๐Ÿš€ Variable Acceleration

A Level Maths Year 1 ยท Mechanics

Level 3 · Ages 16–17

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1 When suvat Fails

The suvat equations only work when the acceleration is constant. When displacement, velocity or acceleration is given as a function of time, you need calculus (DfE content area Q ยท Kinematics, using the differentiation and integration of content areas G and H).

Velocity is the rate of change of displacement; acceleration is the rate of change of velocity. "Rate of change" means "derivative". So you differentiate to go from $s$ to $v$ to $a$, and integrate to go back.
The calculus ladder
$s \;\xrightarrow{\;\frac{\mathrm{d}}{\mathrm{d}t}\;}\; v = \dfrac{\mathrm{d}s}{\mathrm{d}t} \;\xrightarrow{\;\frac{\mathrm{d}}{\mathrm{d}t}\;}\; a = \dfrac{\mathrm{d}v}{\mathrm{d}t} = \dfrac{\mathrm{d}^2 s}{\mathrm{d}t^2}$

$a \;\xrightarrow{\;\int \mathrm{d}t\;}\; v = \displaystyle\int a\,\mathrm{d}t \;\xrightarrow{\;\int \mathrm{d}t\;}\; s = \displaystyle\int v\,\mathrm{d}t$
These link directly to the graphs in Motion Graphs: differentiating finds a gradient, integrating finds an area. At Year 1 the functions are polynomials in $t$, so you only need the power rules from Differentiating Powers of x and Indefinite Integration.
2 From Displacement to Velocity and Acceleration
Worked Example 1 โ€” Differentiating twice

A particle moves along a straight line so that its displacement from $O$ at time $t$ s is $s = t^3 - 6t^2 + 9t$ m, for $t \geqslant 0$. Find expressions for $v$ and $a$, and find when the particle is at rest.

โ‘ $v = \dfrac{\mathrm{d}s}{\mathrm{d}t} = 3t^2 - 12t + 9$
โ‘ก$a = \dfrac{\mathrm{d}v}{\mathrm{d}t} = 6t - 12$
โ‘ขAt rest when $v = 0$: $3(t^2 - 4t + 3) = 3(t - 1)(t - 3) = 0$, so $t = 1$ s and $t = 3$ s.
โ‘ฃPositions: $s(1) = 1 - 6 + 9 = 4$ m;  $s(3) = 27 - 54 + 27 = 0$ m (back at $O$).
t s (m) 4 0 1 2 3 4 v = 0 at t = 1, s = 4 v = 0 at t = 3 s = tยณ โˆ’ 6tยฒ + 9t: the particle turns round where the gradient is zero
Worked Example 2 โ€” Distance travelled when the particle turns round

For the particle in Example 1, find the total distance travelled in the first $4$ seconds.

โ‘ The particle changes direction at $t = 1$ and $t = 3$, so find $s$ at $t = 0, 1, 3, 4$:  $0,\; 4,\; 0,\; 4$.
โ‘ก$0 \to 4$: $4$ m.  $4 \to 0$: $4$ m.  $0 \to 4$: $4$ m.
โ‘ขTotal distance $= 12$ m, although the displacement at $t = 4$ is only $4$ m.
Simply working out $s(4) - s(0)$ gives the displacement, not the distance. Always check whether $v = 0$ inside the interval.
3 Maximum and Minimum Values
Use the same idea as for stationary points: maximum or minimum displacement when $\dfrac{\mathrm{d}s}{\mathrm{d}t} = v = 0$;   maximum or minimum velocity when $\dfrac{\mathrm{d}v}{\mathrm{d}t} = a = 0$.
Worked Example 3 โ€” Greatest displacement

A particle's displacement is $s = 2 + 12t - t^3$ m for $t \geqslant 0$. Find its greatest displacement from $O$ in the positive direction.

โ‘ $v = 12 - 3t^2 = 0 \Rightarrow t^2 = 4 \Rightarrow t = 2$ (as $t \geqslant 0$).
โ‘ก$\dfrac{\mathrm{d}^2 s}{\mathrm{d}t^2} = -6t = -12 < 0$ at $t = 2$, so this is a maximum.
โ‘ข$s(2) = 2 + 24 - 8 = 18$ m.
Worked Example 4 โ€” Greatest velocity

A particle has velocity $v = 8t - 2t^2$ m s$^{-1}$ for $0 \leqslant t \leqslant 4$. Find its maximum velocity.

โ‘ $a = 8 - 4t = 0 \Rightarrow t = 2$.
โ‘ก$\dfrac{\mathrm{d}a}{\mathrm{d}t} = -4 < 0$, so a maximum. $v(2) = 16 - 8 = 8$ m s$^{-1}$.
Also check the end-points of the interval: $v(0) = 0$ and $v(4) = 0$, so $8$ m s$^{-1}$ is indeed the greatest.
4 From Acceleration to Velocity and Displacement

Integrating introduces a constant of integration. You find it from an initial condition โ€” usually the velocity or position at $t = 0$.

