Internal Combustion
Wankel Rotary Engine
A triangular rotor in an epitrochoidal housing — three combustion events per rotor revolution
A Wankel rotary engine replaces the reciprocating piston with a triangular rotor sweeping an epitrochoidal housing. Three combustion events per rotor revolution, double the power density of a piston engine — and an Achilles heel called the apex seal.
- Combustion events3 per rotor turn, 1 per shaft turn
- Power density~2× equivalent-displacement piston engine
- BSFC290 g/kW·h (Wankel) vs ~240 (piston)
- InventedFelix Wankel, prototype 1957 (DKM 54)
- IconMazda 13B-REW, RX-7 FD, 206 kW (280 hp)
- Le Mans winnerMazda 787B 26B, 1991 — 522 kW from 2.6 L
Interactive visualization
Press play, or step through manually. Watch the rotor's eccentric orbit, three faces each running through intake, compression, power, exhaust on every rotor revolution.
Watch the 60-second explainer
A condensed visual walkthrough — narrated, captioned, under a minute.
Why anybody ever built a rotary engine
The reciprocating piston engine is, in mechanical terms, an absurdity. A column of metal accelerates from zero to 25 m/s and back to zero, twice per revolution, while a connecting rod, crankshaft, balance shafts, valves, springs, cams, lifters, and pushrods conspire to translate that lurching one-dimensional motion into smooth shaft rotation. At 7,000 rpm a small piston changes direction 14,000 times per minute and the inertia loads can exceed the combustion loads. Every gram of reciprocating mass costs an exponential price in vibration and bearing wear.
Felix Wankel's insight in the early 1950s — first realised in the DKM 54 of 1957 — was a combustion engine with no reciprocating parts at all. A single triangular rotor turns inside a peanut-shaped housing. Three independent combustion chambers, formed between the three rotor faces and the housing wall, each go through intake, compression, power, and exhaust simultaneously. There is no valvetrain. There is no connecting rod. The only moving parts are the rotor, the eccentric shaft, the apex seals, and the side seals. A single-rotor Wankel has about a dozen moving components total; a single-cylinder piston engine has fifty.
The price for that simplicity is paid in three currencies. First, sealing — each rotor apex must drag a 3 mm steel strip past the housing wall at 16 m/s while keeping combustion gas in the right chamber. Second, fuel economy — the long, thin combustion chamber has a high surface-to-volume ratio at TDC and the flame must travel far. Third, emissions — slow combustion plus partial quench near the housing walls means high HC. The rest of this article is the engineering of that trade.
The epitrochoid and the 3:2 internal gearing
The housing's inner profile is an epitrochoid — the curve traced by a point on a circle of radius r rolling around the outside of a fixed circle of radius R, with R = 2r. Mathematically:
x(t) = (R + r) cos(t) − e cos((R + r)/r × t)
y(t) = (R + r) sin(t) − e sin((R + r)/r × t)
with R = 2r, (R + r)/r = 3: the housing has 2 lobes
and the rotor must have 3 vertices to seal against 2 lobes.
Eccentricity e: the offset between rotor centre and shaft centre.
Generating radius R: determines the housing's "long radius".
On a Mazda 13B: R ≈ 105 mm, e ≈ 15 mm.
The rotor itself rides on an eccentric — a lobe of radius e ground onto the central output shaft, offset from the shaft centreline. A large internal-tooth gear inside the rotor meshes with a stationary external pinion bolted to the side housing. The tooth ratio is exactly 3:2 — there are 3 teeth on the rotor's internal gear for every 2 on the stationary pinion (typically 24:16 or 30:20 in practice). That ratio mechanically constrains the rotor to turn exactly one-third of a revolution about its own axis for every full revolution of the eccentric shaft.
So in one full shaft turn: the eccentric makes one full orbit, dragging the rotor's centre around with it; the rotor rotates 120° about its own axis; one of the three rotor faces completes one full intake-compression-power-exhaust cycle. After three shaft turns the rotor has completed one full revolution and all three faces have each fired once. Power output rate: one combustion event per shaft revolution — comparable to a two-cylinder four-stroke piston engine.
The four phases — same as a four-stroke, but in parallel
Each of the three rotor faces continuously runs through the same four phases as a piston engine, but staggered 120° apart. At any given instant, all four phases are happening at once on different faces. The phases:
- Intake. A rotor face passes the intake port; the trailing apex uncovers the port; the trapped volume grows; fresh mixture rushes in. The intake port is cut into the side housing (later Mazda Renesis) or the peripheral housing (earlier 12A and 13B-REW). Port geometry determines the engine's character: side ports give clean idle and low emissions but limit top-end; peripheral ports give explosive top-end but bad idle.
