Velocity is the derivative of displacement, and acceleration is the derivative of velocity. Integration reverses these relationships: integrating acceleration gives velocity, while integrating velocity gives displacement.
This is part of IB Mathematics: Analysis and Approaches, SL 5.9: Kinematics problems, and may be examined on Paper 1 or Paper 2.
The relationships
Let represent displacement, velocity, and acceleration at time .
| Operation | Relationship | Meaning |
|---|---|---|
| Differentiate displacement | Velocity is the rate of change of displacement. | |
| Differentiate velocity |
Suppose
Differentiating gives
and differentiating again gives
At , , so the particle is moving in the negative direction. Also, , which means the velocity has a stationary value at that instant; it does not mean the particle is stationary. A particle is stationary only when . Here, solving gives and . These times are the turning points of the displacement-time graph.
In reverse, integrating acceleration gives . An initial condition such as is required to determine . Indefinite integration produces a family of functions, so the constant cannot be omitted.
The sign of velocity shows direction: means displacement is increasing, while means it is decreasing. However, means velocity is increasing, not necessarily that the particle is moving forward.
Graphically, the gradient of a displacement-time graph is velocity, while the gradient of a velocity-time graph is acceleration. The signed area under a velocity-time graph gives displacement.
A common misconception is that integrating velocity always gives distance. It gives displacement:
Total distance requires speed:
Exam technique
Show the derivative or integral before giving a value. For total distance, find every time when , split the interval at sign changes, and integrate (|v(t)|). Do not report signed displacement as distance.
