Revision Notes
OCR A Level Mathematics A: Newton's laws, weight and equilibrium in one dimension (H240) – Revision Notes
Condensed revision notes on forces, Newton's laws, weight, normal reaction and straight-line equilibrium for OCR A Level Mathematics A (H240).
- Subject
- Mathematics
- Level
- A LEVELS
- Topic
- Newton's laws, weight and equilibrium in one dimension
- Author
- Marlbridge Academic Team
- Updated
Aligned to OCR A Level Mathematics (H240), Version 3.1 (August 2026), for first assessment in 2018. Official specification .
Syllabus page (what it covers and how it is assessed): OCR A Level Mathematics.
Syllabus points this page covers
H240
- 3.03 Forces and Newton's laws
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These notes condense OCR A Level Mathematics A (H240) specification section 3.03, items 3.03a to 3.03k (Version 3.1, August 2026, first assessment 2018), with 3.03e marked A Level only. For full explanations use the study guide. Then test yourself with the practice questions. Course hub: OCR A Level Mathematics. Printable checklist. Free 10-minute diagnostics. Connected particles, pulleys, two-dimensional equilibrium and friction are in separate units.
Key facts
| Idea | Statement | Ref |
|---|---|---|
| Force | Vector, in newtons; 1 N = 1 kg m s⁻² | 3.03a |
| First law | Constant velocity (or rest) means zero resultant force | 3.03b |
| Second law | Resultant F = ma, same direction as a | 3.03c |
| Vector form | F = ma on vectors, component by component | 3.03d |
| Resolved form | Use F cos θ and F sin θ along and across the motion | 3.03e (A Level only) |
| Weight | W = mg, down; g = 9.8 m s⁻² may be assumed | 3.03f, g |
| Third law | Equal and opposite forces on two different bodies | 3.03h |
| Normal reaction | Perpendicular to the surface; R = 0 means contact is lost | 3.03i |
| Smooth | No friction, so only a normal contact force | 3.03j |
| Light, inextensible string | Same tension along it; same speed and acceleration at both ends | 3.03j |
| Equilibrium | Zero resultant, so zero acceleration | 3.03k |
Method for any straight-line problem
- Draw a force diagram for one body only. Mark every force on it.
- Choose a positive direction, usually the direction of the acceleration.
- Write F = ma along that line, giving each force its sign.
- Write a separate equation across the line if a normal reaction is needed.
- Solve, then use constant-acceleration formulas if time, speed or distance is asked.
- Check the sign and size of the answer: tensions and reactions must not be negative.
Worked reminders
Lift, passenger of mass 25 kg, accelerating up at 0.4 m s⁻²:
R − 25 × 9.8 = 25 × 0.4
R = 245 + 10 = 255 N
The same passenger with the lift accelerating down at 0.4: R = 25(9.8 − 0.4) = 235 N. At constant speed R = 245 N, which is the weight.
Hoist, load of mass 6 kg on a light inextensible cable:
Accelerating up at 0.5: T − 58.8 = 6 × 0.5, so T = 61.8 N
Constant velocity: T = 58.8 N
Decelerating at 0.5 (still rising): 58.8 − T = 6 × 0.5, so T = 55.8 N
Speeding up while rising and slowing down while falling both need T above the weight. Slowing while rising and speeding up while falling need T below it. Check which way the acceleration points before you write the equation.
Falling with resistance: a 2 kg stone falls from rest with constant resistance of 3 N.
2 × 9.8 − 3 = 2a, so a = 8.3 m s⁻²
After 4 s: v = 8.3 × 4 = 33.2 m s⁻¹, distance = ½ × 8.3 × 4² = 66.4 m
Link the second law to the constant-acceleration formulas: v = u + at, then v² = u² + 2as, s = ½(u + v)t, or s = ut + ½at², whichever fits the data.
Vector form: a 2 kg particle with acceleration 3i + 1.5j has resultant 6i + 3j N. Components are independent, so you can also solve i and j parts separately.
Resolved (A Level only): a force P at θ above the horizontal on a smooth horizontal surface gives P cos θ = ma and R + P sin θ = mg. Contact is lost when P sin θ = mg.
Smooth slope (A Level only): the acceleration down a smooth plane at angle θ is g sin θ, and R = mg cos θ.
