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Gate Drive Power⚠ unverified

Electrical / Power Electronics · Compute the gate drive power dissipation

Parameters

InputSymbolUnitDefaultDescription
QgQgC1.0Total gate charge
VgsVgsV1.0Gate-to-source drive voltage
ffHz1.0Switching frequency
OutputSymbolUnitDescription
resultPWGate drive power dissipation, in watts (W)

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

To raise the gate from 0 to $V_{gs}$, the driver must supply charge $Q_g = \int i_g\,dt$. The energy delivered by a constant-voltage gate supply during that charge is

$$E_{on} = Q_g\,V_{gs}.$$

(If the gate is a linear capacitor $C_{iss}$, then $Q_g = C_{iss}V_{gs}$ and $E = C V^2$, of which $\tfrac12 C V^2$ is stored on the gate and $\tfrac12 C V^2$ is lost in the series resistance — total drawn from the supply is still $C V^2 = Q_g V_{gs}$.) Discharging the gate on the next edge typically dissipates the stored energy in the pull-down path; for a full cycle the supply still provided $Q_g V_{gs}$ once per turn-on. At frequency $f$,

$$P = E_{cycle}\,f = Q_g\,V_{gs}\,f.$$

For complementary half-bridge drivers, count both devices (or use total $Q_g$ appropriately).

History

Gate-charge specifications and the $Q_g V f$ power estimate became standard as power MOSFETs replaced bipolars (no large continuous base current, but capacitive gate charge every cycle). Driver ICs and isolated gate-drive supplies are sized around this budget plus quiescent current.

Related Concepts: Switching Loss, Conduction Loss, Efficiency Total, Watt's Law

Notes: Registry calculator gate-drive-power (unverified). $Q_g$ in coulombs (1 nC = $10^{-9}$ C). Simple model: no driver quiescent current, no overlapping cross-conduction in the driver stage.

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