What is Ripple & Ripple Factor?

The complete guide to ripple — the leftover AC riding on a rectifier’s DC output — and the ripple factor γ = Vr(rms)/Vdc = √(FF² − 1) that measures it: why half-wave gives 1.21 and full-wave 0.48, how a smoothing capacitor tames it, and how to reduce and measure it.

Complete Learning Path — Ripple & Ripple Factor

From what ripple is and the ripple factor formula, to half-wave vs full-wave values, capacitor smoothing, reducing ripple, why it matters and how to measure it

What is Ripple?

Ripple is the small, leftover AC variation that rides on the DC output of a rectifier or power supply. Real DC is never perfectly flat — a periodic wobble sits on top of the steady level.

When AC is rectified, the output is a train of humps, not a flat line. Even after a smoothing filter, some of that variation survives. That residual AC is the ripple voltage Vr, and the steady part it rides on is the DC value Vdc — the average value of the output.

A DC output level shown as a dashed line with a small periodic AC ripple wave riding on top, and the peak-to-peak ripple voltage marked on the right
A real supply output = a steady DC average with a small periodic ripple riding on it. The height of that wobble is the ripple voltage; how much AC is left compared with the DC is what the ripple factor measures.
Vr
AC ripple voltage
Vdc
Steady DC (average) level
γ
Ripple factor (ratio)
Lower = better
Smoother DC
Ripple = the AC that survived rectifying & filtering

A perfect DC supply would have zero ripple. In practice we design the filter so the ripple is small enough for the load — the goal is a low ripple factor, not zero.

Ripple Factor & Its Formula

The ripple factor γ is the ratio of the rms value of the AC ripple to the DC value. Split the output into a DC part plus a pure ripple part, and γ compares the two.

The rectifier output decomposed as a steady DC value plus an AC ripple component, with the ripple factor defined as gamma equals ripple rms divided by DC value equals root of form factor squared minus one
Any rectified output is a DC value plus an AC ripple. The ripple factor is the rms of that ripple divided by the DC level — equivalently √(FF² − 1), where FF is the form factor.

γ = Vr(rms) / Vdc = √(FF² − 1)

Ripple factor — rms ripple over DC value; also from the form factor FF = Vrms/Vdc

The second form drops out of the fact that the total rms squared equals the DC squared plus the ripple rms squared: Vrms² = Vdc² + Vr(rms)². Divide through by Vdc² and you get γ = √(FF² − 1). Percentage ripple is just γ × 100%.

Worked example — ripple factor from measurements

A supply reads Vdc = 12 V on a DC meter and Vr(rms) = 0.30 V of AC ripple on an AC meter. The ripple factor is:

γ = 0.30 / 12 = 0.025 = 2.5% ripple

That is a fairly clean supply — well below the 48% of an unfiltered full-wave rectifier.

Rule of thumb

Smaller γ → smoother DC. An ideal battery has γ = 0; a raw rectifier can be over 1; a good regulated supply is a tiny fraction of a percent.

Half-wave vs Full-wave Ripple

The type of rectifier sets the starting ripple. A half-wave rectifier throws away half of every cycle, so it ripples badly; a full-wave or bridge rectifier fills both halves and doubles the ripple frequency.

Half-wave rectified output with large gaps and ripple factor 1.21 at line frequency compared with full-wave rectified output with ripple factor 0.48 at twice the line frequency
Half-wave (left) leaves big gaps — ripple factor 1.21 at the line frequency f. Full-wave (right) has no gaps and twice as many humps — ripple factor 0.48 at 2f, which a filter smooths far more easily.
Rectifier (no filter)Ripple factor γ% RippleRipple frequencyVdc
Half-wave1.21121%f (50 / 60 Hz)0.318 Vm
Full-wave (centre-tap)0.4848%2f (100 / 120 Hz)0.637 Vm
Bridge0.4848%2f (100 / 120 Hz)0.637 Vm
Why full-wave wins twice

Full-wave rectification cuts the ripple factor from 1.21 to 0.48 and doubles the ripple frequency. Both help the filter: a higher frequency and smaller gaps mean a given capacitor smooths the output much better.

Smoothing with a Capacitor

A reservoir capacitor across the output is the classic ripple-buster. It charges to each rectified peak, then feeds the load while the rectifier voltage falls — turning the humps into a small sawtooth ripple.

A reservoir capacitor charging quickly to each rectified peak then discharging slowly into the load, producing a small sawtooth ripple with peak-to-peak equal to load current divided by frequency times capacitance
The capacitor charges fast to each peak, then discharges slowly into the load until the next peak tops it up. The result is a small sawtooth whose peak-to-peak height falls as the capacitance grows.

Vr(pp) ≈ Iload / (f · C)

Peak-to-peak ripple from a reservoir capacitor — use f = 2 × line frequency for full-wave

Because a sawtooth has an rms of about Vr(pp)/(2√3), the ripple factor of a capacitor-filtered full-wave supply works out to γ = 1 / (2√3 · f · Rload · C). Bigger C, bigger load resistance (lighter load), or higher f all shrink it.

Worked example — sizing a reservoir capacitor

A full-wave supply on 50 Hz mains (ripple at f = 100 Hz) delivers Iload = 0.5 A and we want Vr(pp) = 1 V:

C = I / (f · Vr(pp)) = 0.5 / (100 × 1) = 5000 µF

Try the Output Capacitor Ripple Calculator to size one for your own load.

Reducing the Ripple Factor

Once a capacitor has done the coarse work, several techniques push the ripple factor lower still — from a bigger reservoir to a full regulator.

