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Using Commutating Diodes to Protect Inductive Loads

Diodes are widely employed to tame the high‑voltage spikes that arise when current through an inductor is abruptly interrupted—a phenomenon known as inductive kickback.

Inductive Kickback Without Protection

Consider the simple circuit shown below. When the push‑button switch closes, current flows from the battery through the coil, building a magnetic field that stores energy. If the switch is then opened, the collapsing magnetic field forces a voltage spike across the coil because the induced emf is proportional to the rate of change of magnetic flux (Faraday’s Law: e = N·dΦ/dt). This reverse‑polarity pulse can reach hundreds of volts, arcing across the switch contacts and dramatically shortening their life.

Using Commutating Diodes to Protect Inductive Loads

Inductive Kickback With a Commutating Diode

Adding a commutating diode—placed in parallel with the coil—provides a simple and effective solution. The diode is reverse‑biased while the coil is energized, so it does not conduct during normal operation. When the switch opens, the coil’s inductance generates a reverse‑polarized voltage that forward‑biases the diode, allowing the stored energy to circulate safely through the diode instead of arcing across the contacts.

Because the diode’s forward voltage drop (≈0.7 V for silicon) is much lower than the inductive spike, the switch sees only the battery voltage plus a tiny drop, greatly reducing arcing and extending component life.

Using Commutating Diodes to Protect Inductive Loads

What Is a Commutating Diode?

In electronic terminology, commutation refers to the reversal of voltage polarity or current direction. A commutating diode—sometimes called a snubber—acts whenever the voltage reverses, such as when an inductor is suddenly de‑energized. It “snubs” the high‑voltage transient by providing a low‑impedance path for the inductive current.

Drawbacks of Using a Commutating Diode

The main trade‑off is that the diode slows the coil’s demagnetization. With the voltage clamped to the diode’s forward drop, the magnetic flux decays more slowly than in an unprotected circuit. While the discharge time remains well under one second, the added delay can be critical for relays and other electromechanical devices that rely on rapid de‑energization.

Finding a Balance: Diode Plus Resistor

To achieve a compromise between limiting peak voltage and maintaining a faster decay, a resistor can be added in series with the commutating diode. This allows the induced voltage to rise above the diode’s forward drop, accelerating the magnetic field collapse while still keeping the peak voltage within acceptable limits. The resistor value must be chosen to limit the transient to a level the switch contacts can tolerate.

Using Commutating Diodes to Protect Inductive Loads

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