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Year 12 Maths - Methods (Unit 3 & Unit 4) Applications of differentiation

Motion in a straight line

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Theory

Motion in a straight line is analysed with calculus. Differentiate the displacement \(x(t)\) once for the velocity \(v=\dfrac{dx}{dt}\) and again for the acceleration \(a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\). The sign of \(v\) gives the direction, \(v=0\) marks where the particle is momentarily at rest, and the sign of \(v\,a\) tells you whether it is speeding up or slowing down.

For a particle moving on a straight line, its displacement \(x\) (its signed position from a fixed origin \(O\)) is a function of time \(t\). Its motion is described by two derivatives:

Velocity is the rate of change of displacement, \(v=\dfrac{dx}{dt}\). Its sign gives the direction of motion; its size \(|v|\) is the speed.

Acceleration is the rate of change of velocity, \(a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\) — the second derivative of displacement.

The particle is momentarily at rest when \(v=0\); it is moving in the positive direction when \(v>0\) and the negative direction when \(v<0\). It is speeding up when \(v\) and \(a\) share a sign and slowing down when they have opposite signs.

Key idea. \(x \xrightarrow{\;d/dt\;} v \xrightarrow{\;d/dt\;} a\). Differentiate to go from position to velocity to acceleration. At rest \(\Rightarrow v=0\); direction \(\Rightarrow\) sign of \(v\); speeding up \(\Rightarrow v\,a>0\).
Displacement-time graphThe displacement x=t^3-6t^2+9t rises to a maximum of 4 at t=1 where the velocity (gradient) is zero, then falls to 0 at t=3. t x (1,4)
Displacement-time: the gradient is the velocity, so the peak \((1,4)\) (where \(v=0\)) is the maximum displacement
Velocity-time graphThe velocity v=3t^2-12t+9 is zero at t=1 and t=3, where the particle is momentarily at rest; the particle moves in the negative direction between them. t v t=1 t=3
Velocity-time: \(v=0\) at \(t=1\) and \(t=3\) — the particle is momentarily at rest, and \(v<0\) between them

Velocity and acceleration from displacement \(x(t)\):

\[v=\dfrac{dx}{dt},\qquad a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\]
v=dxdt,a=d2xdt2

Reading the motion from the signs:

\[v=0 \ \text{(at rest)},\quad v>0 \ \text{(positive direction)},\quad v<0 \ \text{(negative direction)},\quad \text{speed}=|v|\]
Speeding up or slowing down. Compare the signs of \(v\) and \(a\): if \(v\,a>0\) (same sign) the particle is speeding up; if \(v\,a<0\) (opposite signs) it is slowing down.

Turning points of the motion (for maxima/minima):

\[\text{max/min displacement: } v=\dfrac{dx}{dt}=0;\qquad \text{max/min velocity: } a=\dfrac{dv}{dt}=0\]
a=dvdt=0

