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Decoupling capacitors

Decoupling capacitor guide

Digital ICs don't draw a steady current — their internal gates switch in nanoseconds, pulling short, sharp current spikes from the supply pin. The trace back to the regulator has inductance and can't react that fast, so without help the local supply voltage dips or rings every time the chip switches. A decoupling (or bypass) capacitor sits right at the pin as a tiny local charge reservoir: it supplies that fast current itself, so the regulator only has to deal with the slower average load.

The usual arrangement is two tiers. A small ceramic, almost always around 100 nF, sits directly on the IC's supply pin and handles the fast, high-frequency transients. A larger bulk capacitor, typically in the 1-10 µF range, feeds a small group of nearby ICs or a section of a power rail and restocks the charge those small caps used up, responding to slower, lower-frequency current swings.

Placement matters as much as the printed value. Every millimeter of trace or via between the capacitor and the pin adds parasitic inductance, and that inductance — not the capacitor's rated capacitance — is usually what limits how well it can respond at the frequencies decoupling is meant to fix. The rule of thumb: put it as close to the pin as the footprint allows, with the shortest possible path, ideally a dedicated via straight down, to the ground plane.

A cap's printed value is a starting point, not gospel: small ceramics lose a real chunk of their rated capacitance once DC bias and temperature are applied, so check the manufacturer's DC-bias derating curve rather than the datasheet's nominal number on a marginal design. And more capacitors isn't automatically better — stacking values that are too close together (or too far apart with nothing in between) can create a parallel resonance where the combined impedance briefly rises instead of falling; a roughly decade-spaced pair (100 nF + 1 µF, not 100 nF + 100 µF right next to it) avoids that trap.

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