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Parametric modelling

A parametric model describes two or more related quantities using a third quantity called a parameter. It is especially useful when position changes with time, when a curve is easier to trace than to write as y=f(x)y=f(x), or when one Cartesian equation would hide direction and restrictions.

For example,

x=3t+1,y=2t4x=3t+1,\qquad y=2t-4

describes a moving point. At t=0t=0 it is at (1,4)(1,-4), and each increase of one in tt moves it 33 units right and 22 units up.

This lesson focuses on building and evaluating models. Review parametric equations for the underlying notation and algebra.

By the end of this lesson, you should be able to:

  • choose a meaningful parameter;
  • construct parametric equations from geometry or motion;
  • interpret the parameter, its units and its domain;
  • identify direction and starting position;
  • eliminate the parameter when useful;
  • distinguish a full Cartesian curve from the part traced by a model;
  • test a model against data, assumptions and physical constraints.

A two-dimensional parametric model has the form

x=f(t),y=g(t),tD,x=f(t),\qquad y=g(t),\qquad t\in D,

where DD is the permitted domain of the parameter.

The model contains three different kinds of information:

  1. Path: the set of points (x,y)(x,y) that can be reached.
  2. Direction: the order in which those points are traced as tt increases.
  3. Timing: if tt represents time, how quickly the point moves along the path.

A Cartesian equation such as y=2x6y=2x-6 gives the path, but it usually does not preserve direction or timing.

Consider

x=1+4t,y=52t,0t3.x=1+4t,\qquad y=5-2t,\qquad 0\leq t\leq3.

At the endpoints,

t=0:(x,y)=(1,5),t=0:(x,y)=(1,5), t=3:(x,y)=(13,1).t=3:(x,y)=(13,-1).

As tt increases, xx increases and yy decreases. The model traces the line segment from (1,5)(1,5) towards (13,1)(13,-1).

Eliminating tt gives

t=x14t=\frac{x-1}{4}

and hence

y=52(x14)=112x2.y=5-2\left(\frac{x-1}{4}\right) =\frac{11}{2}-\frac{x}{2}.

However, the model does not trace the whole line. Since 0t30\leq t\leq3,

1x13.1\leq x\leq13.

The parameter domain is part of the answer, not an optional note.

A useful parameter should simplify the relationships and, where possible, have a clear interpretation.

Common choices include:

  • time tt for motion;
  • an angle θ\theta for circles and periodic motion;
  • distance travelled ss along a straight path;
  • a dimension such as radius rr in a changing geometric shape;
  • a dimensionless proportion uu with 0u10\leq u\leq1 between two endpoints.

The parameter need not be tt. Its symbol should match its meaning.

Let A=(2,1)A=(2,-1) and B=(8,11)B=(8,11). A point moving from AA to BB can be modelled using a proportion uu:

x=2+u(82)=2+6u,y=1+u(11(1))=1+12u,0u1.\begin{aligned} x&=2+u(8-2)=2+6u,\\ y&=-1+u(11-(-1))=-1+12u, \end{aligned} \qquad 0\leq u\leq1.

At u=0u=0, the point is at AA. At u=1u=1, it is at BB. At u=1/2u=1/2, it is halfway between them:

(x,y)=(5,5).(x,y)=(5,5).

This construction generalises. For points A=(x1,y1)A=(x_1,y_1) and B=(x2,y2)B=(x_2,y_2),

x=x1+u(x2x1),y=y1+u(y2y1),0u1.x=x_1+u(x_2-x_1),\qquad y=y_1+u(y_2-y_1),\qquad 0\leq u\leq1.

For motion at constant velocity, position equals initial position plus velocity multiplied by time.

If an object starts at (x0,y0)(x_0,y_0) and has constant velocity (vx,vy)(v_x,v_y), then

x=x0+vxt,y=y0+vyt.\boxed{x=x_0+v_xt,\qquad y=y_0+v_yt.}

A boat starts at the point (4,7)(4,7) km relative to a harbour and travels with velocity

(62) km h1.\begin{pmatrix}6\\-2\end{pmatrix} \text{ km h}^{-1}.

