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LTC1759 Datasheet(PDF) 25 Page - Linear Technology |
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LTC1759 Datasheet(HTML) 25 Page - Linear Technology |
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25 / 28 page ![]() 25 LTC1759 voltage will be pulled down by the constant 30W load until it reaches a lower stable state where the switching regu- lators can no longer supply full load. This situation can be prevented by utilizing the DCDIV resistor divider, set higher than the minimum adapter voltage where full power can be achieved. Input and Output Capacitors In the 4A Lithium Battery Charger (Figure 10), the input capacitor (C14) is assumed to absorb all input switching ripple current in the converter, so it must have adequate ripple current rating. Worst-case RMS ripple current will be equal to one half of output charging current. Actual capacitance value is not critical. Solid tantalum low ESR capacitors have high ripple current rating in a relatively small surface mount package, but caution must be used when tantalum capacitors are used for input or output bypass. High input surge currents can be created when the adapter is hot-plugged to the charger or when a battery is connected to the charger. Solid tantalum capacitors have a known failure mechanism when subjected to very high turn-on surge currents. Only Kemet T495 series of “Surge Robust” low ESR tantalums are rated for high surge conditions such as battery to ground. The relatively high ESR of an aluminum electrolytic for C15, located at the AC adapter input terminal, is helpful in reducing ringing during the hot-plug event. Highest possible voltage rating on the capacitor will mini- mize problems. Consult with the manufacturer before use. Alternatives include new high capacity ceramic (at least 20 µF) from Tokin, United Chemi-Con/Marcon, et al. How- ever, using ceramic capacitors in the output filter of the charger can lead to acoustic noise radiation that can be confused with instability. At low charge currents, the charger operates in discontinuous current mode at an audible frequency. Other alternative capacitors include OSCON capacitors from Sanyo. The output capacitor (C3) is also assumed to absorb output switching current ripple. The general formula for capacitor current is: APPLICATIONS INFORMATION IRMS = (L1)(f) VBAT VCC () 0.29 (VBAT) 1 – For example, VCC = 19V, VBAT = 12.6V, L1 = 10µH, and f = 200kHz, IRMS = 0.6A. 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 imped- ance. If the ESR of C3 is 0.2 Ω and the battery impedance is raised to 4 Ω with a bead or inductor, only 5% of the current ripple will flow in the battery. Charger Crowbar Protection If VIN connector of Figure 1 charger can be instantaneously shorted (crowbarred) to ground, then a small P-channel FET M4 should be used to fast turn off the input P-channel FET M3 (see Figure 11), otherwise, high surge current might damage M3. M3 can also be replaced by a diode if dropout voltage and heat dissipation are not problems. Note that LT1759 will operate even when VBAT is grounded. If VBAT of Figure 1 charger gets shorted to ground very quickly (crowbarred) from a high battery voltage, slow loop response may allow charge current to build up and damage the topside N-channel FET M1. A small diode D5 (see Figure 12) from SDB pin to VBAT will shut down switching and protect the charger. Note that M4 and/or D5 are needed only if the charger system can be potentially crowbarred. Protecting SMBus Inputs The SMBus inputs, SCL and SDA, are exposed to uncon- trolled transient signals whenever a battery is connected to the system. If the battery contains a static charge, the SMBus inputs are subjected to ESD which can cause damage after repeated exposure. Also, if the battery’s positive terminal makes contact to the connector before the negative terminal, the SMBus inputs can be forced |
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