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Calculus in kinematicsAQA A-Level Maths: Revision notes

Section 1

Velocity and acceleration as derivatives

The displacement rr of a particle moving in a straight line is its position measured from a fixed point OO. It can be positive or negative, depending on which side of OO the particle is. Velocity is the rate of change of displacement and acceleration is the rate of change of velocity: v=drdt,a=dvdt=d2rdt2.v=\frac{dr}{dt},\qquad a=\frac{dv}{dt}=\frac{d^2r}{dt^2}. Differentiate each power of tt in turn: ddt(tn)=ntn−1\frac{d}{dt}(t^n)=nt^{n-1}. For r=2t3−9t2+12tr=2t^3-9t^2+12t (metres, tt in seconds): v=6t2−18t+12v=6t^2-18t+12 and a=12t−18a=12t-18. When t=3t=3: r=9r=9 m, v=12v=12 m s⁻¹, a=18a=18 m s⁻². The units are m, m s⁻¹ and m s⁻².

Key termsdisplacementvelocityacceleration
Common mistake

Substituting tt into rr and calling it the velocity. Differentiate first, then substitute.

Section 2

Integrating to go the other way

Reversing differentiation gives displacement from velocity and velocity from acceleration: v=∫a dt,r=∫v dt.v=\int a\,dt,\qquad r=\int v\,dt. Each indefinite integral has a constant of integration, found from the information given about the motion, such as the velocity or position at t=0t=0. Worked example: a=6t−4a=6t-4, with v=5v=5 when t=0t=0 and r=0r=0 when t=0t=0. Then v=3t2−4t+cv=3t^2-4t+c and c=5c=5, so v=3t2−4t+5v=3t^2-4t+5. Integrating again, r=t3−2t2+5t+dr=t^3-2t^2+5t+d and d=0d=0, so r=t3−2t2+5tr=t^3-2t^2+5t. When t=2t=2, r=10r=10 m.

Key termsconstant of integration
Common mistake

Leaving out the constant. Without it, the starting velocity or position is lost.

Section 3

Instantaneous rest and turning points

A particle is instantaneously at rest when v=0v=0. Solve v=0v=0 for tt, then use the sign of vv on either side: if vv changes sign the particle reverses direction there, so rr has a turning value. Positive vv means moving in the positive direction, negative vv the opposite way. The velocity is greatest or least when a=0a=0, as a=dvdta=\frac{dv}{dt}. To show it is a maximum, show dadt<0\frac{da}{dt}<0 there, or that aa changes from positive to negative. For v=6t2−18t+12=6(t−1)(t−2)v=6t^2-18t+12=6(t-1)(t-2) the particle is at rest at t=1t=1 and t=2t=2.

Key termsinstantaneous restturning point
Exam tip

Zero velocity does not always mean a change of direction. Check that vv changes sign.

Section 4

Distance and displacement

Displacement is the change of position, with direction. Distance is the total length of path and is never negative. If the particle does not change direction, distance equals the size of the change in displacement. If it does, split the motion at each time when v=0v=0 and add the sizes of each stage. Example: v=3t2−12t+9=3(t−1)(t−3)v=3t^2-12t+9=3(t-1)(t-3) and r=t3−6t2+9tr=t^3-6t^2+9t. In the first 3 s the particle moves from r=0r=0 to r(1)=4r(1)=4, then back to r(3)=0r(3)=0. Displacement =0=0 m, but distance =4+4=8=4+4=8 m.

Key termsdistance
Common mistake

Giving r(t2)−r(t1)r(t_2)-r(t_1) as the distance when the particle has turned round in between.

Section 5

Calculus or constant acceleration formulae?

The equations of constant acceleration (v=u+atv=u+at and so on) hold only when aa is constant. If aa or vv is given as a function of tt, use calculus. Check your results by substituting them back: differentiating your rr should reproduce the given vv, and rr should have the right value at t=0t=0. To compare two particles, write each displacement from the same origin and set them equal for "level". Reject any solution outside the stated time range, such as t>6t>6 when the model is only valid for 0≤t≤60\le t\le6.

Exam tip

Write the time range of the model next to your answer and check each solution lies inside it.

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Exam questions on Calculus in kinematics

  1. A particle moves in a straight line. Its displacement from a fixed point OO at time tt seconds is r=2t3−9t2+12tr=2t^3-9t^2+12t metres.
    Find the values of tt at which the particle is instantaneously at rest.2 marks
  2. A particle moves in a straight line. At time tt seconds its acceleration is (6t−4)(6t-4) m s⁻². When t=0t=0 the particle is at the fixed point OO and has velocity 55 m s⁻¹.
    Show that the particle is never instantaneously at rest.2 marks
  3. A particle PP moves on a straight line through a fixed point OO. At time tt seconds, t≥0t\ge0, its velocity is v=3t2−12t+9v=3t^2-12t+9 m s⁻¹. When t=0t=0, PP is at OO.
    Find the acceleration of PP at each time when it is instantaneously at rest.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).