Section 1 of 9Forces on a falling object
Two forces act on an object falling through air or another fluid: its weight W = mg downwards, and the fluid's drag (air resistance) upwards. Drag increases as the speed rises, and also depends on the shape and cross-sectional area of the object.
Section 2 of 9The stages of a skydive
- The resultant force (weight − drag) gets smaller, so acceleration decreases, although the speed is still rising.
- The resultant force is zero, so acceleration is zero and the speed is constant.
- This steady speed is the terminal velocity.
At terminal velocity the air pushes up with a force exactly equal to the weight.
- and the air pushing back; the faster the object moves, the more air it must push aside each second,
- so the drag increases.
- where the time to fall between two marks on the tube gives the terminal speed.
Section 3 of 9Speed–time graph
The graph starts at the origin with a steep gradient (acceleration g).
Compare a skydiver in a spread-eagled position with the same skydiver in a head-down position.
- so drag at a given speed is smaller and terminal velocity is greater, roughly 55 m/s compared with 90 m/s or more.
Section 4 of 9What affects terminal velocity
The same ideas apply to a ball bearing falling through oil, where terminal velocity is reached in a short distance.
Reading the graph
- if the line is straight and steep at the start, the acceleration is about 9.8 m/s2.
- If the gradient has become zero, the object has reached terminal velocity.
- The distance fallen between two times is the area under the graph, which can be estimated by counting squares.
Section 5 of 9Cars and cyclists
A car also has a top speed at which driving force equals total drag. Streamlined designs reduce drag, allowing higher speed or less fuel use at the same speed.
Section 6 of 9Common description for exams
Always say that weight is equal and opposite to drag, that the resultant force is zero, and that the object moves at constant velocity. Mentioning that acceleration is zero but the object is still moving is the key point.
Remember that drag does not push upwards because of gravity; it opposes the motion, so it acts upwards only because the object is moving down. For a rising object, drag acts downwards. A ball thrown upwards therefore decelerates by more than g on the way up and by less than g on the way down.
Section 7 of 9Worked examples
A skydiver of mass 75 kg reaches terminal velocity. Find the drag force (g = 9.8 N/kg).
At terminal velocity drag = weight = mg = 75 × 9.8 = 735 N.
A 60 kg parachutist has drag of 400 N at one moment. Find the acceleration and its direction (g = 9.8 N/kg).
Weight = 60 × 9.8 = 588 N. Resultant = 588 − 400 = 188 N downwards.
a = 188 / 60 = 3.1 m/s2 downwards.
After opening the parachute the drag is 1800 N on a skydiver of weight 800 N, total mass 82 kg. Find the acceleration.
Resultant = 1800 − 800 = 1000 N upwards.
a = 1000 / 82 = 12 m/s2 upwards (a deceleration).
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Drag | Frictional force from air or liquid opposing motion. |
| Terminal velocity | Constant speed when drag equals weight. |
| Resultant force | Net force on an object. |
| Streamlined | Shaped to reduce drag. |
| Cross-sectional area | Area facing the oncoming fluid. |
Section 9 of 9Exam technique
Constant Acceleration Equations (SUVAT) & Slopes
v = u + at | s = ut + ½at2 | v2 = u2 + 2as | s = ½(u + v)t
- Displacement-Time Graph: Gradient = Velocity (curve = accelerating).
- Velocity-Time Graph: Gradient = Acceleration; Area under curve = Distance travelled / Displacement.
- Free Fall in vacuum:
a = g ≈ 9.81 m/s2downwards (air resistance negligible).