Worked Example 5 โ€” Integrating twice

A particle has acceleration $a = (6t - 4)$ m s$^{-2}$. At $t = 0$ it is at $O$ with velocity $3$ m s$^{-1}$. Find $v$ and $s$ in terms of $t$, and its displacement when $t = 2$.

โ‘ $v = \displaystyle\int (6t - 4)\,\mathrm{d}t = 3t^2 - 4t + c$.
โ‘ก$v = 3$ when $t = 0$, so $c = 3$:  $v = 3t^2 - 4t + 3$.
โ‘ข$s = \displaystyle\int (3t^2 - 4t + 3)\,\mathrm{d}t = t^3 - 2t^2 + 3t + k$; $s = 0$ at $t = 0$, so $k = 0$.
โ‘ฃ$s(2) = 8 - 8 + 6 = 6$ m.
Displacement between two times
displacement from $t_1$ to $t_2 = \displaystyle\int_{t_1}^{t_2} v\,\mathrm{d}t$   (the area under the $v$โ€“$t$ graph)
Worked Example 6 โ€” Definite integral, with a change of direction

A particle has velocity $v = 12 - 3t^2$ m s$^{-1}$. Find (a) its displacement and (b) the distance it travels between $t = 0$ and $t = 3$.

โ‘ (a) $\displaystyle\int_0^3 (12 - 3t^2)\,\mathrm{d}t = \Big[12t - t^3\Big]_0^3 = 36 - 27 = 9$ m.
โ‘ก(b) $v = 0$ at $t = 2$, so split there.
โ‘ข$\displaystyle\int_0^2 = \Big[12t - t^3\Big]_0^2 = 24 - 8 = 16$;   $\displaystyle\int_2^3 = 9 - 16 = -7$.
โ‘ฃDistance $= 16 + 7 = 23$ m.
Worked Example 7 โ€” Recovering the suvat equations

Show that if $a$ is constant, with $v = u$ and $s = 0$ at $t = 0$, then $v = u + at$ and $s = ut + \tfrac12 at^2$.

โ‘ $v = \displaystyle\int a\,\mathrm{d}t = at + c$; at $t = 0$, $v = u$, so $c = u$:  $v = u + at$.
โ‘ก$s = \displaystyle\int (u + at)\,\mathrm{d}t = ut + \tfrac12 at^2 + k$; at $t = 0$, $s = 0$, so $k = 0$:  $s = ut + \tfrac12 at^2$.  $\blacksquare$
5 Common Mistakes
Using suvat when $a$ is not constant. If $a$ contains $t$, suvat gives the wrong answer โ€” even if it "works" numerically.
Forgetting the constant of integration, or assuming it is zero. "Starts from rest at $O$" gives $v = 0$ and $s = 0$ at $t = 0$; "starts at $O$ with speed $3$" gives $v = 3$, not $0$.
Mixing up "at rest" and "at $O$". At rest means $v = 0$; at the origin means $s = 0$. They are different conditions.
6 Quick Reference

Velocity

$v = \dfrac{\mathrm{d}s}{\mathrm{d}t}$

Acceleration

$a = \dfrac{\mathrm{d}v}{\mathrm{d}t} = \dfrac{\mathrm{d}^2 s}{\mathrm{d}t^2}$

Velocity from $a$

$v = \int a\,\mathrm{d}t$ + use initial velocity.

Displacement from $v$

$s = \int v\,\mathrm{d}t$ + use initial position.

At rest

$v = 0$.

At the origin

$s = 0$.

Max/min displacement

$v = 0$; check with $\dfrac{\mathrm{d}^2s}{\mathrm{d}t^2}$.

Max/min velocity

$a = 0$; check with $\dfrac{\mathrm{d}a}{\mathrm{d}t}$.

Distance

Split the integral where $v = 0$; add the sizes.

7 Practice Questions

In every question the particle moves in a straight line, $t$ is in seconds, $s$ in metres and $v$ in m s$^{-1}$.

Question 1

$s = 2t^3 - 5t^2 + 4$. Find the velocity and acceleration when $t = 2$.

โ–ถ Show solution

$v = 6t^2 - 10t$, so $v(2) = 24 - 20 = 4$ m s$^{-1}$.

$a = 12t - 10$, so $a(2) = 14$ m s$^{-2}$.

Question 2

$v = t^2 - 6t + 8$. Find the times when the particle is at rest and its acceleration at each of these times.

โ–ถ Show solution

$(t - 2)(t - 4) = 0$, so $t = 2$ s and $t = 4$ s.

$a = 2t - 6$: $a(2) = -2$ m s$^{-2}$, $a(4) = 2$ m s$^{-2}$.

Question 3

$a = 4 - 2t$, and $v = 5$ when $t = 0$. Find $v$ in terms of $t$ and the maximum velocity.

