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How do forces produce acceleration, and how do you analyse the forces on a particle including friction and connected systems?

Newton's three laws of motion, weight, resolving forces, equilibrium of a particle, friction and the coefficient of friction, motion on an inclined plane, and connected particles.

A focused answer to the OCR A-Level Mathematics A forces content, covering Newton's three laws, weight, resolving forces, equilibrium of a particle, friction and the coefficient of friction, motion on an inclined plane, and connected particles over a pulley.

Generated by Claude Opus 4.812 min answer

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

OCR wants you to apply Newton's three laws, use weight W=mgW = mg, resolve forces into perpendicular components, set up the equilibrium conditions for a particle, model friction with FμRF \le \mu R (and F=μRF = \mu R when moving or on the point of moving), analyse motion on an inclined plane, and solve connected-particle problems such as masses over a pulley.

The answer

Newton's laws

Weight and resolving

Weight is the downward force W=mgW = mg. When a force acts at an angle, resolve it into perpendicular components, usually horizontal and vertical, or along and perpendicular to a slope.

Equilibrium of a particle

A particle is in equilibrium when the resultant force is zero, so the components balance in every direction. Resolving in two perpendicular directions and setting each sum to zero gives the equations.

Friction

Friction opposes motion (or attempted motion) along a surface, up to a maximum.

Examples in context

Newton's second law with friction

The standard method is: resolve perpendicular to the motion to find RR, compute friction μR\mu R, then apply F=maF = ma along the motion.

Motion on an inclined plane

On a slope, resolve along and perpendicular to the surface. The weight contributes mgsinθmg\sin\theta down the slope and mgcosθmg\cos\theta into it (so R=mgcosθR = mg\cos\theta for a particle on the slope with no other perpendicular force).

Connected particles

For two masses connected by a light inextensible string over a smooth pulley, the tension is the same throughout and both share one acceleration. Write Newton's second law for each mass and add the equations to eliminate the tension.

Try this

Q1. A 22 kg mass sits on a rough surface with μ=0.3\mu = 0.3. Find the maximum friction force (g=9.8g = 9.8). [2 marks]

  • Cue. R=2×9.8=19.6R = 2 \times 9.8 = 19.6 N, so Fmax=0.3×19.6=5.88F_{\max} = 0.3 \times 19.6 = 5.88 N.

Q2. A 55 kg block on a smooth slope inclined at 2020^\circ is released. Find its acceleration (g=9.8g = 9.8). [2 marks]

  • Cue. a=gsin20=9.8×0.3423.35a = g\sin 20^\circ = 9.8 \times 0.342 \approx 3.35 m s2^{-2}.

Exam-style practice questions

Practice questions written in the style of OCR exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

OCR 20196 marksA block of mass 55 kg rests on a rough horizontal plane with coefficient of friction 0.250.25. A horizontal force PP is applied. Find the value of PP that produces an acceleration of 22 m s2^{-2}. Take g=9.8g = 9.8 m s2^{-2}.
Show worked answer →

Resolve vertically: the normal reaction R=mg=5×9.8=49R = mg = 5 \times 9.8 = 49 N (M1, A1).

The friction force is F=μR=0.25×49=12.25F = \mu R = 0.25 \times 49 = 12.25 N (M1).

Newton's second law horizontally: PF=maP - F = ma (M1), so P12.25=5×2=10P - 12.25 = 5 \times 2 = 10 (A1).

Therefore P=10+12.25=22.25P = 10 + 12.25 = 22.25 N (A1).

Markers reward the vertical resolution for RR, the friction value, the horizontal equation of motion, and the final force.

OCR 20217 marksTwo particles of mass 22 kg and 66 kg are connected by a light inextensible string passing over a smooth pulley. The system is released from rest. Find the acceleration and the tension in the string. Take g=9.8g = 9.8 m s2^{-2}.
Show worked answer →

The 66 kg mass descends and the 22 kg mass rises with common acceleration aa and tension TT (B1).

For the 66 kg mass (down positive): 6gT=6a6g - T = 6a (M1). For the 22 kg mass (up positive): T2g=2aT - 2g = 2a (M1).

Add to eliminate TT (M1): 6g2g=8a6g - 2g = 8a, so 4g=8a4g = 8a and a=4×9.88=4.9a = \dfrac{4 \times 9.8}{8} = 4.9 m s2^{-2} (A1).

Substitute back: T=2g+2a=2(9.8)+2(4.9)=19.6+9.8=29.4T = 2g + 2a = 2(9.8) + 2(4.9) = 19.6 + 9.8 = 29.4 N (M1, A1).

Markers reward two equations of motion, eliminating TT, the acceleration, and the tension.

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