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M8.6

Understand and use the F ≤ μR model for friction; coefficient of friction; motion of a body on a rough surface; limiting friction and statics.

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Friction

Worked answers and methods for M8.6 on Edexcel A-level Maths 9MA0.

Definition

Specification M8.6: understand and use the F≤μRF\leq\mu R model for friction; coefficient of friction; motion of a body on a rough surface; limiting friction and statics.

Explanation

  • Friction acts along the surface, opposing the motion or the tendency to move, and satisfies F≤μRF\leq\mu R where RR is the normal reaction. Find RR first by resolving perpendicular to the surface; on a slope R=mgcos⁡αR=mg\cos\alpha, and an applied force with a vertical component changes RR.
  • Friction equals μR\mu R only when the body is moving or is in limiting equilibrium, on the point of moving; in ordinary equilibrium friction takes whatever value the other forces need, and the question is whether that value exceeds μR\mu R.
  • To decide whether a body on a slope stays at rest, compare the component of weight down the slope, mgsin⁡αmg\sin\alpha, with the maximum friction μmgcos⁡α\mu mg\cos\alpha and state the conclusion.
  • For a body in motion write F=μRF=\mu R and F=maF=ma along the surface, with friction opposite to the velocity, which reverses when the body slides back down.
  • A range of values for a force comes from the two limiting cases.
On a rough horizontal surface, friction opposes impending or actual motion and satisfies F≤μRF\leq\mu R.

Worked example

1.

A block of mass 66 kg is moving on a rough horizontal surface under the action of a horizontal force of magnitude 2020 N acting in the direction of motion. The coefficient of friction between the block and the surface is 0.250.25. Find the acceleration of the block.

(4)

(Total for Question 1 is 4 marks)

Working

  1. 1.Resolve vertically: R=6g=58.8R=6g=58.8 N.
  2. 2.The block is moving, so friction is limiting: F=μR=0.25×58.8=14.7F=\mu R=0.25\times58.8=14.7 N, acting against the motion.
  3. 3.Horizontally, F=maF=ma: 20−14.7=6a20-14.7=6a, so a=5.36=0.883a=\dfrac{5.3}{6}=0.883 m s−2^{-2}.

Answer: 0.880.88 m s−2^{-2} (2 s.f.)

Mark scheme

Mark scheme for question 1
QuestionSchemeMarks
1.R=6g=58.8R=6g=58.8 NB1
F=μRF=\mu R used: 0.25×0.25\times their RRM1
Equation of motion with the correct terms: 20−F=6a20-F=6aM1
a=0.88a=0.88 m s−2^{-2} or 0.8830.883A1
Notes
M1: Condone sign errors
A1: awrt 0.88

(4 marks)

Common mistakes

  • Don't reverse the direction of friction so that it assists the impending relative motion.
  • Don't set friction equal to the limiting value in every situation, even when equilibrium requires a smaller force.

Mark-scheme wording to use

  • “(2/7) × 4.9 oe seen … M1 (2/7) × their (a) (must be a numerical value) … 1.4, 1.40 or (1/7)g … A1” — Pearson 9MA0, June 2024 Paper 32, Q1(b)
  • “Equation of motion down the plane … M1 … mg sin α − F = ma or mg sin α − F = −ma … A1 … (F =) μ × their R … M1 … A1* Given answer correctly obtained, with at least one further line of working with both trig ratios substituted as fractions.” — Pearson 9MA0, June 2024 Paper 32, Q3(b)
  • “B1 for R = 3gcos(20) and hence maximum friction 0.9gcos(20). M1 for comparing or subtracting 3gsin(20) and 0.9gcos(20). A1* for the justified conclusion that the box starts to move down the plane” — Pearson 9MA0, Specimen Paper 32, Q3(c)

What the examiner wants

RR before FF, and μR\mu R only when friction is limiting. The June 2024 Paper 32 report says most found the limiting friction by multiplying their reaction by 27\frac27 and then realised the applied force had the same value, though some, seeing the word “magnitude”, squared or square-rooted a correct answer and lost the accuracy mark.

Exam tip

Decide whether friction is limiting; otherwise use the force balance to find its actual value within the inequality.

Worked practice

Q1
Tier 1 · Easy

1.

A block is in equilibrium on a rough horizontal surface. The normal reaction is 80 N80\,\text{N} and the coefficient of friction is 0.300.30. A horizontal force of 10 N10\,\text{N} acts on the block. Find the friction force and the greatest possible friction force.

