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Cycloidal Reducer

It is easy to forget how much of the modern world turns slowly and precisely: the joints of a robot arm, the axis of a tracking telescope, the wrist of a machine that places parts thinner than a hair. Each one needs a fast, gentle motor turned into a slow, powerful, almost play-free motion, and one neat way to do that is the cycloidal reducer. In motion it is hard to follow, so we won’t start with the finished machine. We’ll begin with a single shaft and build it up one piece at a time. Every figure below is live: drag it to turn it, and use the sliders to see what is going on inside.

Start with a single shaft

Here is the input shaft. Drag it.

Drag to rotate the input shaft.

What we usually want is the opposite: slow but strong.

The usual way: gears

A small gear driving a big one.

A small gear turns a big gear. The reduction equals the size ratio.

Gears are simple and cheap, but they have weak spots.

The worst, for precise motion, is that real teeth must mesh with a little clearance. Watch the pair rock back and forth, and drag the slider to change how tightly the teeth mesh.

Too loose (right) and the driven gear lags on every reversal — that lost motion is backlash. Too tight (left) and the teeth bind: the motion judders and the contact runs hot and wears (the red flush). Gears only run well in the narrow band between slop and jamming.

tight loose

And that is not the only catch: only one or two teeth ever touch, so a few teeth carry the whole load. To reach a high ratio you stack stage after stage, and the box keeps growing. So we want a drive with no gap to cross, with the load shared across many contacts, small enough to stay a single stage. Let’s build one.

A different idea: a ring of pins

Fix a ring of smooth round pins into the housing.

A fixed ring of pins. Nothing moves yet.

Push, don’t spin

Mount a disc on an eccentric and shove its centre around a tiny circle.

The eccentric carries the disc’s centre around a small circle. It shifts, it doesn’t spin.

On its own the disc would just slide around forever. But the ring of pins is in the way.

Forced to roll

The eccentric can only shove the disc sideways; it can’t spin it. Pressed against the fixed pins, the disc has no choice but to roll along the inside of the ring, like a coin rolling inside a cup.

Red arrows: the loaded pins pushing back on the disc, which forces it to roll. Follow the blue lobe drifting slowly backward.

Several pins share that push at once, and the press-and-react against the fixed ring is what both rolls the disc and lets it carry a load. As the eccentric whips its centre round fast, the disc itself turns slowly, and the other way.

How much it reduces: one fewer lobe

Like the gears earlier, the amount of reduction comes from a count. Here it is the lobes: the disc has exactly one fewer lobe than there are pins, so each input turn slips it back by just one pin.

11 pins · 10 lobes
Input 0.0 turns → output 0.00

One pin out of N is 1/N of a turn, so the reduction ratio is simply the lobe count. Drag the slider: more lobes, more reduction.

Collecting the slow turn

We now have our slow turn. But the disc carrying it is also wobbling, and that slow turn is buried under the wobble. Bolt a load straight onto the disc and it would just shake.

Output pins ride in holes wider than themselves by exactly the wobble. The disc wobbles freely in that slack; the hole edge (white arrows) only ever pushes its pin round the slow way. Those pins tie to one plate, the output shaft.

Input 0.0 turns → output 0.00

So the wobble is absorbed and only the slow turn reaches the output. Now let’s see how all the parts fit together.

How the output binds to the shaft

Last step: fix that whole ring of output pins onto a single green plate. The plate plus its pins is one rigid piece, and that piece is the output shaft. Drag the slider to slide it together with the rest, or apart.

input shaft + eccentric cycloidal disc output plate + pins = output shaft

The green pins stand up from the green plate and plug into the disc’s big holes. The input shaft passes down through a hole in the middle of the green plate without touching it. So the input shaft (up) and the output shaft (down) share the dash-dot axis but turn independently.

assembled exploded

And it’s small

Here is the payoff. To reach a high ratio, an ordinary gear train has to stack stage after stage, and the box keeps growing. A cycloidal drive gets the same ratio from one flat stage. Drag the slider and compare.

cycloidal: 1 stage · gear train: 3 stages
ratio 20:1

As you crank the ratio up, the cycloidal pin ring grows because the pins still need real spacing. The difference is that it stays one flat stage, while the gear train adds more stages.

Cycloidal vs gears, side by side

We started with the gears’ weak spots; now that the whole drive is built, here is how the two stack up, point for point. Every line is one of those early complaints, answered.

Ordinary gears Cycloidal reducer
Load contact Only one or two teeth mesh, so they carry the whole load. Many pins press at once and share the load.
Backlash Gaps between teeth let the output jiggle. Rolling pins leave almost no play.
Wear & life The few loaded teeth wear fastest. Shared load and rolling contact wear slowly.
Shock loads A sudden jolt lands on one tooth, which can chip. Many points of contact absorb sudden overloads.
High ratio, small box High ratios need stage after stage; the box keeps growing. One flat stage reaches the same ratio.

None of this makes gears bad — they are cheaper, simpler, and more efficient per stage, which is why they are everywhere. But where motion has to be slow, strong, and almost play-free inside a small space, the cycloidal drive is hard to beat.