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How do differentiation and integration move between displacement, velocity and acceleration?

Differentiate to pass from displacement to velocity to acceleration, and integrate to reverse the process, fixing constants from initial conditions

A focused answer to the O-Level A-Maths outcome on calculus in kinematics. Differentiating displacement to velocity to acceleration, integrating back the other way, and using initial conditions to find the constants.

Generated by Claude Opus 4.89 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

SEAB wants you to move between displacement, velocity and acceleration using calculus: differentiate to go from displacement to velocity to acceleration, and integrate to go back the other way. Crucially, when you integrate you must use the initial conditions to find the constant of integration, since that is what pins down the actual motion.

The answer

Differentiating down the chain

Velocity is the rate of change of displacement, and acceleration is the rate of change of velocity:

v=dsdt,a=dvdt=d2sdt2.v = \frac{ds}{dt}, \qquad a = \frac{dv}{dt} = \frac{d^2s}{dt^2}.

So differentiating displacement once gives velocity, and twice gives acceleration.

Integrating up the chain

Reversing the arrows, integration recovers velocity from acceleration and displacement from velocity:

v=∫a dt,s=∫v dt.v = \int a\,dt, \qquad s = \int v\,dt.

Each integration introduces a constant of integration that must be found.

Using initial conditions

The constant is fixed by a known value, usually at t=0t = 0: an initial velocity gives the constant in the velocity expression, and an initial displacement gives the constant in the displacement expression. Find each constant before using the expression further.

Distance versus displacement over an interval

Over a time interval, ∫v dt\int v\,dt between the limits gives the change in displacement. If the velocity changes sign in the interval, the particle reverses, so to find the total distance travelled you split at the time when v=0v = 0 and add the magnitudes of the pieces.

Examples in context

Example 1. A car braking to a stop. Given a car's deceleration, integrating once with the initial speed gives the velocity, and the time when that velocity reaches zero is when it stops; integrating again gives the braking distance.

Example 2. A lift's smooth ride. A lift programmed with a known acceleration profile has its velocity and position found by successive integration, with the starting floor and starting rest condition fixing the constants, ensuring it stops level with the next floor.

Try this

Q1. Given s=t3−ts = t^3 - t, find the acceleration. [2 marks]

  • Cue. v=3t2−1v = 3t^2 - 1, so a=dvdt=6ta = \dfrac{dv}{dt} = 6t.

Q2. A particle has a=6ta = 6t and starts from rest. Find its velocity. [3 marks]

  • Cue. v=∫6t dt=3t2+Cv = \int 6t\,dt = 3t^2 + C; v=0v = 0 at t=0t = 0 gives C=0C = 0, so v=3t2v = 3t^2.

Q3. A particle has v=2t+1v = 2t + 1 and is at s=4s = 4 when t=0t = 0. Find ss. [3 marks]

  • Cue. s=∫(2t+1) dt=t2+t+Cs = \int (2t + 1)\,dt = t^2 + t + C; s=4s = 4 at t=0t = 0 gives C=4C = 4, so s=t2+t+4s = t^2 + t + 4.

Exam-style practice questions

Practice questions written in the style of SEAB exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Original6 marksA particle moves in a straight line with acceleration a=6t−4a = 6t - 4 m per second squared. It starts from the origin with velocity 22 m per second. Find expressions for its velocity and displacement at time tt.
Show worked answer →

Integrate acceleration for velocity: v=∫(6t−4) dt=3t2−4t+C1v = \displaystyle\int (6t - 4)\,dt = 3t^2 - 4t + C_1.

Initial condition: at t=0t = 0, v=2v = 2, so C1=2C_1 = 2. Thus v=3t2−4t+2v = 3t^2 - 4t + 2.

Integrate velocity for displacement: s=∫(3t2−4t+2) dt=t3−2t2+2t+C2s = \displaystyle\int (3t^2 - 4t + 2)\,dt = t^3 - 2t^2 + 2t + C_2.

At t=0t = 0, s=0s = 0, so C2=0C_2 = 0. Thus s=t3−2t2+2ts = t^3 - 2t^2 + 2t.

Markers reward integrating with a constant each time, applying both initial conditions, and both expressions.

Original5 marksA particle has velocity v=4t−t2v = 4t - t^2 m per second. Find the displacement travelled from t=0t = 0 to t=4t = 4.
Show worked answer →

The velocity is zero at t=0t = 0 and t=4t = 4 (since 4t−t2=t(4−t)4t - t^2 = t(4 - t)), and positive in between, so the particle moves in one direction over [0,4][0, 4].

Displacement =∫04(4t−t2) dt=[2t2−t33]04=32−643=323= \displaystyle\int_0^4 (4t - t^2)\,dt = \left[2t^2 - \dfrac{t^3}{3}\right]_0^4 = 32 - \dfrac{64}{3} = \dfrac{32}{3} metres.

Markers reward setting up the definite integral, checking the velocity does not change sign, and the value 323\dfrac{32}{3}.

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