Must-know distinctions
| Pair | Difference |
|---|---|
| Mass and weight | Mass (kg) is fixed. Weight (N) is mg, so it follows g |
| Third-law pair and balanced pair | A third-law pair acts on two bodies and can never be balanced. Balanced forces such as weight and R act on one body |
| R = mg and R | R equals mg only when there is no vertical acceleration. In a lift R changes with a |
| Light and smooth | Light describes a string, with no mass. Smooth describes a surface, with no friction |
| Inextensible and light | Inextensible gives equal accelerations at both ends. Light gives equal tension throughout |
| Constant velocity and constant acceleration | Constant velocity means F = 0. Constant acceleration means F is constant and non-zero |
About g: its value varies with place, which is why weight changes from one planet to another while mass does not. Use the value in the question, normally 9.8.
When R becomes 0: the surface no longer pushes and the body leaves it. In a lift this happens when the downward acceleration reaches g. For a pulled body on a smooth surface it happens when the upward component of the pull equals the weight.
When a string goes slack: T = 0. If a string is cut, the tension disappears at once, but velocity does not change at that instant.
Modelling words and what they allow
| Word in the question | What you may assume |
|---|---|
| Particle | Size and rotation are ignored, so all forces act at one point |
| Light | Negligible mass, so equal tension throughout a single string |
| Inextensible | Length is fixed, so connected ends share speed and acceleration |
| Smooth | No friction, so the contact force is normal to the surface |
| Constant force | Constant acceleration, so the constant-acceleration formulas apply |
| Air resistance negligible | Weight is the only force on a falling body, so a = g |
Quick checks before you finish
- Units: forces in N, masses in kg, accelerations in m s⁻². A mass of 450 g is 0.45 kg.
- Direction: say “upwards” or “downwards” when you quote a force or acceleration, or give the sign you chose.
- Sense check: a lift accelerating upwards needs T greater than the weight; in free fall the floor force is zero; a falling body with resistance has a less than 9.8.
- Method: if the question gives time or distance, expect to use a constant-acceleration formula either before or after the second law.
- Vectors: a resultant such as (5i + 20j) + (7i − 4j) is found by adding components, then divide by the mass for the acceleration. The magnitude is √(x² + y²).
- Accuracy: carry unrounded values through the working and give 3 significant figures at the last step, unless the question says otherwise.
Quick self-test
Use g = 9.8 m s⁻².
- Find the weight of an 8 kg body.
- A resultant force of 30 N acts on a 6 kg trolley. Find its acceleration.
- Forces of 20 N and 8 N act in opposite directions on a 5 kg block on a smooth horizontal surface. Find its acceleration.
- Find the force on a 2 kg particle with acceleration (3i + 1.5j) m s⁻².
- A 1000 kg lift rises at constant speed. Find the cable tension.
- The lift floor supports a 50 kg cleaner while the lift accelerates upwards at 2 m s⁻². Find the force the floor exerts on the cleaner.
- State the third-law partner of the gravitational pull of the Earth on a book.
- A 0.5 kg ball falls with constant air resistance of 1.1 N. Find its acceleration.
- A 10 N force acts at 60° above the horizontal on a 2 kg body on a smooth horizontal surface (A Level only). Find the horizontal acceleration.
- A 3 kg particle hangs at rest on a light inextensible string. Find the tension.
- State two assumptions in the term “light inextensible string”.
- What is the reaction on a passenger in a lift that is in free fall?
Answers
- 78.4 N
- 5 m s⁻²
- Resultant 12 N, so a = 12 ÷ 5 = 2.4 m s⁻²
- 6i + 3j N
- 9800 N
- R = 50(9.8 + 2) = 590 N
- The pull of the book on the Earth, equal in size and opposite in direction
- (0.5 × 9.8 − 1.1) ÷ 0.5 = 7.6 m s⁻²
- 10 cos 60° = 2a, so a = 2.5 m s⁻²
- T = 3 × 9.8 = 29.4 N
- The string has negligible mass, so tension is the same throughout; its length does not change, so both ends move together
- R = 0
Where marks are usually lost
- Forgetting the weight in a vertical equation, or including it in a horizontal one.
- Using R = mg for a body that is accelerating vertically.
- Mixing signs: adding a force that opposes the acceleration.
- Treating weight and R as a third-law pair.
- Using F = ma with F as a single force instead of the resultant.
- Answering with kg where newtons are needed, or leaving out units.
- Rounding g to 10 when the question says 9.8, which gives a different final answer.
- Using sin where cos is needed when resolving (A Level only).
- Omitting a short statement of the model when asked, such as light string or smooth surface.
- Leaving a negative tension or reaction without noticing that the situation cannot occur.
Official syllabus
OCR A Level Mathematics A (H240) specification, Version 3.1 (August 2026), first assessment 2018, published by OCR: section 3.03, Forces and Newton’s Laws.
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