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Stopping Distance Under Friction Braking

A car travelling at 25 m/s25\ \text{m/s} brakes to a complete stop. The coefficient of friction between the tyres and the road is μ=0.70\mu = 0.70, and the wheels do not lock.

Take g=9.81 m/s2g = 9.81\ \text{m/s}^2.

Find the minimum stopping distance.

Given
v025 m/sInitial speed
μ0.7 -Coefficient of friction
Hint 1

Find the deceleration first. What force is doing the stopping?

Hint 2

Friction force is μmg, so a = μg — the mass cancels out entirely.

Hint 3

With no time given, use v² = v₀² − 2ad.

Worked solution — try the problem first

Deceleration from friction. The friction force is μmg\mu mg, so by Newton's second law:

ma=μmga=μgma = \mu m g \quad \Longrightarrow \quad a = \mu g

The mass cancels — stopping distance does not depend on how heavy the car is. That is worth internalising; it surprises people.

a=0.70×9.81=6.867 m/s2a = 0.70 \times 9.81 = 6.867\ \text{m/s}^2

Kinematics (no time given, so use the velocity-displacement relation):

v2=v022ad0=2522(6.867)dv^2 = v_0^2 - 2ad \quad \Longrightarrow \quad 0 = 25^2 - 2(6.867)d

d=62513.734=45.5 md = \frac{625}{13.734} = 45.5\ \text{m}

d=45.5 m\boxed{d = 45.5\ \text{m}}

Equivalent energy argument: the kinetic energy 12mv02\tfrac12 mv_0^2 is dissipated by friction work μmgd\mu mgd; cancelling mm gives d=v02/(2μg)d = v_0^2/(2\mu g), the same result.

Concepts:Newton's second lawFrictionKinematicsWork-energy theorem

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