How to analyse straight-line motion

  1. Differentiate. From \(x(t)\), find \(v=\dfrac{dx}{dt}\) and \(a=\dfrac{dv}{dt}\). Evaluate at a required time by substitution.
  2. At rest. Solve \(v=0\) for the time(s); substitute back into \(x\) or \(a\) for the position or acceleration then.
  3. Direction. Read the sign of \(v\): positive means the positive direction, negative means the negative direction.
  4. Speeding up or slowing down. Compare the signs of \(v\) and \(a\): same sign \(\Rightarrow\) speeding up; opposite signs \(\Rightarrow\) slowing down.
  5. Maxima/minima. For greatest displacement solve \(v=0\); for greatest/least velocity solve \(a=0\). Confirm with a second-derivative or sign test and check any interval endpoints.
Distance vs displacement. If the particle changes direction (at a time when \(v=0\)), the distance travelled is the sum of the distances between successive positions, not just the change in displacement.
Example 1 — Velocity at an instant
A particle has displacement \(x=2t^{3}-3t^{2}+4\) metres. Find its velocity when \(t=2\) s.
Solution
Velocity — differentiate the displacement:
\(v=\dfrac{dx}{dt}\)\(=\)\(6t^{2}-6t\)
Evaluate — substitute \(t=2\):
\(v(2)\)\(=\)\(6(2)^{2}-6(2)\)
\(=\)\(24-12\)
\(=\)\(12\)
\(\therefore\) Velocity at \(t=2\): \(12\;\text{m/s}\)
v=12
Example 2 — When is it at rest?
A particle has displacement \(x=t^{3}-6t^{2}+9t+1\) metres. Find when it is momentarily at rest.
Solution
Velocity — differentiate the displacement:
\(v=\dfrac{dx}{dt}\)\(=\)\(3t^{2}-12t+9\)
At rest — set \(v=0\) and solve:
\(3t^{2}-12t+9\)\(=\)\(0\)
\(3(t-1)(t-3)\)\(=\)\(0\)
\(t\)\(=\)\(1\) or \(3\) s
\(\therefore\) Momentarily at rest when \(t=1\) s and \(t=3\) s
t=1 or 3
Example 3 — Speeding up or slowing down
For \(x=t^{3}-3t^{2}-9t+2\) metres, is the particle speeding up or slowing down at \(t=2\) s?
Solution
Velocity and acceleration — differentiate once and twice:
\(v=\dfrac{dx}{dt}\)\(=\)\(3t^{2}-6t-9\)
\(a=\dfrac{dv}{dt}\)\(=\)\(6t-6\)
Evaluate at \(t=2\):
\(v(2)\)\(=\)\(3(2)^{2}-6(2)-9\)
\(=\)\(12-12-9=-9\)
\(a(2)\)\(=\)\(6(2)-6\)
\(=\)\(6\)
Compare signs — form the product \(v\,a\):
\(v\,a\)\(=\)\((-9)(6)\)
\(=\)\(-54\)
\(\therefore\) \(v\,a<0\) (opposite signs), so the particle is slowing down
va<0
Example 4 — Maximum displacement
For \(x=t^{3}-6t^{2}+9t\) metres on \(0\le t\le 3\), find the maximum displacement.
Solution
Stationary points — differentiate and set \(v=0\):
\(v=\dfrac{dx}{dt}\)\(=\)\(3t^{2}-12t+9\)
\(=\)\(3(t-1)(t-3)\)
\(v=0\)\(\Rightarrow\)\(t=1\) or \(t=3\)
Classify \(t=1\) — use the acceleration \(a=6t-12\):
\(a(1)\)\(=\)\(6(1)-12\)
\(=\)\(-6<0\) (maximum)
Displacement there — substitute \(t=1\) into \(x\):
\(x(1)\)\(=\)\((1)^{3}-6(1)^{2}+9(1)\)
\(=\)\(1-6+9\)
\(=\)\(4\)
Check the endpoints of \(0\le t\le 3\):
\(x(0)\)\(=\)\(0\)
\(x(3)\)\(=\)\(27-54+27=0\)
\(\therefore\) Maximum displacement: \(4\;\text{m}\) (at \(t=1\) s)
Displacement-time graphThe displacement x=t^3-6t^2+9t rises to a maximum of 4 at t=1 where the velocity (gradient) is zero, then falls to 0 at t=3. t x (1,4)
xmax=4

Common pitfalls

Do not confuse velocity with acceleration. Velocity is the first derivative of displacement and acceleration is the second. Substituting a time into \(x\) or into the wrong derivative is the most common slip.
Slowing down is not the same as negative acceleration. A particle with \(a<0\) can still be speeding up (if \(v<0\) too). Compare the signs of \(v\) and \(a\): \(v\,a>0\) is speeding up, \(v\,a<0\) is slowing down.
Distance is not just the change in displacement. When the particle reverses direction (where \(v=0\)), add the distances between successive rest positions rather than subtracting the end displacements.

Frequently asked questions

How do you find velocity and acceleration from displacement?

Differentiate: \(v=\dfrac{dx}{dt}\) (once) and \(a=\dfrac{dv}{dt}=\dfrac{d^{2}x}{dt^{2}}\) (twice), then substitute the required time.

When is a particle momentarily at rest?

When \(v=0\). Set the velocity to zero and solve for \(t\); the particle stops there before changing direction.

How do you tell which direction a particle is moving?

By the sign of \(v\): \(v>0\) is the positive direction, \(v<0\) the negative direction, \(v=0\) momentarily at rest.

What is the difference between speeding up and slowing down?

Speeding up: \(v\) and \(a\) have the same sign (\(v\,a>0\)). Slowing down: opposite signs (\(v\,a<0\)).

How do you find the maximum displacement or velocity?

Maximum displacement is where \(v=0\); maximum/minimum velocity is where \(a=0\). Confirm with a second-derivative test and check the interval endpoints.

What is the difference between distance and displacement?

Displacement is the signed change in position; distance is the total path length. When the particle reverses, add the distances between successive rest positions.