(3)

(Total for Question 1 is 3 marks)

Mark scheme

Mark scheme for question 1
QuestionSchemeMarks
1
  • Friction =10 N=10\,\text{N} opposite to the applied force
  • Greatest possible friction =24 N=24\,\text{N}
3
Notes
Equilibrium requires friction to balance the 10 N10\,\text{N} applied force, so F=10 NF=10\,\text{N}. The limiting value is μR=0.30(80)=24 N\mu R=0.30(80)=24\,\text{N}; the actual friction is smaller because the block is not in limiting equilibrium.

(3 marks)

Q2
Tier 2 · Standard

2.

A 4 kg4\,\text{kg} block rests on a rough horizontal surface with coefficient of friction 0.300.30. A horizontal force PP is applied. Using g=9.8 m s−2g=9.8\,\text{m s}^{-2}, find the greatest value of PP for equilibrium and the friction force when P=10 NP=10\,\text{N}.

(4)

(Total for Question 2 is 4 marks)

Mark scheme

Mark scheme for question 2
QuestionSchemeMarks
2
  • Greatest P=11.76 NP=11.76\,\text{N}, or 11.8 N11.8\,\text{N} to 3 significant figures
  • When P=10 NP=10\,\text{N}, friction is 10 N10\,\text{N} opposite to PP.
4
Notes
The normal reaction is R=4g=39.2 NR=4g=39.2\,\text{N}, so the limiting friction is μR=0.30(39.2)=11.76 N\mu R=0.30(39.2)=11.76\,\text{N}. This is the greatest horizontal force that static friction can balance. When P=10 N<11.76 NP=10\,\text{N}<11.76\,\text{N}, friction adjusts to 10 N10\,\text{N}; it is not automatically equal to μR\mu R.

(4 marks)

Q3
Tier 3 · Hard

3.

A 10 kg10\,\text{kg} particle rests on a rough plane inclined at 20∘20^\circ to the horizontal. The coefficient of friction is 0.300.30. A force of magnitude P NP\,\text{N} acts up the plane. Using g=9.8 m s−2g=9.8\,\text{m s}^{-2}, find the complete range of values of PP for which the particle remains in equilibrium.

(7)

(Total for Question 3 is 7 marks)

Mark scheme

Mark scheme for question 3
QuestionSchemeMarks
3
  • 5.89≤P≤61.15.89\leq P\leq61.1
7
Notes
The normal reaction is R=98cos⁡20∘R=98\cos20^\circ, so limiting friction is μR=29.4cos⁡20∘\mu R=29.4\cos20^\circ. The component of weight down the plane is 98sin⁡20∘98\sin20^\circ. Equilibrium requires friction of magnitude ∣98sin⁡20∘−P∣|98\sin20^\circ-P|, so ∣98sin⁡20∘−P∣≤29.4cos⁡20∘|98\sin20^\circ-P|\leq29.4\cos20^\circ. Hence 98sin⁡20∘−29.4cos⁡20∘≤P≤98sin⁡20∘+29.4cos⁡20∘98\sin20^\circ-29.4\cos20^\circ\leq P\leq98\sin20^\circ+29.4\cos20^\circ, giving 5.89≤P≤61.15.89\leq P\leq61.1.

(7 marks)

Q4
Tier 1 · Easy

4.

A particle is in limiting equilibrium on a rough surface. The friction has magnitude 18 N18\,\text{N} and the normal reaction is 60 N60\,\text{N}. Find the coefficient of friction.

(2)

(Total for Question 4 is 2 marks)

Mark scheme

Mark scheme for question 4
QuestionSchemeMarks
4
  • 0.300.30
2
Notes
At limiting equilibrium F=μRF=\mu R, so 18=60μ18=60\mu and μ=0.30\mu=0.30.

(2 marks)

Q5
Tier 2 · Standard

5.

A 6 kg6\,\text{kg} block is on a rough horizontal surface. A force of 24 N24\,\text{N} acts at 45∘45^\circ above the horizontal and the block is on the point of moving in the horizontal direction of the force. Using g=9.8 m s−2g=9.8\,\text{m s}^{-2}, find the coefficient of friction, giving your answer to 3 significant figures.

