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LTC1733 데이터시트(PDF) 12 Page - Linear Technology |
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LTC1733 데이터시트(HTML) 12 Page - Linear Technology |
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12 / 16 page ![]() LTC1733 12 sn1733 1733fs If a thermistor with a tolerance less than ±10%isused, the trip point errors begin to depend on errors other than thermistor tolerance including the input offset voltage of the internal comparators of the LTC1733 and the effects of internal voltage drops due to high charging currents. Constant-Current/Constant-Voltage/ Constant-Temperature The LTC1733 uses a unique architecture to charge a battery in a constant-current, constant-voltage, constant- temperature fashion. Figure 1 shows a simplified block diagram of the LTC1733. Three of the amplifier feedback loops shown control the constant-current, CA, constant- voltage, VA, and constant-temperature, TA modes. A fourth amplifier feedback loop, MA, is used to increase the output impedance of the current source pair, M1 and M2 (note that M1 is the internal P-channel power MOSFET). It ensures that the drain current of M1 is exactly 1000 times greater than the drain current of M2. Amplifiers CA, TA, and VA are used in three separate feedback loops to force the charger into constant-current, temperature, or voltage mode, respectively. Diodes, D1, D2, and D3 provide priority to whichever loop is trying to reduce the charging current the most. The outputs of the other two amplifiers saturate low which effectively re- moves their loops from the system. When in constant- current mode, CA servos the voltage at the PROG pin to be precisely 1.50V (or 0.15V when in trickle-charge mode). TA limits the die temperature to approximately 105 °C when in constant-temperature mode and the PROG pin voltage gives an indication of the charge current as dis- cussed in “Programming Charge Current” . VA servos its inverting input to precisely 2.485V when in constant- voltage mode and the internal resistor divider made up of R1 and R2 ensures that the battery voltage is maintained at either 4.1V or 4.2V. Again, the PROG pin voltage gives an indication of the charge current. In typical operation, the charge cycle begins in constant- current mode with the current delivered to the battery equal to 1500V/RPROG. If the power dissipation of the LTC1733 results in the junction temperature approaching 105 °C, the amplifier (TA) will begin decreasing the charge current to limit the die temperature to approximately 105 °C. As the battery voltage rises, the LTC1733 either returns to constant-current mode or it enters constant- voltage mode straight from constant-temperature mode. Regardless of mode, the voltage at the PROG pin is proportional to the current being delivered to the battery. Power Dissipation The conditions that cause the LTC1733 to reduce charge current due to the thermal protection feedback can be approximated by considering the power dissipated in the IC. For high charge currents, the LTC1733 power dissipa- tion is approximately: PD = (VCC – VBAT) • IBAT where PD is the power dissipated, VCC is the input supply voltage, VBAT is the battery voltage, and IBAT is the battery charge current. It is not necessary to perform any worst- case power dissipation scenarios because the LTC1733 will automatically reduce the charge current to maintain the die temperature at approximately 105 °C. However, the approximate ambient temperature at which the thermal feedback begins to protect the IC is: TA = 105°C – PDθJA TA = 105°C – (VCC – VBAT) • IBAT • θJA Example: Consider an LTC1733 operating from a 5V wall adapter providing 1.2A to a 3.75V Li-Ion battery. The ambient temperature above which the LTC1733 will begin to reduce the 1.2A charge current is approximately: TA = 105°C – (5V – 3.75V) • 1.2A • 40°C/W TA = 105°C – 1.5W • 40°C/W = 105°C – 60°C = 45°C The LTC1733 can be used above 45 °C, but the charge current will be reduced below 1.2A. The approximate charge current at a given ambient temperature can be approximated by: I CT VV BAT A CC BAT JA = ° 105 – (– )• θ Consider the above example with an ambient temperature of 55 °C. The charge current will be reduced to approxi- mately: APPLICATIO S I FOR ATIO |
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