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Friction and inclined planes notes and lesson for A Level physics (free PDF download)

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Friction and inclined planes notes and lesson for A Level physics (free PDF download)

This physics grades 11-12 lesson on friction and inclined planes notes gives the key ideas first, then worked examples and diagrams. After that, practise with the worksheet on friction and inclined planes and check yourself with the quiz.

Quick answer: Newton’s second law states that the resultant force equals mass times acceleration, ΣF = ma. Friction opposes sliding with f = μN, and on a slope of angle θ the normal reaction is mg cos θ while mg sin θ pulls the object down the slope. For connected bodies the acceleration is shared and the tension links the equations.

Level: Physics grades 11-12 (A Level · IB · Class 11-12) · Curriculum: IB A.2

Friction and inclined planes notes: the key ideas

What does Newton’s second law say?

The resultant force on an object equals its mass multiplied by its acceleration. In symbols, ΣF = ma. The resultant is found by adding all the forces as vectors, so friction, tension, weight and the normal reaction must all be included with their directions.

Formula

ΣF = ma. ΣF is the resultant force in newtons (N), m is mass in kilograms (kg) and a is acceleration in m/s². Weight W = mg with g = 9.81 N/kg.

How does friction work?

Friction is a contact force that opposes the relative motion, or the tendency to move, between two surfaces. Static friction can adjust itself up to a limit. Once the object slides, the friction has a nearly constant value.

Definition

The coefficient of friction μ is the ratio of the friction force to the normal reaction force N. For sliding, f = μk N. For the largest value before sliding starts, fmax = μs N. Static friction is at most μs N.

Pair of surfacesTypical μComment
Rubber tyre on dry road0.7 to 0.9good grip
Wood on wood0.3 to 0.5depends on roughness
Steel on steel, dryabout 0.5varies with polish
Ice on iceabout 0.03very slippery
A crate on a rough floor pushed to the right with 180 newtons, with friction of 137 newtons to the left, weight 392 newtons down and normal reaction 392 newtons up40 kgpush 180 NN = 392 NW = 392 Nfriction 137 N
A crate pushed along a rough floor. N equals mg on a level surface.
Worked example 1

A 40 kg crate is pushed with 180 N along a floor with μk = 0.35. N = mg = 40 × 9.81 = 392 N. Friction f = 0.35 × 392 = 137 N. Resultant = 180 − 137 = 43 N. a = 43 ÷ 40 = 1.07 m/s² in the direction of the push.

How do you analyse motion on a slope?

On a slope of angle θ the weight mg is split into a component mg sin θ pulling the object down the slope and a component mg cos θ pressing it into the surface. The normal reaction balances the second component, so N = mg cos θ, which is smaller than mg.

A block on a rough slope inclined at 30 degrees with arrows for weight mg downward, normal reaction N perpendicular to the slope, friction f up the slope, and the weight components mg sin theta along the slope and mg cos theta into the slopeblockmgNfmg sin θmg cos θθ = 30°
Forces on a block sliding down a slope.
Worked example 2

A 5.0 kg box slides down a 30° slope with μk = 0.20. Down the slope: mg sin θ = 5.0 × 9.81 × 0.500 = 24.5 N. N = 5.0 × 9.81 × 0.866 = 42.5 N and f = 0.20 × 42.5 = 8.5 N. Resultant = 24.5 − 8.5 = 16.0 N, so a = 16.0 ÷ 5.0 = 3.2 m/s². Mass cancels: a = g(sin θ − μ cos θ).

How do you treat connected bodies?

If two bodies are joined by a taut string, they have the same acceleration. Write ΣF = ma for each body separately, then solve the two equations together. The tension in the string is the same throughout a light string over a smooth pulley.

A 2.0 kilogram trolley on a table connected by a string over a pulley at the table edge to a 0.50 kilogram mass hanging below, with tension T in the string2.0 kg0.50 kgTWT
A trolley pulled by a hanging mass over a pulley.
Worked example 3

The 2.0 kg trolley and the 0.50 kg hanging mass are on a smooth table. For the whole system: 0.50 × 9.81 = (2.0 + 0.50) × a, so a = 4.905 ÷ 2.5 = 1.96 m/s². For the trolley: T = 2.0 × 1.962 = 3.92 N, which is less than the weight of the hanging mass.

Common mistake

Students write N = mg on a slope and put friction as μmg. The normal reaction is mg cos θ, so friction is μmg cos θ. Also, friction opposes the motion; it does not always act backwards, it acts against the sliding direction.

Lina’s tip

Draw the free-body diagram first and choose axes along and perpendicular to the slope. Write one equation for each axis, and the algebra almost solves itself.

Key points to remember
  • ΣF = ma; weight W = mg, g = 9.81 N/kg
  • Friction f ≤ μN, sliding f = μk N
  • On a slope: N = mg cos θ, driving force mg sin θ
  • Slope acceleration: a = g(sin θ − μk cos θ)
  • Connected bodies share the acceleration; tension links the equations

Forces, friction and motion on slopes: frequently asked questions

What is the difference between static and kinetic friction?

Static friction acts when there is no sliding and can take any value up to a maximum of μs N. Kinetic friction acts when the surfaces slide and is roughly constant at μk N. Normally μs is slightly larger than μk.

Why is the normal reaction smaller on a slope?

Only the component of the weight perpendicular to the surface, mg cos θ, presses the object into the slope. The surface balances this component. The component along the slope, mg sin θ, does not press on the surface.

Does mass affect how fast an object slides down a slope?

For a given slope and coefficient of friction, no. Both the driving force and the friction are proportional to mass, so mass cancels: a = g(sin θ − μ cos θ). Heavy and light objects accelerate equally.

How do you find the tension in a string joining two bodies?

First find the acceleration of the whole system. Then apply ΣF = ma to one body only, including the tension as the unknown force. The tension is the same at both ends of a light string over a smooth pulley.

How can you measure the coefficient of static friction with a slope?

Raise one end of a board until the block just starts to slide. At that angle μs = tan θ, because the friction limit equals the component of weight along the slope. The mass of the block is not needed.

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