โ–ถ Show solution

$v = 4t - t^2 + c$, with $c = 5$:  $v = 5 + 4t - t^2$.

Maximum when $a = 0$: $t = 2$,  $v = 5 + 8 - 4 = 9$ m s$^{-1}$ (a maximum since $\tfrac{\mathrm{d}a}{\mathrm{d}t} = -2 < 0$).

Question 4

$v = 6t - 3t^2$, and the particle starts at $O$. Find $s$ in terms of $t$, and the time when it returns to $O$.

โ–ถ Show solution

$s = 3t^2 - t^3 + k$, with $k = 0$:  $s = 3t^2 - t^3 = t^2(3 - t)$.

$s = 0$ when $t = 0$ or $t = 3$. It returns to $O$ at $t = 3$ s.

Question 5

$v = 3t^2 + 2t$. Find the displacement between $t = 1$ and $t = 3$.

โ–ถ Show solution

$\displaystyle\int_1^3 (3t^2 + 2t)\,\mathrm{d}t = \Big[t^3 + t^2\Big]_1^3 = 36 - 2 = 34$ m.

($v > 0$ throughout, so this is also the distance.)

Question 6

$v = 4t - t^2$. Find the displacement and the distance travelled in the interval $0 \leqslant t \leqslant 6$.

โ–ถ Show solution

$\int v\,\mathrm{d}t = 2t^2 - \tfrac13 t^3$. $v = 0$ at $t = 4$.

$\displaystyle\int_0^4 = 32 - \tfrac{64}{3} = \tfrac{32}{3}$.   $\displaystyle\int_4^6 = (72 - 72) - \tfrac{32}{3} = -\tfrac{32}{3}$.

Displacement $= 0$ m (back at the start). Distance $= \tfrac{64}{3} = 21.3$ m (3 s.f.).

Question 7

$s = t^3 - 9t^2 + 24t$. Find the distance travelled in the first $5$ seconds.

โ–ถ Show solution

$v = 3t^2 - 18t + 24 = 3(t - 2)(t - 4)$, zero at $t = 2$ and $t = 4$.

$s(0) = 0$, $s(2) = 8 - 36 + 48 = 20$, $s(4) = 64 - 144 + 96 = 16$, $s(5) = 125 - 225 + 120 = 20$.

Distance $= 20 + 4 + 4 = 28$ m.

Question 8

$v = t^3 - 6t^2 + 9t + 2$ for $t \geqslant 0$. Find the minimum velocity for $t > 0$, and explain why the particle is never at rest.

โ–ถ Show solution

$a = 3t^2 - 12t + 9 = 3(t - 1)(t - 3)$, zero at $t = 1$ and $t = 3$.

$\tfrac{\mathrm{d}a}{\mathrm{d}t} = 6t - 12$: negative at $t = 1$ (maximum), positive at $t = 3$ (minimum).

$v(3) = 27 - 54 + 27 + 2 = 2$ m s$^{-1}$.

Also $v(0) = 2$, and $v$ increases for $t > 3$. So $v \geqslant 2 > 0$ for all $t \geqslant 0$: the particle is never at rest.

Question 9

A particle starts from rest at $O$. For $0 \leqslant t \leqslant 2$ its velocity is $v = 3t^2$; after $t = 2$ it moves with constant velocity. Find its distance from $O$ when $t = 5$.

โ–ถ Show solution

First stage: $\displaystyle\int_0^2 3t^2\,\mathrm{d}t = \Big[t^3\Big]_0^2 = 8$ m. At $t = 2$, $v = 12$ m s$^{-1}$.

Second stage: $12 \times 3 = 36$ m.

Distance from $O$ $= 8 + 36 = 44$ m.

Question 10

A particle $P$ starts from rest at $O$ and moves in a straight line with acceleration $a = (12 - 6t)$ m s$^{-2}$.

(a) Find $v$ in terms of $t$.   (b) Find the maximum velocity.   (c) Find when $P$ next comes to rest, and its distance from $O$ then.   (d) Find when $P$ returns to $O$, and its speed at that moment.

โ–ถ Show solution

(a) $v = 12t - 3t^2 + c$; $v = 0$ at $t = 0$, so $v = 12t - 3t^2$.

(b) $a = 0$ at $t = 2$; $v(2) = 24 - 12 = 12$ m s$^{-1}$ (maximum, since $\tfrac{\mathrm{d}a}{\mathrm{d}t} = -6 < 0$).

(c) $3t(4 - t) = 0 \Rightarrow t = 4$ s.

$s = 6t^2 - t^3$ (constant zero since $s = 0$ at $t = 0$), so $s(4) = 96 - 64 = 32$ m.

(d) $s = t^2(6 - t) = 0 \Rightarrow t = 6$ s.

$v(6) = 72 - 108 = -36$, so the speed is $36$ m s$^{-1}$ (moving back towards and through $O$).

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