Know that friction (drag) acts on an object moving through a gas (air resistance) – and also through a liquid – and understand the factors that influence its magnitude.
Drag is a type of friction that occurs when a solid object moves through a fluid – either a gas (air) or a liquid (water, oil). It always opposes the motion, but unlike surface friction it does not depend on a normal reaction.
Typical IGCSE examples: sky‑diver falling, paper parachute, falling ball.
Typical IGCSE examples: swimmer moving through water, boat cruising on a lake, stone dropped into oil. Because liquids are much denser than air, the drag forces are considerably larger for the same speed and area.
| Factor (syllabus order) | How it influences drag | Typical IGCSE example |
|---|---|---|
| Speed of the object (v) | At low speeds drag ≈ k v (linear). At higher speeds drag ≈ ½ Cd ρ A v² (quadratic). Drag therefore rises rapidly with speed. | A sky‑diver accelerates until the upward drag equals his weight (terminal velocity). |
| Cross‑sectional area (A) | Larger area presents more fluid to push aside, giving a larger drag force. | A flat sheet of paper falls slower than a rolled‑up sheet of the same mass. |
| Shape (drag coefficient Cd) | Streamlined shapes have low Cd → less drag; blunt shapes have high Cd → more drag. | Airplane wings are shaped to minimise drag. |
| Density of the fluid (ρ) | Denser fluids exert a larger drag for the same speed and area. | Moving through water (ρ≈1000 kg m⁻³) feels much more resistance than moving through air (ρ≈1.2 kg m⁻³). |
| Viscosity of the fluid | Viscosity is the internal “thickness” of a fluid; higher viscosity gives a greater frictional component of drag, especially at low speeds. | A stone falls more slowly in honey than in water. |
Two approximations are used in the syllabus, each appropriate for a different speed regime.
$$F_{d}=k\,v$$
k is a constant that depends on the object's shape, area and the fluid’s properties. This form is valid for very slow motion (e.g. a gently falling feather).
$$F_{d}= \frac{1}{2}\,C_{d}\,\rho\,A\,v^{2}$$
This form is used for objects such as sky‑divers, projectiles, or cars moving quickly through air.
| Aspect | Surface (solid) friction | Drag (air or fluid resistance) |
|---|---|---|
| Medium | Two solid surfaces in contact | Solid object moving through a fluid (gas or liquid) |
| Direction | Opposes relative motion of the surfaces | Opposes the motion of the object through the fluid |
| Dependence on speed | Largely independent of speed (kinetic friction) | Strongly dependent on speed (linear at low v, quadratic at high v) |
| Dependence on normal reaction | Proportional to normal force ( Ff=μN ) | Does **not** depend on a normal reaction |
| Other influencing factors | Nature of the two surfaces (roughness, material) | Cross‑sectional area, shape (Cd), fluid density, viscosity |
| Typical observable effect | Heating of the contact surfaces | Energy loss from the moving object (slower fall, reduced range) |
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