Cambridge International AS & A Level · Topic 4.4
A-Level Maths 9709 / Topic 4.4 / AS & A Level

Down the slope, then up.

On a slope, resolve along and perpendicular to the plane. The weight splits into \(mg\sin\alpha\) down the slope and \(mg\cos\alpha\) into it, and on a rough plane friction always points against the motion, so going up and coming down give different accelerations.

The key idea

Along the plane: resultant force \(= ma\). Perpendicular: \(R = mg\cos\alpha\) (plus or minus any other perpendicular components). Moving up a rough plane, friction acts down it, so \(mg\sin\alpha + \mu R\) slows the particle; moving down, friction acts up, so the driving force is \(mg\sin\alpha - \mu R\).

α R F = μR 20 N motion sin α = 0.6 cos α = 0.8 μ = 0.25
Fig. 1: a 2 kg particle moving UP a rough plane with sin α = 0.6 (α = 36.9°, drawn to scale). Friction acts down the plane, against the motion
Section 01

Smooth slopes.

On a smooth plane the only force along the slope is the weight component \(mg\sin\alpha\), so \(a = g\sin\alpha\) down the plane whichever way the particle is moving. The mass cancels.

Worked example Released on a smooth plane
A particle is released from rest on a smooth plane inclined at \(30^\circ\) to the horizontal. Find its speed after it has slid 4 m and the time taken.
  1. Down the plane: \(mg\sin 30^\circ = ma\), so \(a = 10 \times 0.5 = 5\ \text{m s}^{-2}\).
  2. \(v^2 = 0 + 2(5)(4) = 40\), so \(v = 6.32\ \text{m s}^{-1}\).
  3. \(t = \dfrac{v}{a} = \dfrac{6.325}{5} = 1.26\) s.
Answer: \(6.32\ \text{m s}^{-1}\) after 1.26 s.
Examiner trap

\(a = g\sin\alpha\), not \(g\cos\alpha\). Check with a limiting case: on a vertical "slope" (\(\alpha = 90^\circ\)) the particle falls freely with \(a = g\), and \(\sin 90^\circ = 1\).

Section 02

Rough slopes: up and down differ.

Friction always opposes the motion. A particle sliding down has friction up the plane; a particle moving up has friction down the plane, adding to the weight component. That is why the syllabus expects different accelerations for the two directions.

Worked example Sliding down
A particle of mass 2 kg slides down a rough plane inclined at \(\alpha\) to the horizontal, where \(\sin\alpha = 0.6\). The coefficient of friction is 0.25. Find its acceleration.
  1. Perpendicular: \(R = 20\cos\alpha = 20 \times 0.8 = 16\) N; friction \(= 0.25 \times 16 = 4\) N up the plane.
  2. Down the plane: \(20\sin\alpha - 4 = 2a\).
  3. \(12 - 4 = 8 = 2a\).
Answer: \(a = 4\ \text{m s}^{-2}\) down the plane.
Worked example Projected up the plane (Fig. 1)
The same particle is projected up the plane from point A at \(10\ \text{m s}^{-1}\). Find how far up the plane it travels, and its speed when it returns to A.
  1. Moving up, friction acts down: \(-(12 + 4) = 2a\), so \(a = -8\ \text{m s}^{-2}\).
  2. \(0 = 100 - 16s\), so \(s = 6.25\) m.
  3. At rest, the weight component (12 N) exceeds the maximum friction (4 N), so it slides back with \(a = 4\ \text{m s}^{-2}\) (previous example).
  4. \(v^2 = 0 + 2(4)(6.25) = 50\), so \(v = 7.07\ \text{m s}^{-1}\).
Answer: 6.25 m; it returns at \(7.07\ \text{m s}^{-1}\), slower than it set off because friction did work both ways.
Your turn
A particle slides from rest down a rough plane inclined at \(25^\circ\) and reaches \(3\ \text{m s}^{-1}\) after travelling 3 m. Find the coefficient of friction.
Examiner trap

After a particle stops at the top, do not assume it slides back. Compare the weight component \(mg\sin\alpha\) with the maximum friction \(\mu mg\cos\alpha\): it stays put if \(\mu \ge \tan\alpha\).

Stage 1 · Learn

Check your understanding

Four quick checks. Each correct answer earns XP and records this skill on your profile.

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A particle slides down a smooth plane inclined at \(30^\circ\). What is its acceleration?

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A 4 kg particle rests on a plane inclined at \(30^\circ\), with no other forces perpendicular to the plane. Find the normal reaction.

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A particle is projected up a rough plane. Which way does friction act while it moves up?

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A particle comes to rest on a rough plane inclined at \(\alpha\). When will it stay at rest?

Section 03

Extra forces on the slope.

With a pulling force, resolve it too. A force parallel to the plane leaves \(R = mg\cos\alpha\); a force at an angle to the plane changes \(R\), and so changes the friction.

Worked example Pulled up the plane
A particle of mass 5 kg is pulled up a rough plane inclined at \(20^\circ\) by a force of 50 N parallel to the plane. The coefficient of friction is 0.3. Find the acceleration.
  1. \(R = 50\cos 20^\circ = 46.98\) N, so friction \(= 0.3 \times 46.98 = 14.10\) N down the plane.
  2. Up the plane: \(50 - 50\sin 20^\circ - 14.10 = 5a\).
  3. \(50 - 17.10 - 14.10 = 18.80 = 5a\).
Answer: \(a = 3.76\ \text{m s}^{-2}\)
Worked example A horizontal push
A particle of mass 3 kg is pushed up a rough plane inclined at \(30^\circ\) by a horizontal force of 40 N. The coefficient of friction is 0.2. Find its acceleration.
  1. The horizontal force makes \(30^\circ\) with the plane and pushes into it.
  2. Perpendicular: \(R = 30\cos 30^\circ + 40\sin 30^\circ = 25.98 + 20 = 45.98\) N; friction \(= 9.196\) N.
  3. Up the plane: \(40\cos 30^\circ - 30\sin 30^\circ - 9.196 = 3a\).
  4. \(34.64 - 15 - 9.196 = 10.44 = 3a\).
Answer: \(a = 3.48\ \text{m s}^{-2}\)
Examiner trap

Using \(R = mg\cos\alpha\) when the applied force has a component perpendicular to the plane. In the second example that gives friction 5.20 N instead of 9.20 N.

Stage 2 · Exam

Exam-style questions

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A 2 kg particle slides down a rough plane with \(\sin\alpha = 0.6\) and \(\mu = 0.25\). Find its acceleration.

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The particle is instead projected up the same plane at \(10\ \text{m s}^{-1}\). How far up the plane does it travel?

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It then slides back down. Find its speed when it returns to its starting point.

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A 5 kg particle is pulled up a rough plane inclined at \(20^\circ\) (\(\mu = 0.3\)) by a force of 50 N parallel to the plane. Find the acceleration.

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Go deeper · practice
Six original Cambridge-style questions
A smooth slope, sliding down a rough one, finding mu from the motion, a particle that stops and stays, a horizontal push, and a skier with air resistance.