🪂 Parachute Physics — Terminal Velocity & Drag
Jump from altitude, freefall to terminal velocity, then deploy the canopy and watch the drag spike. Adjust mass, parachute diameter, and deployment altitude to explore the aerodynamics of deceleration.
Parameters
Telemetry
F = mg − ½ρCdAv²
ρ(h) = 1.225·e−h/8500 kg/m³
Cd(freefall) = 1.0 · Abody=0.6 m²
Cd(canopy) = 1.5 · Acanopy=π(d/2)²
How Parachute Drag Works
During freefall, the drag force on a human body is Fdrag = ½ρCdAv², where ρ is air density (decreasing exponentially with altitude), Cd ≈ 1.0 for a prone human, and A ≈ 0.6 m². Terminal velocity is reached when drag equals gravity: vt = √(2mg / ρCdA). At sea level this is roughly 55 m/s (200 km/h) for a prone skydiver. When the canopy deploys, A jumps to π(d/2)² — a huge increase — and the drag spikes dramatically, causing strong deceleration. The safe landing speed is typically < 6 m/s. Air density follows the barometric formula ρ(h) = ρ0·e−h/8500.