Boost Converter Calculator

Design a step-up (boost) DC-DC converter. Compute duty cycle, inductor ripple, output ripple, and peak currents for Vout > Vin applications.

Calculator Electronics Updated Apr 18, 2026
How to Use
  1. Enter input voltage (lower), desired output voltage (higher), and load current.
  2. Set switching frequency and inductor value.
  3. Duty cycle D = 1 − Vin/Vout tells you the fraction of each cycle the switch is closed.
  4. Peak currents are higher than for equivalent buck designs — pick parts accordingly.
Input
V
V
A
Hz (kHz, MHz OK)
H (uH, mH OK)
F (nF, uF OK)
Presets
Switching Waveform
Duty Cycle
%
Avg Input Current
A
Peak Inductor I
A
Output Ripple
mV

Show Work

Enter values to see calculations.

Formulas

Duty Cycle
D = 1 − Vin / Vout
Fraction of cycle the switch is ON.
Input Current
Iin = Iout × Vout / (η × Vin)
Higher than Iout — inversely proportional to Vin.
Inductor Ripple
ΔIL = Vin × D / (L × fsw)
Ripple on the inductor current waveform.
Peak Current
I_pk = Iin + ΔIL / 2
Max inductor current — size switch/inductor above this.
Output Ripple
ΔVout = Iout × D / (fsw × Cout)
Different formula than buck — discontinuous output current.
Minimum Inductor
L_min = Vin × D × (1−D) / (2 × fsw × Iout)
Boundary between CCM and DCM at rated load.

History of the Boost Converter

The boost topology\'s fundamental principle — using inductor flyback to generate a higher voltage than the input — was exploited long before it was formalized. Nineteenth-century induction-coil X-ray sources, Kettering\'s 1910 automotive ignition coil, and Tesla\'s resonant transformers all used the same basic mechanism: dump energy into an inductor, then rapidly interrupt the current to spike the voltage. The modern switching-regulator boost topology was formalized alongside the buck in the 1960s, when integrated PWM controllers made continuous high-frequency switching practical.

The unique challenge of boost design — the right-half-plane zero (RHPZ) in its small-signal control transfer function — was characterized in the early 1970s by researchers including Slobodan Ćuk at Caltech. The RHPZ causes boost converters to briefly decrease output voltage in response to a step load increase (because the switch duty has to drop momentarily to redirect inductor current to the output), making feedback compensation trickier than in buck topology. This is why boost control loops typically have lower bandwidth than buck loops of the same frequency.

Boost converters dominate applications where a battery voltage needs to be stepped up: single-cell LED drivers, USB hosts from lithium batteries, e-paper display bias generators, and solar MPPT chargers. Synchronous boost converters (replacing the diode with a high-side MOSFET) now reach 95%+ efficiency at multi-amp loads; pulse-skipping modes extend that efficiency to micro-amp standby currents.

About This Calculator

Enter input voltage (lower), desired output voltage (higher), load current, switching frequency, and inductor/capacitor values. The calculator returns duty cycle D = 1 − Vin/Vout, average input current (which is higher than output current by the step-up ratio), peak inductor current, and output voltage ripple.

Rule of thumb: avoid step-up ratios above 5:1 in a single stage — above that, duty cycle approaches 90%+ and peak currents explode. Use cascaded boosts, flyback, or charge-pump topologies for very high step-ups. Inductor saturation rating must exceed peak IL, and the output diode/switch must handle Vout reverse voltage plus any ringing. All math runs client-side.

Frequently Asked Questions

What is a boost converter?

A switched-mode converter that steps voltage up. When the switch closes, current ramps up in an inductor. When it opens, the stored energy is dumped into the output through a diode. Result: Vout > Vin, at lower current.

Why are peak currents so high?

In a boost, the inductor sees full input current during the ON time, but only delivers current to the load during OFF time. For Vout = 2×Vin, the inductor carries roughly 2× the load current. This is why boost designs use beefier inductors and switches than equivalent bucks.

Can a boost short the input?

Yes — at D approaching 100%, the switch is closed most of the time, creating a near-short across the inductor. Real designs limit D to ~90% max and include current-limit protection. Boost converters also can't regulate when Vin > Vout (pass-through still happens through the diode).

What's a typical use case?

Battery-powered devices where the load needs more voltage than the cell provides. Single Li-ion (3.7V) boosted to 5V for USB peripherals, 12V for motors, or the high voltages needed to drive white LEDs from low-voltage sources.

Common Use Cases

Single-Cell to 5V

Li-ion (3.0-4.2V) boosted to 5V at 1A for USB output in portable devices.

LED Flashlight Driver

Single AA (1.2-1.5V) boosted to 3.3V to drive a white LED at ~350mA.

E-Paper Display

E-ink requires ±15V or ±30V rails. A boost converter generates these from the battery voltage.

Data Logger Radio

Coin cell (3V) boosted to 4.5V briefly during radio transmission bursts — large peak current during the TX, sleep between.

Solar Charge Controller

Low-voltage solar panel (~5V) boosted to 12V or 24V for battery charging; MPPT variant tracks maximum power point.

Last updated: