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M9.1bLadders, tilting and limiting equilibrium

Edexcel A level Maths (9MA0) · Mechanics › Moments

Practise Ladders, tilting and limiting equilibrium. 3 exam-style questions plus unlimited generated ones on this subtopic, at up to four difficulty levels, with full mark schemes and a progress tracker. Free, no account needed.

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Sample questions

Written for this site in the style of Edexcel exam questions. They are not taken from real past papers.

Question 1Easy8 marks
A ladder \(AB\), of length 5 m and mass 25 kg, rests in equilibrium with its end \(A\) on rough horizontal ground and its end \(B\) against a smooth vertical wall. The ladder makes an angle \(\theta\) with the ground, where \(\tan \theta = \frac{12}{5}\), and lies in a vertical plane perpendicular to the wall. The ladder is modelled as a uniform rod.
Take \(g = 9.8\) m s−2. Give any answer that uses this value of \(g\) to 2 or 3 significant figures.
[object Object]
(a) Find the magnitude of the reaction of the wall on the ladder.[3]
(b) Find the magnitude of the frictional force exerted by the ground on the ladder.[2]
(c) Find the magnitude of the normal reaction of the ground on the ladder.[1]
(d) Show that the coefficient of friction between the ladder and the ground is at least \(\frac{5}{24}\).[2]
Show the answer and mark scheme
(a) Answer: 51.0 N (accept 51 N) N
  • M1 for taking moments about \(A\) with the correct terms
  • A1 for \(S \times 5\sin\theta = 25g \times 2.5\cos\theta\)
  • A1 for 51.0 or 51 (N) or \(\frac{125}{24}g\)

Worked solution: Moments about \(A\): \(S \times 5\sin\theta = 25g \times 2.5\cos\theta\), so \(S = \frac{25g}{2\tan\theta} = \frac{125}{24}g = 51.0\) N.

(b) Answer: 51.0 N (accept 51 N) N
  • M1 for resolving horizontally: \(F = S\)
  • A1ft for 51.0 or 51 (N)

Worked solution: Resolving horizontally: \(F = S = 51.0\) N.

(c) Answer: 245 N (accept 250 N) N
  • B1 for \(R = 25g\) = 245 or 250 (N)

Worked solution: Resolving vertically: \(R = 25g = 245\) N.

(d) Answer: \(F \leqslant \mu R \Rightarrow \mu \geqslant \frac{F}{R} = \frac{5}{24}\)
  • M1 for using \(F \leqslant \mu R\) with their \(F\) and \(R\)
  • A1* for \(\mu \geqslant \frac{5}{24}\)

Worked solution: \(F \leqslant \mu R\) gives \(\mu \geqslant \frac{F}{R} = \frac{\frac{125}{24}g}{25g} = \frac{5}{24}\).

Question 2Medium9 marks
A ladder of length 5 m and mass 12 kg rests with its foot on rough horizontal ground and its top against a smooth vertical wall. The ladder makes an angle of \(65^\circ\) with the ground and is on the point of slipping. The ladder is modelled as a uniform rod, and it lies in a vertical plane perpendicular to the wall.
Take \(g = 9.8\) m s−2. Give any answer that uses this value of \(g\) to 2 or 3 significant figures.
[object Object]
(a) Find the magnitude of the reaction of the wall on the ladder.[3]
(b) Find the coefficient of friction between the ladder and the ground, giving your answer to 3 significant figures.[3]
(c) Explain how you have used the modelling assumption that the ladder is uniform.[1]
(d) In reality the ladder is not uniform: it is heavier near its foot. State, with a reason, whether the true value of the coefficient of friction needed would be greater or smaller than your answer to part (b).[2]
Show the answer and mark scheme
(a) Answer: 27.4 N (accept 27 N) N
  • M1 for moments about the foot of the ladder
  • A1 for \(S \times 5\sin 65^\circ = 12g \times 2.5\cos 65^\circ\)
  • A1 for 27.4 or 27 (N)

Worked solution: \(S = \frac{12g \times 2.5\cos 65^\circ}{5\sin 65^\circ} = 6g\cot 65^\circ = 27.4\) N (3 s.f.)

(b) Answer: \(\mu = 0.233\)
  • M1 for \(F = S\) and \(R = 12g\)
  • M1 for \(F = \mu R\)
  • A1 for awrt 0.233

Worked solution: \(\mu = \frac{F}{R} = \frac{6g\cot 65^\circ}{12g} = \frac{1}{2\tan 65^\circ} = 0.233\) (3 s.f.).

(c) Answer: The weight of the ladder acts at its midpoint, 2.5 m from each end.
  • B1 for the weight acts at the midpoint of the ladder

Worked solution: A uniform ladder has its centre of mass at its midpoint, so its weight acts 2.5 m from the foot.

(d) Answer: Smaller: the centre of mass is nearer the foot, so the moment of the weight about the foot is smaller, the wall reaction is smaller and less friction is needed.
  • B1 for smaller
  • B1 for the weight acts closer to the foot, reducing its moment about the foot and hence the reaction at the wall and the friction required

Worked solution: If the centre of mass is lower, \(S \times 5\sin 65^\circ = 12g \times d\cos 65^\circ\) with \(d \lt 2.5\), so \(S\), and hence the friction required, is smaller.

Question 3Hard9 marks
A uniform ladder \(AB\), of length 6 m and mass 15 kg, rests with its end \(A\) on rough horizontal ground and its end \(B\) against a smooth vertical wall. The ladder makes an angle \(\theta\) with the ground, where \(\tan\theta = 3\), and lies in a vertical plane perpendicular to the wall. A decorator needs to put a pot of paint of mass 5 kg on the ladder, either at \(A\) or at \(B\). The pot of paint is modelled as a particle.
Take \(g = 9.8\) m s−2. Give any answer that uses this value of \(g\) to 2 or 3 significant figures.
[object Object]
(a) Find the least coefficient of friction between the ladder and the ground needed for equilibrium when the pot is at \(A\).[4]
(b) Find the least coefficient of friction needed when the pot is at \(B\).[3]
(c) The coefficient of friction between the ladder and the ground is 0.15. Advise the decorator where to place the pot of paint, giving a reason.[2]
Show the answer and mark scheme
(a) Answer: \(\mu = \frac{1}{8} = 0.125\)
  • M1 for moments about \(A\) (the pot at \(A\) has no moment): \(S \times 6\sin\theta = 15g \times 3\cos\theta\)
  • A1 for \(S = \frac{15g}{6} = 2.5g\) (using \(\tan\theta = 3\))
  • M1 for \(\mu \geqslant \frac{F}{R} = \frac{S}{20g}\)
  • A1 for \(\frac{1}{8}\)

Worked solution: Moments about \(A\): \(6S\sin\theta = 45g\cos\theta\), so \(S = \frac{45g}{6\tan\theta} = 2.5g\). With the pot at \(A\), \(R = 20g\) and \(F = S\), so \(\mu \geqslant \frac{2.5g}{20g} = \frac{1}{8}\).

(b) Answer: \(\mu = \frac{5}{24} \approx 0.208\)
  • M1 for moments about \(A\) including the pot: \(6S\sin\theta = 15g \times 3\cos\theta + 5g \times 6\cos\theta\)
  • A1 for \(S = \frac{75g}{18} = \frac{25g}{6}\)
  • A1 for \(\mu \geqslant \frac{25g/6}{20g} = \frac{5}{24}\)

Worked solution: \(6S \times 3 = 45g + 30g\) (dividing by \(\cos\theta\)), so \(S = \frac{75g}{18} = \frac{25g}{6}\). \(R = 20g\), so \(\mu \geqslant \frac{25}{120} = \frac{5}{24}\).

(c) Answer: At \(A\) (the foot): 0.15 exceeds the \(\frac{1}{8}\) needed, but is less than the \(\frac{5}{24}\) needed with the pot at \(B\), so with the pot at \(B\) the ladder would slip.
  • M1 for comparing 0.15 with both of their values
  • A1 for place it at \(A\), since \(0.125 \lt 0.15 \lt 0.208\) (the ladder would slip if the pot were at \(B\))

Worked solution: Only the arrangement with the pot at the foot needs \(\mu \leqslant 0.15\): \(\frac{1}{8} = 0.125 \lt 0.15\), whereas \(\frac{5}{24} \approx 0.208 \gt 0.15\). So the pot should be placed at \(A\).

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