๐ŸŽก Parametric Modelling

A Level Maths Year 2 ยท Parametric Equations

Level 3 · Ages 17–18

← Back to topic overview
1 The Parameter as Time (or Angle)
In a model, the parameter usually has a physical meaning. Most often it is time $t$: then $(x(t), y(t))$ is where the object is at time $t$. For a wheel or a ride it is often an angle $\theta$ turned through. The Cartesian equation tells you the shape of the path; only the parametric form tells you when the object is at each point.
Question asksโ€ฆWhat to do
Where is it at time $t = 2$?Substitute $t = 2$ into both equations
When does it reach the ground?Solve $y(t) = 0$ (taking the sensible root)
When is it highest?Find the maximum of $y(t)$ โ€” complete the square, or use calculus
What shape is the path?Eliminate $t$ to get a Cartesian equation
For what values is the model valid?Restrict $t$ so that the situation makes sense (e.g. $y \geqslant 0$, $t \geqslant 0$)
Always state units and interpret answers in context: "the ball lands $38.4$ m from the point of projection after $3.2$ seconds", not just "$t = 3.2$".
2 Projectile-like Paths

A ball thrown through the air moves at a steady speed horizontally while its height follows a quadratic in $t$. That gives parametric equations of the form $x = at$, $y = bt - ct^2$. (Where these come from is covered in Year 2 mechanics, on Projectiles.)

Worked Example 1 โ€” A thrown ball

A ball is thrown from ground level. Its position $t$ seconds later is $x = 12t$, $y = 16t - 5t^2$, where $x$ and $y$ are the horizontal and vertical distances in metres.

(a) When and where does it land?  (b) Find its greatest height.  (c) Find the Cartesian equation of its path, with the domain for which the model is valid.

โ‘ (a) $y = 0$: $t(16 - 5t) = 0$, so $t = 0$ (launch) or $t = 3.2$. It lands after $3.2$ s, at $x = 12 \times 3.2 = 38.4$ m.
โ‘ก(b) $y = -5(t^2 - 3.2t) = -5(t - 1.6)^2 + 12.8$. Greatest height $12.8$ m, at $t = 1.6$ s (halfway through the flight), where $x = 19.2$ m.
โ‘ข(c) $t = \dfrac{x}{12}$, so $y = 16\left(\dfrac{x}{12}\right) - 5\left(\dfrac{x}{12}\right)^2 = \dfrac{4x}{3} - \dfrac{5x^2}{144}$.
โ‘ฃThe model applies while the ball is in the air: $0 \leqslant t \leqslant 3.2$, so $0 \leqslant x \leqslant 38.4$.
5 10 15 20 25 30 35 40 -2 2 4 6 8 10 12 14 x y max (19.2, 12.8), t = 1.6 (38.4, 0) y
Does it clear a 2 m wall 30 m away? $x = 30$ when $t = 2.5$, and then $y = 40 - 31.25 = 8.75$ m. Yes, comfortably.
3 Circular Motion: A Big Wheel
Moving round a circle of radius $r$, centre $(a, b)$
$x = a + r\sin(\omega t)$,  $y = b - r\cos(\omega t)$  โ€” starts at the bottom $(a,\, b - r)$ when $t = 0$
One revolution takes $\dfrac{2\pi}{\omega}$ (with the angle in radians)
Worked Example 2 โ€” An observation wheel

A capsule on an observation wheel has position $x = 20\sin\left(\dfrac{\pi t}{15}\right)$, $y = 22 - 20\cos\left(\dfrac{\pi t}{15}\right)$, where $t$ is in minutes, $y$ is the height above the ground in metres and $x$ is the horizontal displacement from the vertical line through the centre.

(a) Find the radius, the height of the centre, and the time for one revolution.  (b) Find the lowest and greatest heights.  (c) For how long in each revolution is the capsule more than $32$ m above the ground?

