2026-08-22
When one MOSFET can't handle the current, engineers reach for the obvious solution: put two (or four, or eight) in parallel. Unlike BJTs, MOSFETs have a positive temperature coefficient of RDS(on) — as a device heats up, its channel resistance rises, forcing current to divert to cooler siblings. This is often described as "self-balancing," and it's used to justify skipping ballast resistors entirely. That's only half the story.
The self-balancing behavior only applies in the fully-enhanced (ohmic) region, where RDS(on) dominates. During switching transitions, MOSFETs briefly operate in saturation, where drain current is set by VGS − VGS(th). Here the temperature coefficient of VGS(th) is negative — a hotter device turns on harder, hogging more current, heating faster, and running away thermally. The result: one FET switches almost all the current for tens of nanoseconds every cycle, while its siblings loaf.
Three failure modes you'll actually see:
Practical mitigations:
Real-world example: A 48 V, 100 A synchronous buck converter uses four IPP083N10N5 MOSFETs (100 V, 8.3 mΩ) in parallel for the low-side switch. Without individual 10 Ω gate resistors, ring frequencies around 40–80 MHz between the four gates caused one FET to see 3 V of overshoot on VGS — degrading its threshold over thousands of hours until it started hogging current and eventually failed short.
Rule of thumb: Switching loss per device scales with the ratio of its own VGS(th) to the group minimum. A 200 mV threshold spread in a hard-switched application means the low-threshold FET dissipates roughly 1.5–2× the switching energy of its siblings. Static RDS(on) sharing may look balanced on a DMM — the failures happen during the nanoseconds you can't measure.