After tt hours its position is

x=4+6t,y=72t,x=4+6t,\qquad y=7-2t,

with t0t\geq0 while the velocity remains valid.

After 1.51.5 hours,

x=4+6(1.5)=13,x=4+6(1.5)=13, y=72(1.5)=4.y=7-2(1.5)=4.

The boat is at (13,4)(13,4) km.

To eliminate tt,

t=x46,t=\frac{x-4}{6},

so

y=72(x46)=25x3.y=7-2\left(\frac{x-4}{6}\right) =\frac{25-x}{3}.

This Cartesian equation identifies the route, but only the parametric model says that the boat starts at (4,7)(4,7) and moves in the direction (6,2)(6,-2) at the stated rate.

In

x=x0+vxt,x=x_0+v_xt,

the units must be consistent:

km=km+(km h1)(h).\text{km}=\text{km}+(\text{km h}^{-1})(\text{h}).

If the units do not balance, the model is wrong or incompletely converted.

A circle with centre (a,b)(a,b) and radius rr has the parametrisation

x=a+rcosθ,y=b+rsinθ.\boxed{x=a+r\cos\theta,\qquad y=b+r\sin\theta.}

The identity cos2θ+sin2θ=1\cos^2\theta+\sin^2\theta=1 confirms that

(xa)2+(yb)2=r2.(x-a)^2+(y-b)^2=r^2.

For 0θ2π0\leq\theta\leq2\pi, the point starts at (a+r,b)(a+r,b) and traces the circle anticlockwise once. Replacing sinθ\sin\theta by sinθ-\sin\theta reverses the direction.

A passenger moves on a wheel of radius 1010 m whose centre is (0,12)(0,12). Suppose the passenger starts at the lowest point and moves anticlockwise. One suitable model is

x=10sinθ,y=1210cosθ.x=10\sin\theta,\qquad y=12-10\cos\theta.

At θ=0\theta=0,

(x,y)=(0,2),(x,y)=(0,2),

the lowest point. At θ=π/2\theta=\pi/2,

(x,y)=(10,12).(x,y)=(10,12).

If only the first quarter-turn is being modelled, the correct domain is

0θπ2.0\leq\theta\leq\frac{\pi}{2}.

The full circle equation alone would incorrectly include positions outside the stated interval of motion.

An ellipse centred at (a,b)(a,b) with horizontal semi-axis pp and vertical semi-axis qq can be modelled by

x=a+pcost,y=b+qsint.x=a+p\cos t,\qquad y=b+q\sin t.

Eliminating tt gives

(xa)2p2+(yb)2q2=1.\frac{(x-a)^2}{p^2}+\frac{(y-b)^2}{q^2}=1.

For example,

x=3+5cost,y=2+2sintx=3+5\cos t,\qquad y=-2+2\sin t

has centre (3,2)(3,-2), horizontal semi-axis 55 and vertical semi-axis 22.

The same path can be traced with different timing.

Compare

A:quadx=cost,y=sint\mathcal A:quad x=\cos t,\qquad y=\sin t

with

B:quadx=cos(3t),y=sin(3t).\mathcal B:quad x=\cos(3t),\qquad y=\sin(3t).

Both trace the unit circle anticlockwise. Model B\mathcal B completes a revolution three times as quickly because its angular displacement is 3t3t.

Now compare

C:quadx=cost,y=sint.\mathcal C:quad x=\cos t,\qquad y=-\sin t.

It traces the same circle clockwise. Eliminating the parameter from all three models gives x2+y2=1x^2+y^2=1, so Cartesian conversion loses timing and direction.

If the parameter is time, the velocity components are

dxdtanddydt.\frac{dx}{dt}\quad\text{and}\quad\frac{dy}{dt}.

The speed is

(dxdt)2+(dydt)2.\sqrt{\left(\frac{dx}{dt}\right)^2+ \left(\frac{dy}{dt}\right)^2}.

These derivatives are developed fully in parametric differentiation.

Converting between parametric and Cartesian forms

Section titled “Converting between parametric and Cartesian forms”

Eliminating the parameter can reveal the familiar shape, make intersections easier to find, or allow comparison with another curve. It must be done without losing restrictions.

