DC-DC · Ćuk (Inverting) · Virtual Lab

Ćuk Converter Simulator

An advanced, physics-accurate simulator of the DC-DC Ćuk converter — a two-inductor, two-capacitor topology that transfers energy through a series coupling capacitor and delivers a negative output with unusually low input and output current ripple. Sweep the duty cycle D, switching frequency, the two inductors and capacitors and the load, add a real device model, and watch every waveform on a real-time oscilloscope — validated live against Vo = −D·Vin/(1 − D) and coupling-cap voltage Vin/(1 − D), with efficiency and a conduction-loss breakdown.

Ćuk DC-DC converter circuit: input inductor L1, MOSFET switch, series coupling capacitor C1, diode, output inductor L2 and output capacitor C2 producing a negative output voltage across load R
Ćuk converter — energy passes through the coupling capacitor C1; the two inductors L1, L2 give low input and output current ripple. Vo = −D·Vin/(1 − D).

Parameters

|Vo| = D·Vin/(1−D) · D<0.5 step-down · D>0.5 step-up
V

Power stage (L₁ L₂ · C₁ C₂ · load)

Device & parasitics model

Ideal (all 0) gives Vo = −D·Vin/(1−D) exactly; add parasitics to see the real drooped output, ripple and losses.

Sampling & display

Points plotted per switching period

Presets

Waveforms to display

Waveforms — one steady-state switching period Ćuk

Vin v_C1 coupling Vo output (−) i_L1 input i_L2 output i_Q / i_D
LIVE

Efficiency & conduction-loss breakdown

Estimated efficiency (conduction losses)
Power lost in each component, computed from the true integrated currents: MOSFET Rds(on), diode Vf, inductor DCR and output-capacitor ESR. Set parasitics above to see the split.

Measurements

Live accuracy check — simulation vs closed-form theory

Output voltage  
Coupling cap & ripple  

What is a Ćuk converter?

The Ćuk converter (named after Slobodan Ćuk) is a DC-DC converter that, like the buck-boost, produces an inverted output that can be higher or lower than the input — but it does so with far lower current ripple on both the source and the load. Its trick is to transfer energy through a series coupling capacitor C₁ rather than an inductor, with an input inductor L₁ and an output inductor L₂ smoothing the two port currents.

How it works — the two switching states

  • Switch ON (0 → D·T): the MOSFET conducts; L₁ charges from Vin while the coupling capacitor C₁ discharges through L₂ into the output. The diode is off.
  • Switch OFF (D·T → T): the diode conducts; L₁ recharges C₁ while L₂ maintains the output current. Volt-second balance on the two inductors sets the conversion ratio.

Key equations

Vo = − D·Vin / (1 − D) (ideal, continuous conduction)
v_C1(avg) = Vin / (1 − D) = Vin + |Vo| · ΔiL = Vin·D/(L·fsw)
Switch & diode blocking voltage = v_C1 = Vin + |Vo|

This simulator numerically integrates the full 4th-order switching circuit (two inductors, two capacitors) with your device parasitics to steady state, then measures Vo, the coupling-cap voltage, the ripple and the losses from the resulting waveforms and compares them to the equations above.

Why the low ripple?

Because an inductor sits in series with both the input and the output, the source and load currents are continuous triangular waveforms rather than the pulsed currents of a basic buck-boost. This reduces conducted EMI at the input and ripple at the output — the Ćuk's main advantage. The cost is an extra inductor and capacitor, and a coupling capacitor C₁ that must handle a large RMS ripple current.

Ćuk vs SEPIC vs ZETA

ConverterPolarityIdeal VoRipple
ĆukInverting (−)−D·Vin/(1−D)Low in & out
SEPICNon-inverting (+)D·Vin/(1−D)Low input
ZETANon-inverting (+)D·Vin/(1−D)Low output

See the SEPIC and ZETA simulators for the non-inverting relatives.

Applications

Low-noise negative-rail supplies, LED drivers, and any application where low input/output current ripple and a wide step-up/step-down range matter more than component count.

Frequently asked questions

What is the output voltage of a Ćuk converter?

In CCM the ideal output is Vo = −D·Vin/(1 − D) — negative, same magnitude as a buck-boost but with much lower ripple.

What is the coupling-capacitor voltage?

The average voltage across C₁ is Vin/(1 − D) = Vin + |Vo| — the simulator plots it live.

Why does the Ćuk have low ripple?

An inductor is in series with both the input and the output, so both port currents are smooth triangular waves rather than pulses.

What must the switch and diode withstand?

Both block the coupling-cap voltage Vin + |Vo| = Vin/(1 − D).

Power4All · Ćuk Converter interactive simulator. All waveforms are produced by numerical integration of the actual 4th-order switching circuit and validated against closed-form theory.