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How do we use calculus to describe motion and derive the equations of motion?

Calculus relationships between displacement, velocity and acceleration, derivation of the equations of motion by integration, and motion under constant and varying acceleration.

An SQA Advanced Higher Physics answer on kinematic relationships, covering velocity and acceleration as derivatives of displacement, deriving the equations of motion by integration, and using calculus for motion under constant and varying acceleration.

Generated by Claude Opus 4.814 min answer

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

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  1. What this key area is asking
  2. Velocity and acceleration as derivatives
  3. Deriving the equations of motion
  4. Motion under varying acceleration
  5. Examples in context
  6. Try this

What this key area is asking

The SQA wants you to treat motion with calculus: to know that velocity is the rate of change of displacement and acceleration the rate of change of velocity, to derive the equations of motion by integration, and to use differentiation or integration to find instantaneous displacement, velocity and acceleration for straight-line motion under constant or varying acceleration. This is the calculus foundation the whole Advanced Higher course rests on.

Velocity and acceleration as derivatives

On a displacement-time graph, the gradient at a point is the instantaneous velocity, found by differentiation. On a velocity-time graph the gradient is the instantaneous acceleration, and the area under the line between two times is the displacement, found by integration. The calculus simply makes these graph rules exact for any curve, not just straight lines.

If you are given displacement as a function of time, differentiate once for velocity and again for acceleration. If you are given acceleration, integrate once for velocity and again for displacement. Each integration introduces a constant of integration that you find from the initial conditions (the velocity or displacement at t=0t = 0).

Deriving the equations of motion

Start from constant acceleration aa. Integrating with respect to time:

v=adt=at+c.v = \int a\, dt = at + c.

At t=0t = 0 the velocity is the initial velocity uu, so c=uc = u and:

v=u+at.v = u + at.

Now integrate the velocity to get displacement:

s=(u+at)dt=ut+12at2+c.s = \int (u + at)\, dt = ut + \tfrac{1}{2}at^2 + c.

Taking displacement as zero at t=0t = 0 gives c=0c = 0, so:

s=ut+12at2.s = ut + \tfrac{1}{2}at^2.

The third equation, v2=u2+2asv^2 = u^2 + 2as, follows by eliminating tt between these two. The crucial point the SQA tests is that these results hold only for constant acceleration, because the integration treated aa as a constant.

Motion under varying acceleration

When acceleration is not constant, the equations of motion fail and you must work from the calculus directly.

For example, if s=2t4s = 2t^4 then v=8t3v = 8t^3 and a=24t2a = 24t^2, so the acceleration grows with time and no single equation of motion applies. Reading the question to decide whether acceleration is constant (use the equations of motion) or varying (use calculus) is the key first step.

Examples in context

A car pulling away has a roughly constant acceleration, so the equations of motion fit, but a rocket burns fuel and loses mass, so its acceleration rises and only calculus describes it. A damped oscillator has an acceleration that depends on position and time, so its motion is found by solving the relationship a=dvdta = \frac{dv}{dt} directly. Engineers fitting a polynomial to motion-sensor data differentiate it to recover velocity and acceleration, exactly the operation this key area drills.

Try this

Q1. State what physical quantity the second derivative of displacement with respect to time represents. [1 mark]

  • Cue. The acceleration.

Q2. The displacement of an object is s=5t2+2ts = 5t^2 + 2t. Find an expression for its velocity. [2 marks]

  • Cue. v=dsdt=10t+2 m s1v = \frac{ds}{dt} = 10t + 2\ \text{m s}^{-1}.

Q3. State why the equation s=ut+12at2s = ut + \tfrac{1}{2}at^2 cannot be used when the acceleration varies with time. [1 mark]

  • Cue. It is derived by integrating a constant acceleration, so it only holds for constant aa.

Exam-style practice questions

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

SQA AH style5 marksThe displacement of an object moving in a straight line is given by s=3t32t2+5ts = 3t^3 - 2t^2 + 5t, where ss is in metres and tt in seconds. Derive expressions for the velocity and acceleration, and find the acceleration at t=2.0t = 2.0 s.
Show worked answer →

Velocity is the first derivative of displacement with respect to time.

Differentiate: v=dsdt=9t24t+5v = \frac{ds}{dt} = 9t^2 - 4t + 5.

Acceleration is the derivative of velocity (the second derivative of displacement).

Differentiate again: a=dvdt=18t4a = \frac{dv}{dt} = 18t - 4.

Substitute t=2.0t = 2.0: a=18(2.0)4=32 m s2a = 18(2.0) - 4 = 32\ \text{m s}^{-2}.

Markers reward differentiating term by term, recognising acceleration as the second differential, and the final value with unit. A common error is to differentiate only once and quote the velocity as the acceleration.

SQA AH style4 marksThe acceleration of an object is given by a=6ta = 6t. At t=0t = 0 the object has velocity 4extms14 ext{m s}^{-1}. Use integration to find an expression for the velocity as a function of time.
Show worked answer →

Velocity is the integral of acceleration with respect to time.

Integrate: v=6tdt=3t2+cv = \int 6t\, dt = 3t^2 + c.

Apply the initial condition v=4v = 4 when t=0t = 0: 4=3(0)2+c4 = 3(0)^2 + c, so c=4c = 4.

Therefore v=3t2+4 m s1v = 3t^2 + 4\ \text{m s}^{-1}.

Markers reward integrating correctly, including the constant of integration, and using the initial condition to evaluate it. The frequent error is omitting the constant cc, which loses the initial-velocity information.

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