โ‘ (a) $x^2 + (y - 22)^2 = 400$: a circle, radius $20$ m, centre $22$ m above the ground. One revolution when $\dfrac{\pi t}{15} = 2\pi$: $t = 30$ minutes.
โ‘ก(b) $\cos$ ranges from $-1$ to $1$, so $y$ ranges from $22 - 20 = 2$ m (at $t = 0$) to $22 + 20 = 42$ m (at $t = 15$).
โ‘ข(c) $22 - 20\cos\left(\dfrac{\pi t}{15}\right) > 32 \Rightarrow \cos\left(\dfrac{\pi t}{15}\right) < -\dfrac12$.
โ‘ฃFor $0 \leqslant \dfrac{\pi t}{15} \leqslant 2\pi$ this holds when $\dfrac{2\pi}{3} < \dfrac{\pi t}{15} < \dfrac{4\pi}{3}$, i.e. $10 < t < 20$.
โ‘คSo the capsule is above $32$ m for $10$ minutes of each $30$-minute revolution.
4 A Point on a Rolling Wheel
A bicycle wheel of radius $r$ rolls along flat ground. A small stone stuck in the tyre traces a cycloid: $x = r(\theta - \sin\theta)$, $y = r(1 - \cos\theta)$, where $\theta$ is the angle (in radians) the wheel has turned. The $r\theta$ term is how far the wheel's centre has moved; the $\sin$ and $\cos$ terms describe the stone's position relative to the centre.
1 2 3 4 0.5 1 x y ฮธ = ฯ€ ฮธ = 2ฯ€: x = 2ฯ€r โ‰ˆ 2.20
Worked Example 3 โ€” A stone in a tyre

A wheel has radius $0.35$ m. Using the cycloid model, find (a) the greatest height of the stone and where it occurs in the first revolution, (b) how far the bicycle moves in one revolution, and (c) the first value of $\theta$ at which the stone is $0.525$ m above the ground.

โ‘ (a) $y = 0.35(1 - \cos\theta)$ is greatest when $\cos\theta = -1$, i.e. $\theta = \pi$: $y = 0.7$ m (the top of the wheel). Then $x = 0.35\pi \approx 1.10$ m.
โ‘ก(b) One revolution is $\theta = 2\pi$: $x = 0.35(2\pi - 0) = 0.7\pi \approx 2.20$ m โ€” the circumference, as expected.
โ‘ข(c) $0.35(1 - \cos\theta) = 0.525 \Rightarrow 1 - \cos\theta = 1.5 \Rightarrow \cos\theta = -\tfrac12 \Rightarrow \theta = \dfrac{2\pi}{3}$.
5 Restricting the Domain and Criticising the Model
The equations of a model usually make sense mathematically for all $t$, but physically only for some. State the restriction, and say why.
Worked Example 4 โ€” Two boats: paths cross, but do they collide?

Two boats move so that, $t$ hours after noon, boat A is at $x = t$, $y = 2t$ and boat B is at $x = 6 - t$, $y = t + 3$ (distances in km). Do their paths cross? Do the boats collide?

โ‘ Paths: A lies on $y = 2x$; B lies on $y = (6 - x) + 3 = 9 - x$. These meet where $2x = 9 - x$: $x = 3$, $y = 6$. So the paths cross at $(3, 6)$.
โ‘กA is at $(3, 6)$ when $t = 3$. B is at $x = 3$ when $t = 3$, and then $y = 6$. Both are there at the same time.
โ‘ขSo the boats collide at 3 pm (if the model is right and the boats are treated as points).
Paths crossing is not the same as a collision. The Cartesian equations only tell you about the paths; you need the parameter to check whether the objects are there at the same time.
Worked Example 5 โ€” Limitations

Give three limitations of the model $x = 12t$, $y = 16t - 5t^2$ for the ball in Worked Example 1.

โ‘ It ignores air resistance, which would slow the ball and shorten its range.
โ‘กIt treats the ball as a particle, ignoring its size and any spin.
โ‘ขIt does not apply for $t > 3.2$: the formula would give negative heights, but the ball has hit the ground.
6 Quick Reference

Position at time $t$

Substitute into both equations.

Lands

Solve $y(t) = 0$, take $t > 0$.

Highest point

Complete the square on $y(t)$.

Path

Eliminate $t$; state the domain.

