The diffuser: the pump at the back
The suction under a ground-effect car is made at the floor's narrow throat — but it is the diffuser, the gentle upward ramp at the back, that makes it possible. Its job sounds humble: slow the fast underbody air back down and hand it to the outside world at street pressure. Do it gracefully and the whole floor pulls harder. Ask one degree too much and the flow lets go, the tunnel chokes, and the downforce collapses mid-corner.
The pump is at the back
The ground-effect chapter told the front half of the story: squeeze air through a narrowing tunnel under the car, it speeds up, its pressure drops, and the floor becomes a suction pad. But that air cannot simply be dumped at the back still travelling far faster than the world around it — flow only keeps rushing into the tunnel if there is a graceful way out. That is the diffuser: an expanding ramp that trades the air's speed back for pressure, delivering it to the wake at roughly ambient conditions. Seen from the physics, the low-pressure throat is not where the work is done at all — the diffuser at the exit is the pump that keeps the whole floor drinking.
The exit sets the flow
How much air the tunnel can swallow — and therefore how hard the throat can suck — is fixed by how much speed the diffuser can shed at the exit. A bigger, well-behaved diffuser means faster air at the throat and more suction everywhere upstream. This is why designers speak of a floor being “pumped” by its diffuser, and why so much of a modern car's downforce is decided in the last half-metre of its underside. Make the ramp steeper and the floor pulls harder, lap after lap — which invites the obvious question: why not steeper still?
Adverse pressure is a cliff
Because slowing air against rising pressure is the hardest thing in aerodynamics. Air accelerating into falling pressure clings happily to any surface; air being asked to climb into risingpressure is always looking for an excuse to give up. The excuse is the ramp angle: past roughly a 10–14° effective slope, the flow separates from the diffuser wall, the tunnel chokes on its own turbulence, and the downforce doesn't fade — it collapses. The wing chapter met this same physics as the stall; the diffuser is a stall you drive on. The Lotus 79's designers lived one degree from that cliff, and every ground-effect designer since has too.
Still the game today
Skirts were banned, flat floors mandated, shaped floors returned — but through every rulebook since 1978, one thing has stayed constant: every racing car's floor ends in a diffuser, and diffuser behaviour still decides how much of the floor's potential the car actually keeps. Even on road cars the idea has quietly taken over: the upswept rear undertray on an ordinary hatchback is a diffuser in civilian clothes, tidying the wake to cut drag rather than to make grip.
Go deeper: pressure recovery and separationfor engineers
Along the floor, Bernoulli links speed and pressure: is (nearly) constant, so the throat's high speed is its low pressure. The diffuser must then recover from throat pressure back to ambient across its length. Its performance is measured by the pressure-recovery coefficient
The steeper the ramp, the more recovery is demanded per metre — but the boundary layer, already slowed by friction, has the least momentum of any air in the tunnel and is the first to surrender to the rising pressure. When it reverses, the flow separates and the effective tunnel shape is no longer the metal one. The 10–14° figure is not a law of nature but a robust rule of thumb for single-plane diffusers; multi-element designs, vortex generators and blown floors all exist to bribe the boundary layer into climbing a steeper hill.