Sep 11, 2026

a Kelvin source changes the switching tradeoff

I recently came across a paper on the tradeoff between switching losses and EMI in SiC MOSFETs, and one thing stood out to me:

A Kelvin source connection doesn't make switching “better”—it changes the switching tradeoff.

In a conventional 3-pin SiC MOSFET, part of the source inductance is shared by both:

During turn-on, the rapidly changing source current creates a voltage across this shared inductance. Since the MOSFET responds to the actual gate-to-source voltage at the die, this common-source inductance opposes the applied gate drive.

The result:

Hand-drawn diagram of a conventional 3-pin SiC MOSFET showing common-source inductance shared by the power-current and gate-driver-return paths
Conventional 3-pin package: the gate-driver return shares the power-source inductance.

The intuitive conclusion is that common-source inductance should always be minimized. A Kelvin source connection does exactly that by providing a separate, low-current source connection for the gate-driver return:

The two connections represent the same electrical node at DC, but behave very differently during a fast switching transient. By preventing most of the power-path inductance from appearing in the gate-driver loop, the Kelvin connection allows the MOSFET to switch faster and reduce switching loss.

Hand-drawn diagram of a 4-pin SiC MOSFET showing separate power-source and Kelvin-source paths
4-pin package: the Kelvin-source return bypasses the power-source inductance.

Wolfspeed gives a good example at 30 A:

But fast switching also means higher di/dt and dv/dt, which can increase overshoot, ringing, EMI, and parasitic effects if the rest of the gate-driver design isn't reconsidered.

So switching from a conventional source connection to a Kelvin source isn't simply a packaging improvement that can be done in isolation. It changes the switching dynamics and inherently changes the gate-driver design required around the device.