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Buck Inductor Ripple⚠ unverified

Electrical / Power Electronics · Compute the peak-to-peak inductor current ripple in a buck converter

Parameters

InputSymbolUnitDefaultDescription
VinVinV1.0Input voltage
VoutVoutV1.0Output voltage
LLH1.0Inductance
ffHz1.0Switching frequency
DD1.0Duty cycle (dimensionless). Default is None, in which case it is computed from ``buck_converter_duty(Vin, Vout)``
OutputSymbolUnitDescription
resultΔIAPeak-to-peak inductor current ripple, in amperes (A)

The science & history

Understanding the Parameters

Derivation (Approaching a Proof)

While the high-side switch is on for time $t_{on} = D/f$, the inductor sees approximately constant voltage $V_L = V_{in} - V_{out}$ (ideal switch and diode/sync-FET drops neglected). From $v = L\,di/dt$,

$$\Delta I = \frac{V_L}{L}\,t_{on} = \frac{(V_{in} - V_{out})}{L}\cdot\frac{D}{f} = \frac{(V_{in} - V_{out})\,D}{L\,f}.$$

During the off interval the current ramps down by the same $\Delta I$ (steady state: volt-second balance). The triangular ripple sits on the DC load current $I_{out}$; continuous conduction requires $I_{out} > \Delta I/2$.

Check with ideal $D$: substituting $D = V_{out}/V_{in}$ gives the common form $\Delta I = V_{out}(1-D)/(L f) = V_{out}(V_{in}-V_{out})/(V_{in} L f)$.

History

Inductor ripple sizing has been standard buck-converter design practice since early switch-mode regulators. Modern point-of-load modules still quote $\Delta I$ targets (often 20–40% of $I_{out}$) as a rule of thumb balancing size, efficiency, and transient response.

Related Concepts: Buck Converter Duty Cycle, Output Voltage Ripple, Inductor Stored Energy, Conduction Loss

Notes: Registry calculator buck-inductor-ripple (unverified). Ideal CCM; ignores DCR, switch drops, and discontinuous mode. Units: $L$ in H, $f$ in Hz → $\Delta I$ in A.

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