SNVAAB4 January 2026 LM63615-Q1 , LM63625-Q1 , LM63635-Q1
In the above text, the above tests conducted through the EVM find that there is indeed a large reverse current in the current application. While the chip on EVM is not damaged, large sample sizes can significantly increase the risk of breakdown due to reverse current. This chapter details how reverse current causes instantaneous failure during the switching process of a buck converter, along with the complete failure sequence.
(1) Q1 turn-on and dead-time phase
Figure 6-1 Q1 turn-on and dead-time phaseAt power down or when the input falls below the output, the reverse current path is VOUT-> SW-> Q1 body diode-> VIN. During this phase, Cds is charged.
(2) Phase at which Q1 turns off and Q2 turns on
Figure 6-2 Phase at which Q1 turns off and Q2 turns onWhen upper transistor Q1 turns off and lower transistor Q2 turns on:
Generally, the turn-on time of the lower transistor is at ns level. Consequently, calculations indicate that even with reverse currents of merely several hundred mA, di/dt variation becomes substantial enough to reach levels capable of damaging the lower transistor MOSFET.
(3) Failure process analysis
Figure 6-3 Lower transistor failureAdditionally, some failures manifest as BOOT PIN short-circuits. This can be explained by the substantial di/dt simultaneously creating Figure 6-4 a significant potential difference across the BOOT capacitor. When this potential difference exceeds the breakdown voltage of BOOT capacitor, it forms a short-circuit loop with VCC breakdown.
Figure 6-4 BOOT failure(4) Other issues
Depending on the failure process of the reverse current, the following questions may arise:
AUTO Mode (PFM Mode): Under light load, the chip reduces switching frequency to minimize switching and conduction losses, thereby lowering power consumption.
FPWM Mode: The chip maintains a constant switching frequency set by RT throughout operation, and it is currently designed to be 2.1MHz.
The charge accumulation in Cds during Q1 conduction is determined by the charging duration. This charging time of Cds comprises Q1 conduction and dead time, with the latter being fixed. Consequently, the primary influencing factor is Q1's conduction time. Therefore, under light load conditions, the frequency is lower, resulting in a shorter discharge time for Q2 when it turns on. If the discharge time for the reverse recovery current of the Cds and diode is too short, it will generate a substantial di/dt within a short period.
In summary, when the chip operates under light load conditions, a lower switching frequency results in a longer cycle time. Ton duration becomes longer compared to lower frequencies, meaning the upper transistor remains switched on for a longer period. This prolongs the charging time of the parasitic capacitances Cds and Cboot, leading to a greater current surge when the lower transistor switches on.
The same power board in this case also utilizes 2pcs of LM63635-Q1 devices, though their outputs are set to 3.9V/3.3V, without any failure issues observed. For POC power supply applications, outputs are often set to 8V. Automotive batteries typically operate within a 9-16V range, with some requiring 6-16V. When the automotive battery voltage is inherently low, reverse current is more readily induced on the 3.3V/3.9V/5V power rails during power-down. In the current case, the camera load is relatively light. Compared to 3.9V load on the other LM63635-Q1 on the board, it is more prone to entering PFM Mode, thereby further increasing the probability of reverse current breakdown.