Example: a parabola with restricted motion

Section titled “Example: a parabola with restricted motion”

Let

x=2t+1,y=t24,qquad1t3.x=2t+1,\qquad y=t^2-4,qquad -1\leq t\leq3.

From the first equation,

t=x12.t=\frac{x-1}{2}.

Substitution gives

y=(x12)24=(x1)244.y=\left(\frac{x-1}{2}\right)^2-4 =\frac{(x-1)^2}{4}-4.

Since 1t3-1\leq t\leq3 and x=2t+1x=2t+1 increases with tt,

1x7.-1\leq x\leq7.

The Cartesian model is therefore

y=(x1)244,qquad1x7,y=\frac{(x-1)^2}{4}-4,qquad -1\leq x\leq7,

traced from left to right.

Consider

x=t2,y=t3.x=t^2,\qquad y=t^3.

Then

y2=t6=x3,y^2=t^6=x^3,

so the Cartesian equation is

y2=x3.y^2=x^3.

Writing t=xt=\sqrt{x} would silently assume t0t\geq0 and lose the lower branch where t<0t<0 and y<0y<0. Squaring can also introduce points unless restrictions are checked. Always test the converted equation against the original parametrisation.

A simplified model places a ball at

x=12t,x=12t, y=1+18t5t2,y=1+18t-5t^2,

where tt is measured in seconds and distances in metres.

Interpret the constants:

  • x(0)=0x(0)=0 and y(0)=1y(0)=1, so the initial position is (0,1)(0,1);
  • horizontal position increases at 1212 m s1^{-1};
  • the vertical model initially rises because the coefficient of tt is positive;
  • the negative t2t^2 term eventually makes the height decrease.

The physical domain ends when the ball reaches the ground, not when the algebraic formula ceases to exist. Set y=0y=0:

1+18t5t2=0.1+18t-5t^2=0.

Thus

t=18±182+2010=9±221.55.t=\frac{18\pm\sqrt{18^2+20}}{10} =\frac{9\pm2\sqrt{21.5}}{5}.

Only the positive root is physically meaningful, approximately

t=3.65 s.t=3.65\text{ s}.

The model domain is therefore approximately

0t3.65.0\leq t\leq3.65.

Eliminating tt using t=x/12t=x/12 gives

y=1+32x5144x2,y=1+\frac32x-\frac{5}{144}x^2,

with the corresponding horizontal restriction

0x43.8.0\leq x\lesssim43.8.

The quadratic continues below ground level, but that part of the graph is not part of the flight model.

A mathematical formula is not automatically a good model. State what has been simplified and decide where the simplification is reasonable.

For the flight model above, possible assumptions include:

  • constant gravitational acceleration;
  • negligible air resistance and wind;
  • motion in a vertical plane;
  • no spin or lift;
  • flat ground at y=0y=0;
  • a point-like ball;
  • accurate initial position and velocity.

These assumptions limit the model. Air resistance may make horizontal speed decrease, wind may move the ball sideways, and uneven ground changes the landing condition.

Ask five questions.

State what xx, yy and the parameter represent, including units.

A model of a journey may apply only between departure and arrival. A model of height must not be interpreted after impact.

Check the start, end and one or more intermediate values. For periodic models, check quarter-turns or half-turns.

Do not add metres to metres per second. Check whether computed sizes are plausible.

Identify effects that the formula does not represent and explain how they might affect predictions.

Suppose two cyclists have positions

A:quadx=2+5t,y=1+2tA:quad x=2+5t,\qquad y=1+2t

and

B:quadx=14t,y=7,B:quad x=14-t,\qquad y=7,

where tt is in hours.

They meet only if both coordinates agree at the same time. From the yy coordinates,

1+2t=7,1+2t=7,

so t=3t=3. At this time,

xA=2+5(3)=17,x_A=2+5(3)=17,

but

xB=143=11.x_B=14-3=11.

They do not meet. Their Cartesian paths might intersect at different times, but simultaneous position requires one common parameter value satisfying every coordinate equation.