- Compression. Both the leading and trailing apexes of that face are now between ports; the trapped volume shrinks as the rotor advances; pressure rises 8 to 10 times. Compression ratio is typically 9:1 on a naturally aspirated 13B, 8.5:1 on the turbocharged 13B-REW.
- Power. The face passes the spark plug (often two: leading and trailing); combustion sweeps from the leading edge of the chamber to the trailing edge; expanding gas pushes the rotor face outward, which (via the eccentric) drives the central shaft. Combustion is slow compared to a piston engine — the chamber is roughly 8 cm long and the flame must traverse it.
- Exhaust. The leading apex uncovers the exhaust port; the volume shrinks as the rotor advances; spent gas evacuates. Wankels famously have no exhaust valve overlap with intake (the geometry separates the ports), so no scavenging is possible — which is good for emissions but means the engine can't use exhaust pulse tuning to boost mid-range torque.
Worked example — sizing a Mazda 13B
The 13B (twin-rotor, 1.3 litres displacement total) is the canonical Wankel. Its dimensions are public. Let's work through the kinematics.
Geometry:
Generating radius R = 105 mm
Eccentricity e = 15 mm
Rotor face width B = 80 mm
Compression ratio = 9.0:1 (naturally aspirated)
Effective displacement = 654 cc per rotor → 1308 cc twin
Manufacturer's rating (1992 FD RX-7, 13B-REW twin-turbo):
Power = 206 kW @ 6500 rpm
Torque = 314 Nm @ 5000 rpm
Red line = 8000 rpm
Power-impulse rate:
1 combustion per shaft turn × 2 rotors = 2 impulses / shaft turn
At 6500 rpm: 6500 / 60 × 2 = 217 power impulses / second
Equivalent piston engine: 4-cylinder 4-stroke at same rpm
= 6500 / 60 × 4 / 2 = 217 / s (identical!)
Specific output:
206 kW / 1.308 L = 157 kW/L (twin-turbo)
175 kW / 1.308 L = 134 kW/L (Renesis NA, RX-8 2003)
Compare: Honda K20A i-VTEC 2.0L NA = 110 kW/L
Fuel economy (BSFC):
13B-REW under load: 290 g/kW·h
Honda B16B NA: 240 g/kW·h
Penalty: ~20 % more fuel for same work
Two things stand out. First, the rotor's power-impulse rate is identical to a comparable 4-cylinder piston engine at the same rpm — they are kinematically the same. Second, the specific power per litre is roughly double what a naturally aspirated piston engine of the era could deliver. That's the entire commercial case for the Wankel — you can pack RX-7-class performance into an engine bay one-third smaller than the equivalent V6, which is exactly what Mazda did.
The apex-seal problem in detail
Three apex seals (one at each rotor tip), six side seals (running along each side of the rotor between apexes), and three corner seals (where apex meets side seal) together do the job a set of piston rings does on a reciprocating engine. The apex seals are the killer.
Each apex seal is a steel or carbon-impregnated strip roughly 3 mm wide, 8 mm tall, and the rotor's full thickness (80 mm on a 13B). It sits in a groove machined into the rotor tip with a spring underneath pressing it outward. Combustion-chamber pressure also enters a relief behind the seal, augmenting the spring force when load is highest. The seal slides at the rotor-tip velocity past the chrome- or ceramic-coated housing inner wall — about 16 m/s at 9,000 rpm.
The wear mechanisms that limit life are:
- Adhesive wear. Local micro-welding between seal and housing when the lubricating oil film thins. Cured by adding small amounts of two-stroke-style oil to the intake charge (Mazda's premix or OMP — Oil Metering Pump — system).
- Abrasive wear. Carbon particles from incomplete combustion act as grinding paste. Cured by direct injection (Renesis 13B has port injection but later experimental versions used DI) and rich-burn calibration.
- Apex-seal flutter. At high rpm the seal can momentarily lift off the housing wall as gas pressure behind it cycles. Cured by stiffer springs and lower seal mass — carbon fibre or PEEK seals.
- Spring fatigue. The spring under each seal cycles at engine rpm. After 100,000+ km of fatigue the spring relaxes and seal contact pressure drops. Cured by twin springs or wave-spring designs.
- Thermal distortion. The housing's lobe centre runs hotter than the side housings; differential thermal expansion creates oval distortion of the trochoid. The seal must conform. Cured by ceramic housings (experimental only) or careful coolant routing.
