let RS1 = 100mV/2A = 0.05Ω. This limits RS1 power to 0.2W. Let RPROG = 5k, then: RS2 = RS3 = = = 200 Ω (IBAT)(RPROG)(RS1) 2.465V (2A)(5k)(0.05) 2.465V Charge current can also be programmed by pulse width modulating IPROG with a switch Q1 to RPROG at a frequency higher than a few kHz (Figure 3). Charge current will be proportional to the duty cycle of the switch with full current at 100% duty cycle. 100mV 500 Ω CLP CLN VCC UV 1769 F02 R5 LT1769 R6 1 µF + RS4* VIN AC ADAPTER OUTPUT *RS4 = 100mV ADAPTER CURRENT LIMIT + – + CL1 Figure 2. Adapter Input Current Limiting Adapter Current Limiting An important feature of the LT1769 is the ability to automatically adjust charge current to a level which avoids overloading the wall adapter. This allows the product to operate at the same time the batteries are being charged without complex load management algorithms. Addition- |
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