  • Omitting the domain: the equations and the parameter interval together define the model.
  • Treating the parameter as an axis: tt controls both coordinates but is not normally plotted as a third axis in a plane curve.
  • Assuming tt always means time: it may represent angle, distance or a dimensionless proportion.
  • Finding a Cartesian curve and claiming equivalence: conversion can lose direction, timing, repeated tracing and restrictions.
  • Choosing both square-root signs carelessly: recovering tt from t2=xt^2=x requires attention to the original domain.
  • Confusing path intersection with collision: moving objects collide only if they occupy the same point at the same time.
  • Extending a physical model indefinitely: a formula may remain algebraically valid after its assumptions have failed.
  • Ignoring units: inconsistent units expose an invalid construction.
  • Describing limitations vaguely: say which assumption fails and how that could change the prediction.

A particle has position

x=73t,y=2+4t,qquad0t5.x=7-3t,\qquad y=2+4t,qquad 0\leq t\leq5.

Find its starting point, endpoint and direction of travel.

Answer

At t=0t=0, the particle is at (7,2)(7,2). At t=5t=5, it is at

(715,2+20)=(8,22).(7-15,2+20)=(-8,22).

As tt increases, xx decreases and yy increases, so it travels left and upwards from (7,2)(7,2) to (8,22)(-8,22).

Eliminate tt from

x=3t2,y=t2+1,qquad0t4.x=3t-2,\qquad y=t^2+1,qquad 0\leq t\leq4.
Answer

Since

t=x+23,t=\frac{x+2}{3},

we obtain

y=(x+23)2+1.y=\left(\frac{x+2}{3}\right)^2+1.

The domain 0t40\leq t\leq4 gives

2x10.-2\leq x\leq10.

The curve is traced from left to right.

Construct a parametric model for the line segment from P=(3,4)P=(-3,4) to Q=(5,2)Q=(5,-2).

Answer

Using 0u10\leq u\leq1,

x=3+u(5(3))=3+8u,x=-3+u(5-(-3))=-3+8u, y=4+u(24)=46u.y=4+u(-2-4)=4-6u.

Describe

x=4+3cost,y=13sint,qquad0tπ.x=4+3\cos t,\qquad y=1-3\sin t,qquad 0\leq t\leq\pi.
Answer

The path lies on the circle

(x4)2+(y1)2=9.(x-4)^2+(y-1)^2=9.

It starts at (7,1)(7,1) when t=0t=0, passes through (4,2)(4,-2) when t=π/2t=\pi/2, and ends at (1,1)(1,1) when t=πt=\pi. It traces the lower semicircle clockwise.

Explain one difference between

x=2cost,y=2sintx=2\cos t,\quad y=2\sin t

and

x=2cos(4t),y=2sin(4t).x=2\cos(4t),\quad y=2\sin(4t).
Answer

Both trace the circle x2+y2=4x^2+y^2=4 anticlockwise. If tt is time, the second model travels around the circle four times as quickly. Over the same parameter interval, it may also trace the circle more times.

A height is modelled by

h=2+14t4.9t2.h=2+14t-4.9t^2.

Why is t0t\geq0 alone an inadequate model domain?

Answer

The formula eventually gives negative heights. If the object lands when h=0h=0, the domain should end at the positive solution of

2+14t4.9t2=0.2+14t-4.9t^2=0.

The exact endpoint depends on the physical event being modelled, but values after impact should not be included without a new model.

7. Distinguish intersection from collision

Section titled “7. Distinguish intersection from collision”

Two particles move according to

A:quadx=t,y=t2A:quad x=t,\quad y=t^2

and

B:quadx=2s,y=1,B:quad x=2-s,\quad y=1,

where both parameters measure time from the same starting instant. What must be true for a collision?

Answer

The particles must have the same coordinates at the same time, so set s=ts=t and solve

t=2t,t=2-t, t2=1.t^2=1.

The first equation gives t=1t=1, which also satisfies t2=1t^2=1. Therefore they collide at (1,1)(1,1) at time 11, provided t=1t=1 lies in both model domains.

Merely finding an intersection between the two Cartesian paths would not be sufficient.

Use parametric equations to strengthen conversion and curve interpretation. Then study parametric differentiation to find gradients, tangents, stationary points, velocity and speed directly from a parametric model.