A-level Mathematics

16.7 Friction and the F <= mu R model — Practise with help

Work each one first, closed book. Find the normal reaction before you find any limit. Compare the driving force with μR\mu R, then decide whether the body stays at rest or slides. Take g=9.8g = 9.8 m s−2^{-2}.

Warm-up: remember

  1. Work out 0.4×419.40.4 \times 419.4.
  2. Find the component of a weight of 441441 N acting down a slope of 18∘18^\circ.
  3. Which is larger, 136.3136.3 or 167.8167.8?
Answers
  1. 0.4×419.4=167.760.4 \times 419.4 = 167.76.
  2. 441sin⁡18∘≈136.3441\sin 18^\circ \approx 136.3 N.
  3. 167.8167.8 is larger.

If question 2 was hard, revise resolving a weight on a slope in Section 16.5 before you continue.

Practise with help

1. A block of mass 88 kg rests on a rough horizontal floor. The coefficient of friction is 0.50.5. A horizontal push of 3030 N is applied. Find the friction force.

Hint

Find the normal reaction and the limit μR\mu R first.

Next step

R=8×9.8=78.4R = 8 \times 9.8 = 78.4 N, so μR=0.5×78.4=39.2\mu R = 0.5 \times 78.4 = 39.2 N. Compare the push with the limit.

Full working

The push of 3030 N is below the limit of 39.239.2 N, so the block stays at rest. Static friction matches the push:

F=30 NF = 30 \text{ N}

backwards.

2. The same block is pushed with 5050 N instead. Find the friction force and the acceleration.

Hint

The limit is unchanged at 39.239.2 N. Compare the new push with it.

Next step

Since 50>39.250 > 39.2, the block slides and friction takes its greatest value. Subtract the friction from the push, then divide by the mass.

Full working F=μR=39.2 N,F = \mu R = 39.2 \text{ N}, a=50−39.28=10.88=1.35 m s−2.a = \frac{50 - 39.2}{8} = \frac{10.8}{8} = 1.35 \text{ m s}^{-2}.

3. A block of mass 1010 kg is released on a rough slope of 20∘20^\circ. The coefficient of friction is 0.60.6. Show that the block stays at rest, and find the friction force.

Hint

On a slope the normal reaction is mgcos⁡θmg\cos\theta, not mgmg.

Next step

The weight is 9898 N. The downhill component is 98sin⁡20∘=33.5298\sin 20^\circ = 33.52 N and the limit is 0.6×98cos⁡20∘=55.250.6 \times 98\cos 20^\circ = 55.25 N.

Full working

The downhill component, 33.5233.52 N, is below the limit of 55.2555.25 N, so the block stays at rest. Friction matches the downhill component:

F=33.52 NF = 33.52 \text{ N}

up the slope.

4. A block of mass 66 kg is released on a rough slope of 35∘35^\circ. The coefficient of friction is 0.40.4. Show that the block slides, and find its acceleration.

Hint

Compare the downhill component with the limit. If the component is larger, the block slides.

Next step

The weight is 58.858.8 N. Downhill: 58.8sin⁡35∘=33.7358.8\sin 35^\circ = 33.73 N. Limit: 0.4×58.8cos⁡35∘=19.270.4 \times 58.8\cos 35^\circ = 19.27 N. The block slides, so friction is 19.2719.27 N.

Full working a=33.73−19.276=14.466≈2.41 m s−2a = \frac{33.73 - 19.27}{6} = \frac{14.46}{6} \approx 2.41 \text{ m s}^{-2}

down the slope.

5. A block on a rough slope of 25∘25^\circ is in limiting equilibrium. Find the coefficient of friction.

Hint

At limiting equilibrium the downhill component equals the greatest friction.

Next step

Write mgsin⁡25∘=μ mgcos⁡25∘mg\sin 25^\circ = \mu\,mg\cos 25^\circ, then divide.

Full working μ=tan⁡25∘≈0.466.\mu = \tan 25^\circ \approx 0.466.

The mass cancels, so the answer does not depend on the mass.

6. A block of mass 1515 kg rests on a rough horizontal floor. The coefficient of friction is 0.350.35. Find the smallest horizontal force that will start the block moving.

Hint

The block starts to move when the push reaches the limiting friction.

Next step

R=15×9.8=147R = 15 \times 9.8 = 147 N, and the limiting friction is 0.35×1470.35 \times 147.

Full working Fmin⁡=μR=0.35×147=51.45 N.F_{\min} = \mu R = 0.35 \times 147 = 51.45 \text{ N}.

7. A block of mass 1010 kg is pulled along a rough horizontal floor by a rope at 30∘30^\circ to the horizontal with a tension of 6060 N. The coefficient of friction is 0.40.4. Find the normal reaction and the acceleration.

Hint

The rope has an upward component, so the normal reaction is less than the weight.

Next step

R=98−60sin⁡30∘=68R = 98 - 60\sin 30^\circ = 68 N, so the limit is 0.4×68=27.20.4 \times 68 = 27.2 N. The horizontal pull is 60cos⁡30∘=51.9660\cos 30^\circ = 51.96 N, which beats the limit.

Full working R=98−30=68 N,F=0.4×68=27.2 N.R = 98 - 30 = 68 \text{ N}, \qquad F = 0.4 \times 68 = 27.2 \text{ N}. a=51.96−27.210=24.7610≈2.48 m s−2.a = \frac{51.96 - 27.2}{10} = \frac{24.76}{10} \approx 2.48 \text{ m s}^{-2}.

8. A block of mass 2020 kg on a rough horizontal floor is just on the point of moving when a horizontal force of 5050 N is applied. Find the coefficient of friction.

Hint

At the point of moving, the push equals the limiting friction.

Next step

R=20×9.8=196R = 20 \times 9.8 = 196 N and 50=μ×19650 = \mu \times 196.

Full working μ=50196≈0.255.\mu = \frac{50}{196} \approx 0.255.

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