Revision Notes
OCR A Level Physics A: Dynamics, free-body diagrams, drag and terminal velocity (H556) – Revision Notes
Condensed notes on F = ma, weight, contact forces, free-body diagrams, drag and terminal velocity for OCR A Level Physics A (H556), with a self-test.
- Subject
- Physics
- Level
- A LEVELS
- Topic
- Dynamics, free-body diagrams, drag and terminal velocity
- Author
- Marlbridge Academic Team
- Updated
Aligned to OCR A Level Physics (H556), Version 3.0 (March 2026), for first assessment in 2017. Official specification .
Syllabus page (what it covers and how it is assessed): OCR A Level Physics.
Syllabus points this page covers
H556
- 3.2 Forces in action
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Quick recall for OCR A Level Physics A (H556), sections 3.2.1 Dynamics and 3.2.2 Motion with non-uniform acceleration (specification Version 3.0, March 2026). For full explanations and worked examples, read the study guide. Then test yourself with the practice questions. Hub: OCR A Level Physics. Tick off topics on the printable checklist, and find weak spots with the free 10-minute diagnostics. Vector resolving is revised in Foundations of Physics.
Key equations and definitions
| Item | Statement | Spec |
|---|---|---|
| Newton’s second law as used here | net force = mass × acceleration, F = ma | 3.2.1(a) |
| The newton | Net force producing 1 m s⁻² in a 1 kg mass; 1 N = 1 kg m s⁻² | 3.2.1(b) |
| Weight | W = mg, with g = 9.81 N kg⁻¹ near Earth’s surface | 3.2.1(c) |
| Resolving a force | Fx = F cos θ, Fy = F sin θ (θ measured from x) | 3.2.1(f) |
| Slope, weight components | Along slope mg sin θ; perpendicular mg cos θ | 3.2.1(f) |
| Drag | Frictional force on an object moving through a fluid | 3.2.2(a) |
| Terminal velocity | Constant velocity when the resultant force is zero | 3.2.2(d) |
Recall F = ma and W = mg from memory. The specification expects it.
The four named forces
| Force | Direction | Typical mistake |
|---|---|---|
| Tension | Along the rope or cable, away from the object | Drawing it for a string that is slack |
| Normal contact force | Perpendicular to the surface | Drawing it vertical on a slope |
| Upthrust | Up, from the fluid | Leaving it out for a ball in a liquid |
| Friction | Parallel to the surface, against the relative motion | Drawing it in the direction of motion |
Free-body diagram checklist
- One object only, as a dot or box.
- Arrows start on the object and show forces on it.
- Every force is named: weight, tension, normal contact force, upthrust, friction, drag, applied force.
- Equal and opposite forces are drawn equal in length.
- No arrows for velocity, acceleration or a “force of motion”.
- Resolve on a slope along and perpendicular to the surface.
Method: any constant-force problem
- Draw the free-body diagram.
- Choose a positive direction (or two perpendicular axes).
- Resolve any force at an angle.
- Write net force = ma in each direction.
- Use constant-acceleration equations for speed, time or distance.
- Check units and significant figures.
Dynamics reminders
- Tension in a lift cable moving up with acceleration a: T = m(g + a). With constant speed, T = mg. For deceleration while moving up, T = m(g − a).
- A block on a slope with friction F: net force down the slope = mg sin θ − F.
- Projectile (no drag): horizontal velocity constant, vertical acceleration g. Treat each direction separately.
- A force perpendicular to the motion changes the direction of travel, not the component of speed along the original direction.
Worked reminders
Horizontal pull with friction. A 5.0 kg box is pulled by a horizontal 20 N force against friction of 8.0 N. Net force = 20 − 8.0 = 12 N, so a = 12/5.0 = 2.4 m s⁻².
Smooth slope. A 3.0 kg trolley is on a frictionless slope at 30°. Only the down-slope component of weight gives a net force. a = g sin 30° = 9.81 × 0.50 = 4.9 m s⁻², and the mass cancels.
Projectile. A ball rolls off a table 0.80 m high at 8.0 m s⁻¹ (ignore drag). t = √(2 × 0.80/9.81) = 0.40 s, so the horizontal distance is 8.0 × 0.404 = 3.2 m.
Falling with drag. A 0.10 kg object falls with a drag of 0.40 N at that instant. a = (0.10 × 9.81 − 0.40)/0.10 = 5.8 m s⁻² downward.
Terminal velocity in liquid. A 2.0 g marble falls through oil with upthrust 3.0 mN. Weight = 2.0 × 10⁻³ × 9.81 = 19.6 mN, so drag at terminal velocity = 19.6 − 3.0 = 16.6 mN, about 17 mN.
