2026-05-05
Every time you switch off current through an inductor — a relay coil, transformer primary, brushed motor, or even a long PCB trace — the collapsing magnetic field tries to keep current flowing. With nowhere to go, it generates a voltage spike governed by V = L·di/dt. Open a switch fast enough on a 100 mH coil carrying 1 A, and you can easily see hundreds of volts ringing across your switching device. That's how MOSFETs die.
A snubber absorbs that energy and damps the resulting ringing. Three flavors you'll meet most often:
Concrete example: a 24 V relay with 200 mH coil, 50 mA holding current, switched by a small N-channel MOSFET. When the FET turns off in ~100 ns, di/dt ≈ 5×10⁵ A/s and the spike potential is L·di/dt ≈ 100 kV (clamped in practice by parasitics, but easily 200+ V). A flyback diode across the coil is the cheapest fix; add a 100 Ω + 10 nF RC across the FET drain–source to kill the residual ringing that EMI tests will otherwise flag.
Rule of thumb for RC snubbers: measure the parasitic ringing frequency fr with the snubber off. The parasitic capacitance is roughly Cp ≈ 1/((2π fr)²·L). Pick Csnub ≈ 3–10× Cp, then choose R = √(L/Csnub) for critical damping. Verify the resistor's power rating: P ≈ ½·Csnub·V²·fswitch. At 100 kHz with 10 nF and 50 V, that's already 1.25 W — don't size it casually.
Place the snubber physically close to the switching node. A snubber three centimeters away with a long ground return is barely a snubber at all — its own loop inductance defeats the purpose.
