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LTC4100 Datasheet(PDF) 25 Page - Linear Technology |
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LTC4100 Datasheet(HTML) 25 Page - Linear Technology |
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25 / 30 page ![]() LTC4100 25 4100fb APPLICATIONS INFORMATION Soft-Start and Undervoltage Lockout The LTC4100 is soft-started by the 0.12μF capacitor on the ITH pin. On start-up, ITH pin voltage will rise quickly to 0.5V, then ramp up at a rate set by the internal 30μA pull-up current and the external capacitor. Battery charging current starts ramping up when ITH voltage reaches 0.8V and full current is achieved with ITH at 2V. With a 0.12μF capacitor, time to reach full charge current is about 2ms and it is assumed that input voltage to the charger will reach full value in less than 2ms. The capacitor can be increased up to 1μF 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 computer 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 30W, a 15V adapter might be current limited at 2.5A. If adapter voltage is less than (30W/2.5A = 12V) when full power is drawn, the adapter voltage will be pulled down by the constant 30W 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 the DCDIV resistor divider, set higher than the minimum adapter voltage where full power can be achieved. Input and Output Capacitors We recommend the use of high capacity low ESR/ESL X5R type ceramic capacitors. Alternative capacitors include OSCON or POSCAP type capacitors. Aluminum electrolytic capacitors are not recommended for poor ESR and ESL reasons. Solid tantalum low ESR capacitors are acceptable, but caution must be used when tantalum capacitors are used for input or output bypass. High input surge currents can be created when the power adapter is hot-plugged into the charger or when a battery is connected to the charger. Use only “surge robust” low ESR tantalums. Re- gardless of which type of capacitor you use, after voltage selection, the most important thing to meet is the ripple current requirements followed by the capacitance value. By the time you solve the ripple current requirements, the minimum capacitance value is often met by default. The following equation shows the minimum COUT (±20% tolerance) capacitance values for stability when used with the compensation shown in the typical application on the back page. COUT(MIN) = 200/L1 The use of aluminum electrolytic for C1, located at the AC adapter input terminal, is helpful in reducing ringing during the hot-plug event. Refer to Application Note 88 for more information. In the 4A lithium battery charger (typical application on back page), the input capacitor (C2) 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. C2 is recommended to be equal to or greater than C4 (output capacitor) in capacitance value. The output capacitor (C4) is also assumed to absorb output switching current ripple. The general formula for capacitor current is: I V V V Lf RMS BAT BAT DCIN = ( ) ⎛ ⎝⎜ ⎞ ⎠⎟ 029 1 1 .• – • For example, VDCIN = 19V, VBAT = 12.6V, L1 = 10μH, and f = 300kHz, IRMS = 0.41A. EMI considerations usually make it desirable to minimize ripple current in the battery leads, and beads or induc- tors may be added to increase battery impedance at the 300kHz switching frequency. Switching ripple current splits between 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 0.2Ω and the battery impedance is raised to 4Ω with a bead or inductor, only 5% of the current ripple will flow in the battery. |
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