A 4.5 kg trolley with net force 12 N has a = 12/4.5 = 2.7 m s⁻².
Drag
- Acts opposite to the velocity relative to the fluid.
- In air, drag increases with speed, cross-sectional area, less streamlined shape and air density.
- Always say which factor and in which direction. “More area, so more air pushed aside, so more drag” earns more than “air resistance”.
Falling with drag: three stages
| Stage | Drag | Net force | Acceleration |
|---|---|---|---|
| Release | About zero | Weight | g |
| Speeding up | Rising | Falling | Falling (graph gets shallower) |
| Terminal velocity | Equals weight (air) | Zero | Zero (graph is horizontal) |
In a liquid: weight = drag + upthrust at terminal velocity. If drag changes (parachute opens): drag > weight, so the object decelerates; drag falls with speed until it again equals weight at a lower terminal velocity.
Graphs for a fall with drag
- Velocity–time: starts at zero with gradient g, curves over with a decreasing gradient, then becomes horizontal at the terminal velocity.
- Acceleration–time: starts at g and decreases to zero.
- Distance–time: starts flat, steepens, then becomes a straight line whose gradient is the terminal velocity.
Template for “explain terminal velocity”
- Weight acts down; drag (and upthrust, in a liquid) acts up.
- Speed increases, so drag increases.
- The net force decreases, so the acceleration decreases.
- Drag (plus upthrust) equals weight, so the net force is zero and the velocity is constant.
Determining terminal velocity (PAG1 examples)
| Technique | Key points |
|---|---|
| Ball bearing in viscous liquid | Tall cylinder; equal marked intervals well below the surface; micrometer for diameter; time each interval by video or light gates; speed constant means terminal velocity reached; drop along the axis; repeat and average |
| Cones in air | Fixed release height of at least 2 m; time the last stretch; stack cases to change weight; no draughts; repeat |
Graph check: a distance–time graph that becomes a straight line shows constant speed. The gradient of that straight section is the terminal velocity.
Must-know distinctions
- Mass (kg, scalar) versus weight (N, vector).
- Net force versus any single force.
- Balanced forces (constant velocity, possibly moving) versus no forces.
- Terminal velocity in air (weight = drag) versus in liquid (weight = drag + upthrust).
Quick self-test
- A 0.40 kg trolley accelerates at 3.5 m s⁻². What net force acts on it?
- Find the weight of a 65 kg student, using g = 9.81 N kg⁻¹.
- Find the mass of an object that weighs 49 N.
- A force of 50 N acts at 40° above the horizontal. Find its horizontal and vertical components.
- A lift of mass 640 kg moves upward at a steady speed. State the tension in the cable.
- State the direction of the normal contact force on a block resting on a slope.
- A parachutist of weight 710 N falls at terminal velocity. State the drag force.
- A paper cone of mass 1.2 g falls at terminal velocity in air. Find the drag on it.
- Explain why the acceleration of a falling ball falls as its speed rises.
- State two precautions when timing a ball bearing falling in oil.
Answers
- F = ma = 0.40 × 3.5 = 1.4 N.
- W = 65 × 9.81 = 638 N.
- m = W/g = 49/9.81 = 5.0 kg.
- Horizontal 50 cos 40° = 38 N; vertical 50 sin 40° = 32 N.
- Constant speed means zero net force, so T = mg = 640 × 9.81 = 6.3 kN.
- Perpendicular to the slope, away from the surface.
- 710 N, upward, because the net force is zero.
- W = 1.2 × 10⁻³ × 9.81 = 0.012 N, so drag is 0.012 N.
- Drag increases with speed, so net force (weight minus drag) falls, so acceleration falls.
- Any two: drop along the cylinder axis; wait until the ball is moving at constant speed before timing; use video or light gates instead of a stopwatch; keep the temperature steady; repeat and average.
Where marks are usually lost
- Quoting weight in kg, or mass in N.
- Writing “gravity” for weight, or “friction” for drag in a liquid, when the question wants the named force.
- Forgetting upthrust in a liquid.
- Putting the normal contact force vertical on a slope.
- Using g for the acceleration of a falling object when drag is acting.
- Saying “the forces cancel” for an accelerating object.
- Not stating the direction when a quantity is a vector.
- Giving a terminal velocity from a single timed run with no check that the speed had stopped changing.
- Giving terminal velocity as the point where drag is zero.
- Rounding in the middle of a calculation, then losing a significant figure.
- Describing an experiment without saying how to know that terminal velocity has been reached.
Official syllabus
OCR A Level Physics A (H556) specification, Version 3.0 (March 2026), for first assessment in 2017, published by OCR. Sections 3.2.1 and 3.2.2.
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