Formula 1

Timelines · Formula 1 · 2 of 7

Lotus 491967

The car that discovered aircraft physics works upside down — bolt on wings, corner faster.

1967·Ford-Cosworth DFV 3.0 L V8 (structural)·~408 hp·Won on debut, 1967; 1968 Drivers’ title (G. Hill); 12 GP wins·~270 kg at 240 km/h with 1968 wings

· THE STORY

Aircraft physics, upside down

For sixty years racing cars had fought physics with grip from rubber alone. The Lotus 49 and its rivals realised you could take an aircraft wing, flip it upside down, and use the air itself to press the car into the road. Within two seasons every Formula 1 car sprouted wings, and cornering speeds jumped beyond what anyone had thought tyres could allow.

· WHY IT MATTERED

Downforce: free grip at speed

A tyre grips in proportion to how hard it is pressed down. Weight presses it down but must also be accelerated; a wing presses it down for nothing but a little drag. The faster you go, the harder the air pushes — exactly when you need the grip most.

tubsuspension bolts to the block
Cosworth DFV carrying the rear suspension — no frame around it

· WHY IT MATTERED

The engine as part of the car

The 49 bolted its Cosworth DFV engine directly to the back of the cockpit as a structural piece — no frame around it. Lighter and stiffer, and it gave the rear wing something solid to stand on. Every F1 car since is built this way.

load²
The 1968–69 high wing, on slender struts above the car

· WHY IT MATTERED

A warning written in broken wings

The first wings stood on tall, flexing struts and several collapsed at speed, causing huge crashes. The sport learned that aerodynamic loads are structural loads — and modern wing regulations date from those failures.

· TRY IT

Wings on, wings off: downforce vs speed

Set the speed and the wing angle and watch the air press the car down. The readout turns that downforce into what a driver feels: cornering grip and corner speed up, a little top speed sacrificed to drag — the trade every race engineer has haggled over since 1968.

01002003000125250375500speed (km/h)downforce (kg)no wings (1967)188 kg pressing down

Readout

Downforce at 200 km/h188 kg
Effective grip1.74 g
Fast-sweeper corner speed178 km/h
… gain over wingless+12 km/h
Top speed252 km/h
… cost of the wings45 km/h

Downforce squares with speed, so the grip arrives exactly where the fast corners are. Trading a little straight-line speed for a lot of cornering speed is why lap times fell off a cliff in 1968 — and why the trade has been the centre of race engineering ever since.

Lotus 49, 2 of 7