Mazda's evolution of apex-seal life is a microcosm of the rotary's history. The 1967 10A used flat steel apex seals lasting 50,000 km. The 1992 13B-REW used four-piece tipped seals with carbon-impregnated apex caps lasting 150,000 km. The 2003 Renesis used ceramic-tipped seals lasting 200,000 km under good maintenance. None ever matched a piston engine's typical 300,000 km piston-ring life, which is the entire reliability-perception problem of the rotary.
Variants and notable configurations
| Variant | Rotors | Displacement | Output | Application |
|---|---|---|---|---|
| NSU KKM 502 | 1 | 500 cc | ~30 kW | 1964 NSU Spider — first production Wankel |
| Mazda 10A | 2 | 982 cc | 82 kW | 1967 Cosmo Sport |
| Mazda 12A | 2 | 1146 cc | 96 kW | 1978 RX-7 FB, peripheral port |
| Mazda 13B-REW | 2 | 1308 cc | 206 kW | 1992 RX-7 FD — twin sequential turbo |
| Mazda Renesis 13B | 2 | 1308 cc | 175 kW NA | 2003 RX-8 — side intake ports |
| Mazda 26B | 4 | 2616 cc | 522 kW | 1991 787B — Le Mans winner |
| NSU Ro80 | 2 | 995 cc | 85 kW | 1967 sedan — premature apex-seal failure killed NSU |
| Mercedes C111 III | 4 | 3600 cc | 257 kW | 1970 concept — never produced |
| Mazda 8C | 1 | 830 cc | 55 kW gen | 2023 MX-30 R-EV range-extender |
Failure modes — what actually kills a rotary
- Apex-seal failure. Most common. Symptom: low compression on one face of one rotor (180–250 kPa instead of 700+). Diagnosis: compression test with rotary-specific tester. Cure: rotor rebuild, ~3000 USD.
- Side-seal failure. Less common but as terminal. Symptoms: oil burning, blue smoke under boost. Cure: full engine rebuild.
- Coolant-seal failure. O-rings between the side housings and rotor housings fail under thermal cycling. Symptom: coolant in oil, milky oil cap. Cure: rebuild, typically combined with apex-seal refresh.
- Stationary-gear fracture. The internal-pinion gear that constrains rotor rotation can crack at very high rpm. Symptom: catastrophic engine failure. Cure: replace the side housing.
- Carbon build-up in ports. The Renesis side ports plug with carbon over 50,000 km on cars driven gently, costing power and creating idle problems. Cure: periodic 'Italian tune-up' (high-rpm operation) or chemical decarbonisation.
- Catalyst meltdown. If the engine runs rich for extended periods (a common failure mode of older rotaries) the catalytic converter overheats and the substrate melts. Common 1980s–1990s RX-7 failure; cured on the RX-8 by tighter combustion control.
How the Wankel compares to a four-stroke piston
| Property | Wankel | 4-stroke piston (similar displacement) |
|---|---|---|
| Specific power (kW/L) | 130–160 NA, 200+ turbo | 60–100 NA, 130+ turbo |
| Moving parts (single-cyl/rotor) | ~12 | ~40–50 |
| BSFC (g/kW·h) | 280–300 | 230–260 |
| Smoothness | Excellent (no reciprocating mass) | Requires balance shafts |
| Red line (rpm) | 8,000–9,000 (street); 10,500 (race) | 6,500–7,500 typical |
| HC emissions | High (wall quench) | Lower |
| Apex/ring life | 150,000–200,000 km | 250,000–400,000 km |
| Cold-start emissions | Worse (cool walls) | Better |
| Power density (kW/kg) | 1.5–2.0 | 0.7–1.2 |
Why Mazda brought it back — and what comes next
The MX-30 R-EV (2023) put a single-rotor 8C Wankel back in a Mazda showroom for the first time since 2012. The engine is a 0.83-litre single-rotor making 55 kW (74 hp), used not as a traction engine but as a series-hybrid range-extender feeding a generator. It runs at near-constant rpm and load — the worst conditions for a rotary's fuel economy (transient response) are eliminated. The smooth, compact, light Wankel is well-suited to that duty: it tucks into the wheel-arch space ahead of the front axle without intruding into the cabin, weighs ~15 kg less than a comparable piston engine, and produces no second-order vibration that would otherwise leak into the cabin floor.
Hydrogen rotary research at Mazda continues. The wide flammability range and high flame speed of hydrogen partially compensate for the long, thin combustion chamber that hurts gasoline rotaries; emissions become trivial (water vapour plus a little NOx); the apex-seal problem persists but is no worse. A future MX-30 R-EV variant running on hydrogen is openly speculated about and consistent with Mazda's public patent activity.
