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Newton's laws of motion · Subtopic 2 of 4

Motion on Inclined Planes

Gravity pulls along the slope with mgsin⁡αmg\sin\alpha; friction, if any, opposes the motion with μmgcos⁡α\mu mg\cos\alpha. Put them into F=maF=ma along the slope, then let suvat finish the job.

Cambridge 9709 Paper 4Edexcel 9MA0 Paper 3AQA 7357 Paper 2≈ 35 minRevision 5 · updated 2026-10-27
Section 1 of 14

Learning objectives

  • Write F=maF=ma along an inclined plane, with RR from resolving perpendicular to it.
  • Find accelerations up and down smooth and rough slopes.
  • Find μ\mu from a measured acceleration.
  • Combine slope dynamics with suvat, including a particle projected up a slope.
Pause and think

A block slides down a rough slope. Then it is pushed up the same slope with the same speed and allowed to slow down. Is the size of its acceleration the same both ways?

Section 2 of 14

Core idea

Start hereSledging

A sledge slides down a snowy hill. Steeper hills give bigger accelerations; rougher snow slows it. Combine "weight along the slope" with friction and F=maF=ma to predict exactly how fast.

The big idea

Along the slope: (forces down) − (forces up) =ma=ma. Perpendicular: no acceleration, so forces balance, giving RR. On a smooth slope a=gsin⁡αa=g\sin\alpha.

1. Sliding down

Forces on a block on a 30° slope (sliding down)
W = mgRFmg sin αmg cos αα
Split the weight into two parts: mgsin⁡αmg\sin\alpha pulling down the slope and mgcos⁡αmg\cos\alpha pushing into it. Friction acts up the slope, opposing the motion (or the tendency to move).
Worked example2 kg on 30∘30^\circ, μ=0.25\mu=0.25

Find the acceleration down the slope.

Goal
aa.
Strategy
RR then friction then F=maF=ma.
  1. R=20cos⁡30∘=17.32R=20\cos30^\circ=17.32
    Perpendicular.
  2. F=0.25×17.32=4.33F=0.25\times17.32=4.33
    Sliding.
  3. 20sin⁡30∘−4.33=2a⇒a=2.8320\sin30^\circ-4.33=2a\Rightarrow a=2.83
    Along.
Answer2.832.83 m s−2^{-2}.
✓ CheckLess than the smooth-slope value 55 ✓.
Acceleration down a smooth slope as the angle grows
204060802468100angle α (degrees)a (m/s²)a = g sin α30°: 5 m/s²
Flat (0∘0^\circ): no acceleration. Vertical (90∘90^\circ): free fall at 1010 m/s². Friction reduces these values.

2. Projected up

Worked exampleProjected up at 8 m/s

Same slope. How far up, and does it slide back?

Goal
Distance; yes/no.
Strategy
Friction now acts down the slope too.
  1. 10+4.33=2a⇒a=7.17 (deceleration)10+4.33=2a\Rightarrow a=7.17\text{ (deceleration)}
    Both forces down the slope.
  2. 0=64−2(7.17)s⇒s=4.470=64-2(7.17)s\Rightarrow s=4.47
    v2=u2+2asv^2=u^2+2as.
  3. 10>4.3310>4.33
    Down-slope pull beats max friction: slides back.
Answer4.474.47 m; yes.
✓ CheckUp deceleration (7.177.17) > down acceleration (2.832.83): friction always opposes motion ✓.
Common misconceptionFriction direction Friction flips when the motion reverses.
Pause and think

Smooth 20∘20^\circ slope acceleration?

Summary

  • Perpendicular for RR; along for mama.
  • Friction opposes current motion.
Key words
Resolve
Find a component.
HistoryDiluting gravity. Galileo's ramps worked because a smooth slope "dilutes" gravity: a ball rolling down accelerates at gsin⁡αg\sin\alpha instead of gg. With a gentle slope he could slow free fall down enough to time it with water dripping from a tank, and so discovered the laws of falling bodies.
Fun factSkis are almost frictionless. Waxed skis on snow have μ\mu as low as about 0.050.05, because a thin film of melted water forms under them. On a 20∘20^\circ slope that gives an acceleration of 10(sin⁡20∘−0.05cos⁡20∘)≈2.9 m s−210(\sin20^\circ-0.05\cos20^\circ)\approx2.9\ \text{m s}^{-2}, almost as much as a smooth slope. Air resistance is what really limits a skier's speed.
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