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5.9 KinematicsIB Maths: Analysis and Approaches HL: Revision notes

Section 1

Displacement, velocity and acceleration

For motion in a straight line:

  • displacement ss is the position relative to a fixed point O, with a sign showing which side;
  • velocity v=dsdtv=\frac{ds}{dt} is the rate of change of displacement;
  • acceleration a=dvdt=d2sdt2a=\frac{dv}{dt}=\frac{d^{2}s}{dt^{2}} is the rate of change of velocity.

Example: s=t3−6t2+9ts=t^{3}-6t^{2}+9t gives v=3t2−12t+9v=3t^{2}-12t+9 and a=6t−12a=6t-12. Units follow: m, m s−1^{-1}, m s−2^{-2}.

Key termsdisplacementvelocityacceleration
Exam tip

Differentiate to go s→v→as\to v\to a; integrate to go a→v→sa\to v\to s, using given starting values to find each constant.

Section 2

Speed, rest and direction

Speed is the magnitude of velocity, ∣v∣|v|, so it is never negative. If v(2)=−3v(2)=-3 m s−1^{-1}, the speed is 3 m s−1^{-1} and the particle is moving in the negative direction.

A particle is at rest when v=0v=0. It changes direction only when vv changes sign, which usually happens at a moment of rest.

The particle is speeding up when vv and aa have the same sign and slowing down when they have opposite signs.

Key termsspeedat rest
Common mistake

"At rest" means v=0v=0, not s=0s=0. s=0s=0 means the particle is at O.

Common mistake

Assuming a negative acceleration means slowing down. If v<0v<0 too, the particle is speeding up.

Section 3

Displacement from velocity

The change in displacement between t1t_{1} and t2t_{2} is ∫t1t2v(t) dt.\int_{t_{1}}^{t_{2}}v(t)\,dt. To find the actual displacement from O, add the starting displacement. Alternatively integrate v(t)v(t) to get s(t)+cs(t)+c and use a known value (e.g. s(0)=2s(0)=2) to find cc.

Example: v=8−2tv=8-2t from the marker gives ∫06(8−2t) dt=12\int_{0}^{6}(8-2t)\,dt=12 m: the cyclist ends 12 m past the marker.

Key termschange in displacement

Section 4

Total distance travelled

Distance ignores direction, so distance=∫t1t2∣v(t)∣ dt.\text{distance}=\int_{t_{1}}^{t_{2}}|v(t)|\,dt. Without a calculator: find where v=0v=0, split the interval there, integrate each piece and add the absolute values. For v=8−2tv=8-2t on [0,6][0,6]: v=0v=0 at t=4t=4, ∫04=16\int_{0}^{4}=16, ∫46=−4\int_{4}^{6}=-4, so distance =16+4=20=16+4=20 m while displacement =12=12 m.

For a function like s=10cos⁡πt4s=10\cos\frac{\pi t}{4} you can also track the positions at each turning point: 10→−10→010\to-10\to0 gives 20+10=3020+10=30 cm.

Key termstotal distance
Common mistake

Integrating vv straight across a change of direction gives displacement, not distance.

Exam tip

With a GDC, type ∫t1t2∣v(t)∣ dt\int_{t_1}^{t_2}|v(t)|\,dt directly; on Paper 1 split at the zeros of vv.

Section 5

Interpreting motion in context

IB questions often ask you to describe motion in words. Say where the object is (sign of ss), which way it is moving (sign of vv), how fast (∣v∣|v|) and whether it is speeding up or slowing down (compare the signs of vv and aa). For the spring s=10cos⁡πt4s=10\cos\frac{\pi t}{4}, a=−π216sa=-\frac{\pi^{2}}{16}s, so acceleration always points towards the rest position: this is the signature of oscillation.

Example

v(t)=(3t−1)(t−1)<0v(t)=(3t-1)(t-1)<0 for 13<t<1\frac13<t<1: the particle moves in the negative direction between its two moments of rest.

Must know

  • v=dsdtv=\frac{ds}{dt}, a=dvdt=d2sdt2a=\frac{dv}{dt}=\frac{d^{2}s}{dt^{2}}.
  • Speed =∣v∣=|v|; at rest means v=0v=0.
  • Displacement change =∫v dt=\int v\,dt; distance =∫∣v∣ dt=\int|v|\,dt (split at v=0v=0).
  • Use initial conditions to find constants when integrating.
  • Always give units: m, m s−1^{-1}, m s−2^{-2}.

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