Circle

$x = a + r\sin\omega t$, $y = b - r\cos\omega t$; period $\tfrac{2\pi}{\omega}$.

Cycloid

$x = r(\theta - \sin\theta)$, $y = r(1 - \cos\theta)$.

Collision

Same point at the same $t$.

Validity

Restrict $t$: e.g. $t \geqslant 0$, $y \geqslant 0$.

7 Practice Questions
Question 1

A cyclist's position $t$ hours after setting off is $x = 2t$, $y = 3t + 1$ (km). (a) Where is she when $t = 2$?  (b) Find the Cartesian equation of her path.  (c) Find her speed.

โ–ถ Show solution

(a) $(4, 7)$.

(b) $t = \tfrac{x}{2}$, so $y = \tfrac32 x + 1$ โ€” a straight line.

(c) Each hour $x$ increases by $2$ and $y$ by $3$, so she travels $\sqrt{2^2 + 3^2} = \sqrt{13} \approx 3.61$ km per hour.

Question 2

A particle moves so that $x = t^2 - 4$, $y = 2t$, for $0 \leqslant t \leqslant 3$. Find its start and end points, and when and where it crosses the $y$-axis.

โ–ถ Show solution

$t = 0$: $(-4, 0)$.   $t = 3$: $(5, 6)$.

$x = 0$: $t^2 = 4$, $t = 2$ (as $t \geqslant 0$). Position $(0, 4)$.

Question 3

A ball is hit from a height of $1.5$ m. Its position after $t$ seconds is $x = 15t$, $y = 1.5 + 10t - 4.9t^2$ (metres). Find (a) its greatest height, (b) the horizontal distance travelled before it hits the ground. Give answers to 3 significant figures.

โ–ถ Show solution

(a) $y = -4.9\left(t - \tfrac{10}{9.8}\right)^2 + 1.5 + \dfrac{10^2}{4 \times 4.9}$, so the greatest height is $1.5 + \dfrac{100}{19.6} = 6.60$ m (3 s.f.), at $t \approx 1.02$ s.

(b) $4.9t^2 - 10t - 1.5 = 0 \Rightarrow t = \dfrac{10 + \sqrt{100 + 29.4}}{9.8} = 2.181\ldots$ (the other root is negative).

$x = 15 \times 2.181\ldots = 32.7$ m (3 s.f.).

Question 4

A car drives round a roundabout with $x = 15\cos\left(\dfrac{t}{3}\right)$, $y = 15\sin\left(\dfrac{t}{3}\right)$ (metres, seconds). Find the Cartesian equation of the path and the time for one full circuit.

โ–ถ Show solution

$x^2 + y^2 = 225$: a circle of radius $15$ m centred on the origin.

One circuit when $\tfrac{t}{3} = 2\pi$: $t = 6\pi \approx 18.8$ seconds.

Question 5

A capsule on a big wheel has $x = 60\sin\left(\dfrac{\pi t}{15}\right)$, $y = 65 - 60\cos\left(\dfrac{\pi t}{15}\right)$, with $t$ in minutes and $y$ the height in metres. Find the greatest height, and how long in each revolution the capsule is more than $35$ m above the ground.

โ–ถ Show solution

Greatest height $65 + 60 = 125$ m. One revolution takes $30$ minutes.

$65 - 60\cos\left(\dfrac{\pi t}{15}\right) > 35 \Rightarrow \cos\left(\dfrac{\pi t}{15}\right) < \dfrac12$.

For one revolution: $\dfrac{\pi}{3} < \dfrac{\pi t}{15} < \dfrac{5\pi}{3}$, so $5 < t < 25$.

That is $20$ minutes of each revolution.

Question 6

A stone in a tyre of radius $0.3$ m follows $x = 0.3(\theta - \sin\theta)$, $y = 0.3(1 - \cos\theta)$. Find the horizontal position of the stone when it first reaches a height of $0.45$ m.

โ–ถ Show solution

$0.3(1 - \cos\theta) = 0.45 \Rightarrow \cos\theta = -0.5 \Rightarrow \theta = \dfrac{2\pi}{3}$ (first time).

