The Intuition: Why a Falling Object Stops Accelerating
Drop a steel ball bearing into a jar of honey. You expect it to fall, but it doesn't crash down like it would in air. Instead, it sinks slowly and steadily, at a constant speed, almost from the moment you let go. That constant speed is the terminal velocity.
Why does it happen? Two forces are at work. Gravity pulls the ball down. But the honey resists its motion — that's viscous drag. At the start, the ball is moving slowly, so the drag is small. Gravity wins, and the ball accelerates. But as speed increases, drag grows. Eventually, drag becomes exactly as strong as the net downward pull (weight minus buoyancy). At that point, the net force is zero. No net force means no acceleration — the ball continues at whatever speed it has reached. That speed is terminal velocity.
Terminal velocity is not a limit you approach from above. You reach it from below, as acceleration dies out.
The Precise Statement
For a small, smooth sphere falling through a viscous fluid at low speeds (so the flow is laminar, not turbulent), the drag force is given by Stokes' law:
Fdrag=6πηrv
where η is the fluid's viscosity, r is the sphere's radius, and v is its speed.
The other forces are:
- Weight downward: W=34πr3ρg (where ρ is the sphere's density)
- Buoyant force upward: Fb=34πr3σg (where σ is the fluid's density)
The net downward force (weight minus buoyancy) is:
Fnet=34πr3(ρ−σ)g
At terminal velocity, drag equals this net downward force:
6πηrvt=34πr3(ρ−σ)g
Solve for vt:
vt=9η2r2(ρ−σ)g
vt=9η2r2(ρ−σ)g
What the Formula Tells You
- Radius squared — a larger sphere falls much faster. Double the radius, quadruple the terminal speed.
- Density difference — if the sphere is only slightly denser than the fluid, it falls slowly. If it's lighter than the fluid (ρ<σ), vt becomes negative — it rises.
- Viscosity — thicker fluids (higher η) give a lower terminal speed. Honey stops a ball far more than water does.
This formula only holds for laminar flow (low Reynolds number). For a fast-falling sphere in a low-viscosity fluid like air, turbulence sets in and Stokes' law breaks down. Then terminal velocity follows a different law involving the square root of size, not the square.
A Concrete Example …