What the Wankel demonstrably is not: a viable replacement for the piston engine in mainstream automotive applications. The fuel-economy disadvantage and apex-seal life problem have never been solved at scale, and the regulatory and emissions targets of the 2020s do not tolerate either. What it is: an extraordinary special-purpose engine for niches where smoothness, power density, and packaging matter more than fuel economy — exactly the niches Mazda keeps finding for it.
Common pitfalls when learning the rotary
- Counting combustion events wrong. Three per rotor revolution, one per shaft revolution (3:1 gearing). The shaft turns three times faster than the rotor. A single-rotor 13B has the same power-impulse rate as a two-cylinder four-stroke.
- Thinking the rotor 'spins'. It orbits and rotates at the same time. The combination produces the trochoidal sweep — neither motion alone gives the working chambers.
- Treating it like a high-rpm piston. Wankels need the OMP oil injection working perfectly, premix fuel for serious abuse, and a 30-second cool-down after hard running. They cost more in consumables than a piston engine of equal output.
- Ignoring the housing-coating spec. Different generations used chrome, Nikasil, or steel TiN coatings. The wrong oil for the wrong coating accelerates wear. The owner's manual is not optional.
- Believing turbocharging fixes the BSFC problem. Forced induction increases peak power but does not improve BSFC — it makes the surface-to-volume problem worse by raising peak cylinder pressure. The 13B-REW is faster than the Renesis NA but uses more fuel.
Frequently asked questions
How does a Wankel rotary engine actually work?
A triangular rotor with curved sides spins inside an epitrochoidal housing — a peanut-shaped curve. The rotor rides on an eccentric on the central output shaft, so the rotor's centre orbits a small circle while the rotor itself rotates more slowly about its own axis (3:1 ratio, geared by internal-tooth pinions). Each of the rotor's three faces traps a working chamber against the housing wall, and as the rotor moves each chamber expands and contracts through intake, compression, power, and exhaust in turn. Three combustion events per rotor revolution, one per shaft revolution.
Why was the Wankel ever attractive in the first place?
Three real advantages: mechanical simplicity (no valves, no rods, ~12 moving parts per rotor), smoothness (no reciprocating mass, smooth past 9,000 rpm), and power density (a 1.3 L 13B made 206 kW twin-turbo — twice the specific power of a same-displacement piston engine). The 1991 Le Mans-winning Mazda 787B 26B made 522 kW from 2.6 L at 9,000 rpm.
What is the apex-seal problem?
Each rotor tip carries a thin steel or carbon strip pressed outward against the housing wall by a spring. It must seal combustion gases while sliding at 16 m/s past the housing wall. Wear is far higher than a piston ring. Apex seals failed at 50,000 km on early 1960s rotaries; later ceramic-tipped versions reach 200,000+ km but rarely match a piston engine's 300,000 km ring life. Failed apex seals leak combustion gas and produce a 'cold rotor' on the compression test.
Why does a Wankel use more fuel than a piston engine?
Three reasons. (1) The combustion chamber is long and thin — flame must travel further, losing heat to walls. (2) High surface-area-to-volume ratio at TDC means more heat-transfer loss. (3) Apex-seal leakage adds a few percent cycle work loss. Net: BSFC of 290 g/kW·h vs ~240 for a comparable piston engine — about 20 percent worse fuel economy.
Where has Mazda actually used the rotary engine in production?
1967 Cosmo Sport (10A) → R100, RX-2, RX-3, RX-5 sedans → 1978 RX-7 SA/FB (12A) → 1985 RX-7 FC → 1992 RX-7 FD (twin-turbo 13B-REW, 206 kW) → 2003 RX-8 (Renesis side-port 13B, 175 kW). Production ended 2012. 2023 MX-30 R-EV: single-rotor 8C as an EV range-extender. The 1991 four-rotor 26B won Le Mans.
What about hydrogen rotaries — does it solve the emissions problem?
Partially. Hydrogen's wide flammability range and high flame speed compensate for the slow-burn / long-chamber problem. Mazda demonstrated the RX-8 Hydrogen RE (2006) and Premacy Hydrogen RE (2009). The architecture separates intake from combustion better than a piston engine, reducing pre-ignition risk. NOx is still produced; unburned-fuel emissions effectively go to zero. A future hydrogen MX-30 R-EV variant is openly speculated about.
How does the rotary actually move — is the rotor spinning or orbiting?
Both, simultaneously. The output shaft carries an eccentric lobe offset from centreline. The rotor rides on a bearing around that eccentric, so the rotor's centre traces a circle (orbit). Inside the rotor a large internal gear meshes with a stationary external pinion at 3:2 ratio, forcing the rotor to rotate at one-third the shaft speed. Combined motion sweeps three trochoidal pockets through intake-compression-power-exhaust three times per rotor turn.