$x = 0.3\left(\dfrac{2\pi}{3} - \dfrac{\sqrt3}{2}\right) = 0.3(2.0944 - 0.8660) = 0.369$ m (3 s.f.).

Question 7

A stone is thrown with $x = 20t$, $y = 30t - 5t^2$ (metres, seconds). Find the Cartesian equation of its path, and state the values of $x$ for which the model is valid.

โ–ถ Show solution

$t = \tfrac{x}{20}$, so $y = \dfrac{30x}{20} - \dfrac{5x^2}{400} = \dfrac{3x}{2} - \dfrac{x^2}{80}$.

Valid while $y \geqslant 0$: $5t(6 - t) \geqslant 0$, so $0 \leqslant t \leqslant 6$, i.e. $0 \leqslant x \leqslant 120$.

Question 8

Drone P is at $x = 2t$, $y = t + 1$ and drone Q at $x = t + 3$, $y = 3t - 4$, $t$ seconds after launch (in metres, at the same height). Show that their paths cross, and determine whether they collide.

โ–ถ Show solution

P's path: $y = \tfrac{x}{2} + 1$. Q's path: $t = x - 3$, so $y = 3(x - 3) - 4 = 3x - 13$.

Paths meet when $\tfrac{x}{2} + 1 = 3x - 13 \Rightarrow \tfrac52 x = 14 \Rightarrow x = 5.6$, $y = 3.8$.

P reaches $x = 5.6$ at $t = 2.8$; Q reaches $x = 5.6$ at $t = 2.6$.

They are at the crossing point at different times, so they do not collide.

Question 9

A bird flies with $x = 10t$, $y = 20 + 5\sin\left(\dfrac{\pi t}{2}\right)$ (metres, seconds). (a) State its lowest and greatest heights.  (b) Find the Cartesian equation of its path.  (c) Find when and where it first reaches a height of $22.5$ m.

โ–ถ Show solution

(a) $15$ m and $25$ m.

(b) $t = \tfrac{x}{10}$, so $y = 20 + 5\sin\left(\dfrac{\pi x}{20}\right)$.

(c) $5\sin\left(\dfrac{\pi t}{2}\right) = 2.5 \Rightarrow \sin\left(\dfrac{\pi t}{2}\right) = \tfrac12 \Rightarrow \dfrac{\pi t}{2} = \dfrac{\pi}{6} \Rightarrow t = \tfrac13$ s.

Then $x = \tfrac{10}{3} \approx 3.33$ m.

Question 10

A golf ball is struck from ground level. Its position after $t$ seconds is modelled by $x = 30t$, $y = 20t - 4.9t^2$, in metres.

(a) Find the Cartesian equation of the path.  (b) Find the horizontal distance to where the ball lands.  (c) A tree $10$ m tall stands $90$ m away along the line of flight. Does the ball clear it?  (d) Find the greatest height.  (e) State the domain of $t$ for which the model applies, and give one reason why the actual distance might be shorter.

โ–ถ Show solution

(a) $t = \tfrac{x}{30}$: $y = \dfrac{20x}{30} - \dfrac{4.9x^2}{900} = \dfrac{2x}{3} - \dfrac{49x^2}{9000}$.

(b) $y = 0$: $t(20 - 4.9t) = 0 \Rightarrow t = \dfrac{20}{4.9} = 4.08\ldots$ s. Then $x = 30 \times 4.0816\ldots = 122$ m (3 s.f.).

(c) $x = 90$ when $t = 3$: $y = 60 - 4.9 \times 9 = 15.9$ m. That is more than $10$ m, so the ball clears the tree by about $5.9$ m.

(d) $y = -4.9\left(t - \tfrac{20}{9.8}\right)^2 + \dfrac{20^2}{4 \times 4.9}$, so the greatest height is $\dfrac{400}{19.6} = 20.4$ m (3 s.f.), at $t \approx 2.04$ s.

(e) $0 \leqslant t \leqslant \dfrac{20}{4.9}$ (about $4.08$ s), while the ball is in the air. Air resistance, ignored by the model, would slow the ball and reduce the distance.

Parametric Modelling · A Level Maths Year 2 · Created with MathJax