Worked Example · Calculus · Paper 2 · 7 marks
Kinematics: Total Distance from a Velocity Function
Written by Rig, our founder
8 years teaching IGCSE & SPM maths · Updated 16 August 2026
The examiner’s trap in kinematics is the phrase “total distance”. The particle reverses direction partway through, so integrating velocity straight across the interval gives displacement, and understates the distance. You must find where it turns and add the legs separately.
A particle moves in a straight line so that, at time seconds after passing a fixed point , its velocity is . (i) Find the times at which the particle is instantaneously at rest. [2] (ii) Find the total distance travelled in the first seconds. [5]
The working
(i) “At rest” means :
The particle is momentarily at rest at and , so it changes direction at .
(ii) Displacement is the integral of velocity:
Evaluate the position at the key times:
The particle moves from to (first s), then back from to (next s). Add the two legs as distances:
Note the displacement over the s is , the particle ends where it started, which is exactly why “distance” and “displacement” give different answers here.
Where the marks are won and lost
- Part (i) is not decoration: the rest times are the split points for part (ii). Skipping them almost guarantees the distance error.
- Integrating from to in one go gives . A student who writes “distance m” has computed displacement and lost three marks.
- Each leg’s contribution is a modulus. The backward leg is as a signed displacement but as a distance.
Common mistakes
- Reporting the displacement ( m) as the distance.
- Forgetting the constant of integration reasoning ( at ).
- Splitting at the wrong time, the turning point is where , i.e. inside the interval (the endpoint is the interval’s end).
Full method: Kinematics notes. Topic home: Calculus pillar.