(5)

(Total for Question 5 is 5 marks)

Mark scheme

Mark scheme for question 5
QuestionSchemeMarks
5
  • μ=0.406\mu=0.406
5
Notes
Vertical equilibrium gives R+24sin⁡45∘=6(9.8)R+24\sin45^\circ=6(9.8), so R=58.8−122 NR=58.8-12\sqrt2\,\text{N}. At limiting equilibrium the friction is μR\mu R and horizontal equilibrium gives μR=24cos⁡45∘=122\mu R=24\cos45^\circ=12\sqrt2. Hence μ=122/(58.8−122)=0.406\mu=12\sqrt2/(58.8-12\sqrt2)=0.406 to 3 significant figures.

(5 marks)

Q6
Tier 3 · Hard

6.

A 5 kg5\,\text{kg} block is in equilibrium on a rough horizontal surface with coefficient of friction 0.250.25. A horizontal force of 10 N10\,\text{N} acts to the left. A second force of magnitude P NP\,\text{N} acts upwards and to the right at an angle α\alpha above the horizontal, where tan⁡α=34\tan\alpha=\dfrac34. Given P≥0P\geq0 and using g=9.8 m s−2g=9.8\,\text{m s}^{-2}, find the complete range of values of PP for which equilibrium is possible. Give the upper bound to 3 significant figures.

(6)

(Total for Question 6 is 6 marks)

Mark scheme

Mark scheme for question 6
QuestionSchemeMarks
6
  • 0≤P≤44519 N0\leq P\leq\dfrac{445}{19}\,\text{N}, or 0≤P≤23.4 N0\leq P\leq23.4\,\text{N} to 3 significant figures
6
Notes
Since cos⁡α=4/5\cos\alpha=4/5 and sin⁡α=3/5\sin\alpha=3/5, vertical equilibrium gives R=49−3P/5R=49-3P/5. The friction required has magnitude ∣4P/5−10∣|4P/5-10|. Equilibrium is possible when ∣4P/5−10∣≤(1/4)(49−3P/5)|4P/5-10|\leq(1/4)(49-3P/5). The lower inequality gives P≥−45/13P\geq-45/13, which is replaced by the stated P≥0P\geq0. The upper inequality gives 4P/5−10≤49/4−3P/204P/5-10\leq49/4-3P/20, so 19P/20≤89/419P/20\leq89/4 and P≤445/19=23.4 NP\leq445/19=23.4\,\text{N} to 3 significant figures. This range also keeps R>0R>0.

(6 marks)

Q7
Tier 2 · Standard

7.

The angle α\alpha between a rough plane and the horizontal satisfies tan⁡α=34\tan\alpha=\dfrac34. A 4 kg4\,\text{kg} block slides down the plane and the coefficient of friction is 14\dfrac14. Model the block as a particle. Take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Find its acceleration down the plane.

(4)

(Total for Question 7 is 4 marks)

Mark scheme

Mark scheme for question 7
QuestionSchemeMarks
7
  • Acceleration =3.92 m s−2=3.92\,\text{m s}^{-2} down the plane
4
Notes
Since tan⁡α=3/4\tan\alpha=3/4, sin⁡α=3/5\sin\alpha=3/5 and cos⁡α=4/5\cos\alpha=4/5. The normal reaction is R=4g(4/5)R=4g(4/5), so the friction opposing the downward motion is μR=(1/4)4g(4/5)=4g/5 N\mu R=(1/4)4g(4/5)=4g/5\,\text{N}. Resolving down the plane, 4a=4g(3/5)−4g/5=8g/54a=4g(3/5)-4g/5=8g/5, hence a=2g/5=3.92 m s−2a=2g/5=3.92\,\text{m s}^{-2}.

(4 marks)

Q8
Tier 3 · Hard

8.

The angle α\alpha between a rough plane and the horizontal satisfies tan⁡α=34\tan\alpha=\dfrac34. A 5 kg5\,\text{kg} block moves up the plane while a horizontal force of 48 N48\,\text{N} acts towards the upward side. The coefficient of friction is 0.200.20. Model the block as a particle. Take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Find the normal reaction and the acceleration of the block. Given that its speed is initially 4 m s−14\,\text{m s}^{-1}, find its speed and direction of motion 3 s3\,\text{s} later.

