A flat plain gives the impression of aerodynamic calm, yet a low supercar there is primed to hit the ground harder than gravity ever could. Its body is shaped as a set of inverted wings, so at speed the airflow over and under the shell creates a pressure differential that pushes the chassis downward instead of lifting it into the air.
The strange part is that the car does not need a ramp or banking; it weaponises the air itself. As air meets the nose, splitters and ducts manage the stagnation point, then accelerate flow under the floor; Bernoulli’s principle says faster flow means lower static pressure, so the region beneath the car becomes a moving low‑pressure zone sucking it toward the asphalt.
More dramatic still is ground effect, the same aerodynamic principle that once reshaped racing. A low ride height turns the gap between floor and road into a narrowing channel; this Venturi tunnel geometry speeds the air, drops pressure further, and multiplies downforce with every rise in velocity, until the vertical load can exceed the car’s own mass and make it feel bolted to the surface.