Two capacitor-filtered outputs compared: a small capacitor gives a large sawtooth ripple and high ripple factor while a large capacitor gives a small ripple and low ripple factor
Double the capacitance (or halve the load current) and the sawtooth ripple roughly halves. That is the first and cheapest lever for a lower ripple factor.

Bigger capacitor

Ripple is inversely proportional to C. Doubling the reservoir roughly halves the ripple — the cheapest first step.

Full-wave instead of half

Switching to a bridge cuts γ from 1.21 to 0.48 and doubles the ripple frequency, so the same capacitor works twice as hard.

LC or π filter

Adding an inductor (choke) or a second capacitor forms an LC or π-filter that attenuates the ripple much further.

Voltage regulator

A linear or switching regulator has a high ripple rejection and can cut the remaining ripple by hundreds or thousands of times.

Ripple rejection ratio

A regulator’s ripple rejection (often 60–80 dB) says how much it suppresses input ripple. That is why almost every clean DC supply ends with a regulator stage.

Why Ripple Matters

Ripple is not just cosmetic — it shows up as real noise, flicker and heat, and every sensitive circuit sets a limit on how much it can tolerate.

Hum in audio

Ripple at 50/100 Hz leaks into amplifiers as an audible mains hum — a classic sign of a tired reservoir capacitor.

Noise on signals

Ripple on the rail adds noise to sensor, ADC and radio circuits, degrading accuracy and dynamic range.

Capacitor heating

The ripple current flowing in and out of the reservoir capacitor heats it up; exceeding its rating shortens its life.

Ripple current is a real rating

Electrolytic capacitors are rated for a maximum ripple current, not just voltage. In switching supplies this often decides the capacitor choice — see the Inductor Ripple Current Calculator.

Measuring Ripple

Ripple is measured as the AC riding on the DC, so you separate the two: read the DC level and the AC ripple, then take the ratio.

Oscilloscope (AC coupled)

AC-couple the scope to block the DC and magnify the ripple, then read its peak-to-peak or rms directly.

DMM: DC then AC

Read Vdc in DC mode and Vr(rms) in AC mode; γ = Vr(rms) / Vdc.

Ripple calculator

Predict it from the design with the Ripple & Form Factor Calculator.

Watch the coupling & bandwidth

Measure ripple AC-coupled and note the bandwidth — high-frequency switching spikes can dwarf the low-frequency sawtooth, and a wide-band reading looks worse than a filtered one.

Key Terms at a Glance

The essential ripple vocabulary students and engineers search for.

Ripple voltage (Vr)

The residual AC on the DC output.

Ripple factor (γ)

Vr(rms) / Vdc = √(FF² − 1).

Percentage ripple

γ × 100%.

Ripple frequency

f for half-wave, 2f for full-wave.

Reservoir capacitor

Charges to the peak, feeds the load between peaks.

Ripple current

The AC current heating the smoothing capacitor.

Frequently Asked Questions

Quick, expert answers to the questions people ask most about ripple and ripple factor.

What is ripple in a power supply?

Ripple is the small residual AC variation that remains on the DC output of a rectifier or power supply after filtering. Instead of a perfectly flat line, the output has a periodic wobble made of the rectifier’s output frequency and its harmonics.

What is ripple factor?

The ripple factor is the ratio of the rms of the AC ripple to the DC value of the output: γ = Vr(rms) / Vdc. It tells you how much AC is left on the DC — a smaller ripple factor means smoother, cleaner DC.

What is the formula for ripple factor?

It is γ = Vr(rms) / Vdc, which can also be written γ = √(FF² − 1) using the form factor FF = Vrms/Vdc, because the total rms squared equals the DC squared plus the ripple rms squared.

What is the ripple factor of a half-wave and full-wave rectifier?

Without a filter, a half-wave rectifier has a ripple factor of about 1.21 (121%) and a full-wave or bridge rectifier about 0.48 (48%). Full-wave is far lower because there are no gaps and the ripple frequency is doubled.

What is the ripple frequency?

For a half-wave rectifier it equals the line frequency (50 or 60 Hz). For a full-wave or bridge rectifier it is twice the line frequency (100 or 120 Hz), because both halves of every cycle produce an output hump.

How does a capacitor reduce ripple?

A reservoir capacitor charges to each rectified peak, then supplies the load as the rectifier voltage falls, so the output only sags a little before the next peak recharges it. This gives a small sawtooth ripple of roughly Vr(pp) = Iload / (f × C).

How do you reduce ripple further?

Use a larger capacitor, a full-wave instead of a half-wave rectifier, an LC or π filter, or a voltage regulator. A regulator has a high ripple rejection and can cut the remaining ripple by a factor of hundreds or thousands.

What is percentage ripple?

Percentage ripple is the ripple factor as a percentage: %ripple = γ × 100. An unfiltered full-wave rectifier at γ = 0.48 has 48% ripple; a well-filtered, regulated supply can be well under 1%.

Conclusion & Key Takeaways

Ripple is the AC that survives rectifying and filtering; the ripple factor γ = Vr(rms)/Vdc measures it. Full-wave rectification and a good smoothing capacitor bring it down, and a regulator finishes the job.

Ripple = leftover AC

A wobble on the DC output.

γ = Vr(rms)/Vdc

Also √(FF²−1).

Half 1.21, full 0.48

Full-wave also doubles f.

Capacitor smooths

Vr(pp) = I/(fC).

Lower = better

Bigger C, LC/π, regulator.

It matters

Hum, noise, capacitor heat.

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