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LTC4095 датащи(PDF) 13 Page - Linear Technology |
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LTC4095 датащи(HTML) 13 Page - Linear Technology |
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13 / 16 page ![]() LTC4095 13 4095fa APPLICATIONS INFORMATION Figure 6. USB Soft Connect Circuit charge currents, the LTC4095 power dissipation is approximately: PD = (IN – BAT) • IBAT where PD is the power dissipated, IN is the input supply voltage, BAT is the battery voltage and IBAT is the charge current. It is not necessary to perform any worst-case power dissipation scenarios because the LTC4095 will automatically reduce the charge current to maintain the die temperature at approximately 115°C. However, the approximate ambient temperature at which the thermal feedback begins to protect the IC is: TA = 115°C – PDθJA TA = 115°C – (IN – BAT) • IBAT • θJA Example: Consider an LTC4095 operating from a USB port providing 500mA to a 3.5V Li-Ion battery. The ambient temperature above which the LTC4095 will begin to reduce the 500mA charge current is approximately: TA = 115°C – (5V – 3.5V) • (500mA) • 60°C/W TA = 115°C – 0.75W • 60°C/W = 115°C – 45°C TA = 70°C The LTC4095 can be used above 70°C, but the charge cur- rent will be reduced from 500mA. The approximate current at a given ambient temperature can be calculated: I CT IN BAT BAT A JA = ° () 115 – –• θ Using the previous example with an ambient temperature of 88°C, the charge current will be reduced to approximately: I CC VV C W C CA BAT = °° () ° = ° ° = 115 88 53 5 60 27 90 – –. • / / 3 300mA Furthermore, the voltage at the PROG pin will change proportionally with the charge current as discussed in the Programming Charge Current section. It is important to remember that LTC4095 applications do not need to be designed for worst-case thermal conditions since the IC will automatically reduce power dissipation when the junction temperature reaches approximately 115°C. USB Inrush Limiting When a USB cable is plugged into a portable product, the inductance of the cable and the high-Q ceramic input capacitor form an L-C resonant circuit. If there is not much impedance in the cable, it is possible for the voltage at the input of the product to reach as high as twice the USB voltage (~10V) before it settles out. In fact, due to the high voltage coefficient of many ceramic capacitors (a nonlinearity), the voltage may even exceed twice the USB voltage. To prevent excessive voltage from damaging the LTC4095 during a hot insertion, the soft connect circuit in Figure 6 can be employed. In this circuit, capacitor C2 holds MN1 off when the cable is first connected. Eventually C2 begins to charge up to the USB input voltage applying increasing gate support to MN1. The long time constant of R1 and C1 prevent the current from building up in the cable too fast thus dampening out any resonant overshoot. LTC4095 USB CABLE IN GND C1 10 µF C2 100nF 4095 F06 MN1 Si2302 R1 40k 8 2 5V USB INPUT Battery Charger Stability Considerations The LTC4095’s battery charger contains both a constant- voltage and a constant-current control loop. The constant- voltage loop is stable without any compensation when a battery is connected with low impedance leads. Excessive lead length, however, may add enough series inductance to require a bypass capacitor of at least 1µF from BAT to GND. Furthermore, a 4.7µF capacitor in series with a 0.2Ω to 1Ω resistor from BAT to GND is required to keep ripple voltage low when the battery is disconnected. High value, low ESR multilayer ceramic chip capacitors reduce the constant-voltage loop phase margin, possibly resulting in instability. Ceramic capacitors up to 22µF may be used in parallel with a battery, but larger ceramics should be decoupled with 0.2Ω to 1Ω of series resistance. |
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