Mathematics/Lessons/Variable Acceleration/Maxima and Minima Problems
Mechanics · Variable Acceleration · Year 1

Maxima and Minima Problems

Instantaneous rest, greatest velocity, greatest speed — all three are questions about turning points, and calculus finds them the same way it finds any other maximum or minimum.

12 min read 3 worked examples

Three different questions, one method

Calculus answers several distinct-sounding questions about motion using the same turning-point technique:

Instantaneous rest: solve $v(t)=0$.
Maximum or minimum displacement: solve $\dfrac{ds}{dt}=v(t)=0$, then classify using $\dfrac{d^2s}{dt^2}$.
Maximum or minimum velocity: solve $\dfrac{dv}{dt}=a(t)=0$, then classify using $\dfrac{d^2v}{dt^2}$.
Classifying a turning point

At a stationary value, a negative second derivative means a maximum and a positive second derivative means a minimum — exactly the same test used for stationary points of any curve.

Worked example 1

Maximum height, with a justified restriction
A toy drone rises from the ground and later lands again. Its height above the ground, $h$ metres, at time $t$ seconds is modelled by $h = 2.4t + 0.6t^2 - 0.3t^3$ for $0 \le t \le 4$. a Justify the restriction $0 \le t \le 4$. b Find the maximum height reached, correct to 3 s.f.
MethodFactorise to justify the domain, then differentiate to maximise
a
$h = 0.3t(8+2t-t^2) = 0.3t(4-t)(2+t)$.
Factorise the cubic.
For $00$, $(4-t)>0$ and $(2+t)>0$, so $h>0$ throughout — the drone stays above the ground. At $t=4$, $h=0$: the drone has landed, so the model should not continue past this point.
h must be non-negative, and motion starts at t=0.
b
$\dfrac{dh}{dt} = 2.4+1.2t-0.9t^2$. Setting this to zero: $0.9t^2-1.2t-2.4=0 \Rightarrow 3t^2-4t-8=0$.
Divide through by 0.3, then rearrange to standard form.
$t = \dfrac{4\pm\sqrt{16+96}}{6} = \dfrac{4\pm\sqrt{112}}{6}$. Taking the positive root: $t = 2.4305\ldots$ s.
Quadratic formula; reject the negative root.
$\dfrac{d^2h}{dt^2}=1.2-1.8t$, which is negative at $t=2.4305$, confirming a maximum.
Second derivative test.
$h(2.4305\ldots) = 2.4(2.4305)+0.6(2.4305)^2-0.3(2.4305)^3 = 5.07\ \text{m}$ (3 s.f.).
Substitute the unrounded t-value.
▪ solved
A cubic curve for h against t, rising from the origin, reaching a single maximum marked at t=2.43, then falling back to the t-axis at t=4.
The maximum height occurs at the single turning point inside the valid domain, between $t=0$ and the drone's landing at $t=4$.

Worked example 2

Rest points and maximum velocity
A particle's velocity at time $t$ seconds ($0 \le t \le 8$) is $v = 18t - 3t^2\ \text{m s}^{-1}$. Find the times at which the particle is instantaneously at rest, and its maximum velocity in this interval.
MethodSolve v = 0 for rest, dv/dt = 0 for the turning point of v
1
Instantaneous rest: $18t-3t^2=0 \Rightarrow 3t(6-t)=0$, so $t=0$ or $t=6$.
Factorise and solve.
2
$\dfrac{dv}{dt}=18-6t$. Setting this to zero: $t=3$.
A turning point of v occurs where a = 0.
3
$\dfrac{d^2v}{dt^2}=-6<0$, so $t=3$ gives a maximum.
Second derivative test.
4
$v(3) = 18(3)-3(9) = 54-27=27\ \text{m s}^{-1}$.
Substitute t = 3.
▪ solved

Worked example 3

Greatest speed — don't forget the endpointsChallenge
A particle's velocity at time $t$ seconds ($0 \le t \le 7$) is $v = t^2 - 8t + 12\ \text{m s}^{-1}$. Find the greatest speed of the particle in this interval.
MethodFind the interior turning point, then check both endpoints too
1
$\dfrac{dv}{dt}=2t-8=0 \Rightarrow t=4$. Since $\dfrac{d^2v}{dt^2}=2>0$, this is a minimum of $v$: $v(4)=16-32+12=-4\ \text{m s}^{-1}$.
The only interior turning point.
2
Check the endpoints too: $v(0)=12\ \text{m s}^{-1}$ and $v(7)=49-56+12=5\ \text{m s}^{-1}$.
The greatest speed can occur at either end of a closed interval.
3
Speeds at the three candidate points: $|12|=12$, $|-4|=4$, $|5|=5$. The greatest is $12\ \text{m s}^{-1}$, occurring at $t=0$.
Compare magnitudes, not signed velocities.
▪ solved
The interior turning point is not always the answer

The minimum of $v$ occurs at $t=4$, but that is a minimum of velocity, not the greatest speed. The greatest speed here actually occurs at the very start of the interval, $t=0$ — always check both endpoints of a closed interval, not just the interior stationary point.

A velocity-time graph, an upward parabola dipping below the t-axis. Points are marked at t=0 with v=12, t=4 with v=-4 (the interior minimum), and t=7 with v=5, showing that the greatest speed occurs at the endpoint t=0 rather than at the interior turning point.
The interior turning point at $t=4$ gives the smallest velocity, but the largest speed in the interval is actually at the endpoint $t=0$.
Common mistake

Reporting the interior stationary value of $v$ as the "greatest speed" without checking the endpoints of the given interval. On a closed interval $[0,T]$, the greatest speed can occur at $t=0$, at $t=T$, or at an interior point where $v=0$ or $a=0$ — all candidates must be compared. Confusing "greatest velocity" (a signed quantity, can be negative) with "greatest speed" (always non-negative, $|v|$) is the other frequent error.

Check yourself

A particle's velocity at time $t$ seconds ($0 \le t \le 6$) is $v = 10t - 2t^2\ \text{m s}^{-1}$. Find the times at which the particle is instantaneously at rest, and its maximum velocity in this interval, justifying that it is a maximum.
(Hint: solve v = 0, then dv/dt = 0, and classify with the second derivative.)

$10t-2t^2=0 \Rightarrow 2t(5-t)=0$, so the particle is at rest at $t=0$ and $t=5$.

$\dfrac{dv}{dt}=10-4t=0$ at $t=2.5$, and $\dfrac{d^2v}{dt^2}=-4<0$, confirming a maximum. $v(2.5)=25-12.5=12.5\ \text{m s}^{-1}$.