Table 2. Design Parameters

9.2.2.1 Selection of Input and Output Capacitors

In most applications, all that is needed is a high-frequency decoupling capacitor on the input power pin. For normal charging applications, a 0.1 μF ceramic capacitor, placed in close proximity to the IN pin and GND pad works best. In some applications, depending on the power supply characteristics and cable length, it may be necessary to increase the input filter capacitor to avoid exceeding the OVP voltage threshold during adapter hot plug events where the ringing exceeds the deglitch time.

The charger in the bq25071-Q1 requires a capacitor from OUT to GND for loop stability. Connect a 1 μF ceramic capacitor from OUT to GND close to the pins for best results. More output capacitance may be required to minimize the output drop during large load transients.

The LDO also requires an output capacitor for loop stability. Connect a 0.1 μF ceramic capacitor from LDO to GND close to the pins. For improved transient response, this capacitor may be increased.

9.2.2.2 Thermal Considerations

The bq25071-Q1 is packaged in a thermally enhanced QFN package. The package includes a thermal pad to provide an effective thermal contact between the IC and the printed circuit board (PCB). Full PCB design guidelines for this package are provided in the application note entitled: QFN/SON PCB Attachment Application Note (SLUA271).

The most common measure of package thermal performance is thermal impedance (θ_JA) measured (or modeled) from the chip junction to the air surrounding the package surface (ambient). The mathematical expression for θ_JA is:

Where:

Equation 5.

T_J = chip junction temperature
T_A = ambient temperature
P_D = device power dissipation

Factors that can greatly influence the measurement and calculation of θ_JA include:

• Whether or not the device is board mounted
• Trace size, composition, thickness, and geometry
• Orientation of the device (horizontal or vertical)
• Volume of the ambient air surrounding the device under test and airflow
• Whether other surfaces are in close proximity to the device being tested

The device power dissipation, P_D, is a function of the charge rate and the voltage drop across the internal PowerFET. It can be calculated from the following equation when a battery pack is being charged:

P_D = (V_IN – V_OUT) × I_OUT

Due to the charge profile of LiFePO₄ batteries the maximum power dissipation is typically seen at the beginning of the charge cycle when the battery voltage is at its lowest. See the charging profile, Figure 10. If the board thermal design is not adequate the programmed fast charge rate current may not be achieved under maximum input voltage and minimum battery voltage, as the thermal loop can be active, effectively reducing the charge current to avoid excessive IC junction temperature.