(6)

(Total for Question 8 is 6 marks)

Mark scheme

Mark scheme for question 8
QuestionSchemeMarks
8
  • Normal reaction =68 N=68\,\text{N}
  • Acceleration =0.92 m s−2=0.92\,\text{m s}^{-2} down the plane
  • After 3 s3\,\text{s} the block moves up the plane at 1.24 m s−11.24\,\text{m s}^{-1}
6
Notes
Here sin⁡α=3/5\sin\alpha=3/5 and cos⁡α=4/5\cos\alpha=4/5. Perpendicular to the plane, the weight contributes 5g(4/5)=39.2 N5g(4/5)=39.2\,\text{N} into the plane and the horizontal force contributes 48(3/5)=28.8 N48(3/5)=28.8\,\text{N} into the plane, so R=68 NR=68\,\text{N}. Since the block moves up the plane, friction 0.20R=13.6 N0.20R=13.6\,\text{N} acts down the plane. Taking up the plane as positive, the resultant is 48(4/5)−5g(3/5)−13.6=38.4−29.4−13.6=−4.6 N48(4/5)-5g(3/5)-13.6=38.4-29.4-13.6=-4.6\,\text{N}. Thus a=−4.6/5=−0.92 m s−2a=-4.6/5=-0.92\,\text{m s}^{-2}. After 3 s3\,\text{s}, v=4−0.92(3)=1.24 m s−1v=4-0.92(3)=1.24\,\text{m s}^{-1}, which is still up the plane.

(6 marks)

Q9
Tier 3 · Hard

9.

An 8 kg8\,\text{kg} block slides on a rough horizontal plane. The only horizontal force is friction, modelled with coefficient μ\mu. The block has speed 10 m s−110\,\text{m s}^{-1} and comes to rest after travelling 25 m25\,\text{m}. Take g=9.8 m s−2g=9.8\,\text{m s}^{-2} and assume the friction model applies throughout. Find the exact value of μ\mu, the friction force and the time taken to stop. Give all numerical answers exactly.

(6)

(Total for Question 9 is 6 marks)

Mark scheme

Mark scheme for question 9
QuestionSchemeMarks
9
  • μ=1049\mu=\dfrac{10}{49}
  • Friction force =16 N=16\,\text{N} opposite to the motion
  • Stopping time =5 s=5\,\text{s}
6
Notes
Taking the direction of motion as positive, 0=102+2a(25)0=10^2+2a(25) gives a=−2 m s−2a=-2\,\text{m s}^{-2}. The friction magnitude is therefore m∣a∣=8(2)=16 Nm|a|=8(2)=16\,\text{N}. Vertically, R=8(9.8)=78.4 NR=8(9.8)=78.4\,\text{N}, so μ=F/R=16/78.4=10/49\mu=F/R=16/78.4=10/49. Finally 0=10−2t0=10-2t, giving t=5 st=5\,\text{s}.

(6 marks)

Q10
Tier 3 · Hard

10.

A 10 kg10\,\text{kg} block moves on a rough horizontal plane with acceleration 0.8 m s−20.8\,\text{m s}^{-2} to the right. The coefficient of friction is 1/41/4. A force of magnitude P NP\,\text{N} acts downwards and to the right at an angle α\alpha below the horizontal, where tan⁡α=3/4\tan\alpha=3/4. Model the block as a particle, assume the friction model applies and take g=9.8 m s−2g=9.8\,\text{m s}^{-2}. Find the exact values of PP, the normal reaction and the friction force. Give all numerical answers exactly.

(6)

(Total for Question 10 is 6 marks)

Mark scheme

Mark scheme for question 10
QuestionSchemeMarks
10
  • P=50 NP=50\,\text{N}
  • Normal reaction =128 N=128\,\text{N}
  • Friction force =32 N=32\,\text{N} to the left
6
Notes
Here cos⁡α=4/5\cos\alpha=4/5 and sin⁡α=3/5\sin\alpha=3/5. Vertical equilibrium gives R=98+3P/5R=98+3P/5, so friction is R/4R/4. Resolving horizontally to the right, 4P/5−(98+3P/5)/4=10(0.8)4P/5-(98+3P/5)/4=10(0.8). Thus 13P/20−24.5=813P/20-24.5=8, so 13P/20=32.513P/20=32.5 and P=50 NP=50\,\text{N}. Hence R=98+30=128 NR=98+30=128\,\text{N} and friction is 128/4=32 N128/4=32\,\text{N} to the left.

(6 marks)

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