Free fall in the kinematics unit assumed the air was not there. That assumption is excellent for a dropped stone over a short distance and hopeless for a parachutist, a leaf or a coffee filter. Putting the air back in needs no new equations — only one more arrow on the free-body diagram, and the willingness to think about what happens to the net force as the object speeds up.
Air resistance is a force that grows with speed
Air resistance, also called drag, is the force the air exerts on an object moving through it. It always points opposite to the object's motion, because it comes from the object having to shove air out of the way. The feature that makes it interesting is that it is not a fixed number: the faster you move, the more air you displace each second, so the harder the air pushes back. A cyclist feels almost nothing at walking pace and a wall of it at .
- Speed — the dominant factor. Doubling the speed of a car more than doubles the drag on it, which is why highway fuel economy is so much worse than city economy.
- Cross-sectional area — the frontal area facing the airflow. A skydiver spread flat has several times the drag of the same skydiver diving head-down.
- Shape — a streamlined teardrop lets the air close smoothly behind it; a flat plate leaves a turbulent wake that drags it back.
- Air density — thinner air at altitude means less drag, which is why aircraft cruise high and why records are set in mountain velodromes.
Reaching terminal velocity
| Stage of the fall | Weight | Air resistance | Net force | Acceleration |
|---|---|---|---|---|
| The instant of release | down | Zero — no speed yet | down | down, the full value |
| Speeding up | down | Growing, still less than | Downward but shrinking | Downward and decreasing |
| Terminal velocity | down | Exactly up | Zero | Zero — the speed stops changing |
Read that table as a story. The object leaves your hand with gravity alone acting, so it accelerates at the full . As it picks up speed the drag grows, the net force shrinks, and the acceleration shrinks with it — so the object is still speeding up, just less enthusiastically each moment. On a velocity-time graph this shows as a line that starts steep and bends over. Eventually the drag has grown to exactly equal the weight, the net force is zero, and by Newton's first law the velocity stops changing. That final constant speed is the terminal velocity, and the graph flattens into a horizontal line.
Opening a parachute changes one thing only — the area facing the airflow, by an enormous factor. The drag immediately becomes far larger than the weight, so the net force flips to point upward while the skydiver is still moving downward. Opposite signs on velocity and acceleration mean rapid slowing, which is the violent jolt of the opening. As the speed falls the drag falls with it, until the drag once again equals the weight and a new, much lower terminal velocity is reached — around , a survivable landing speed. The weight never changed; only the drag did.
Safety technology: the same stop, spread over more time
A collision is a very fast stop. The occupant of a car is travelling at the car's speed, and after the crash they are travelling at zero — that change in velocity is fixed by the physics of the situation and no safety device can alter it. What a safety device can alter is how long the change takes. Because the acceleration is the change in velocity divided by the time it takes, stretching the stopping time shrinks the acceleration, and Newton's second law then shrinks the force in exactly the same proportion.
| Technology | What it physically does | Why the force on the body falls |
|---|---|---|
| Crumple zone | The front structure folds progressively instead of stopping dead | The cabin takes around to stop instead of around |
| Airbag | Inflates so the head and chest decelerate against a deep, soft cushion | The occupant stops over tens of centimetres rather than against a rigid steering wheel |
| Seatbelt with a load limiter | Holds the occupant to the seat, then pays out webbing under very high load | The occupant decelerates with the car, over the car's whole stopping time |
| Cycling or hockey helmet | A crushable foam liner collapses under impact | The skull stops over the thickness of the liner instead of instantly against the ground |
| Gym mats and playground surfacing | Compress under a falling body | The fall is arrested over several centimetres instead of on bare concrete |
| Bending your knees when you land | Your legs fold instead of staying locked | Your torso stops over perhaps rather than on impact |
- Stopping time of a few hundredths of a second
- Very large acceleration, since is fixed
- Very large force on the body, from
- Little visible damage to the vehicle
- Severe injury to the occupants
- Stopping time stretched by a factor of five to ten
- Acceleration reduced by that same factor
- Force on the body reduced by that same factor
- The vehicle is visibly wrecked
- Occupants survive forces their bodies can tolerate