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Parametric equations in modellingEdexcel A-Level Maths: Revision notes

Section 1

Parametric models

In modelling, the parameter is often time tt, and the pair x=f(t)x=f(t), y=g(t)y=g(t) gives the position of an object at time tt. This describes a path and also how fast the object moves along it, which a single equation y=f(x)y=f(x) cannot do. Typical questions ask you to:

  • build x(t)x(t) and y(t)y(t) from information in words,
  • find the position at a given time (substitute tt),
  • find the time at which a condition holds (solve for tt, then substitute back),
  • find the Cartesian path by eliminating tt. Always state units, and check that your tt lies in the range where the model applies (for example t≥0t\ge0, or until the ball lands).
Key termsmodelposition vector
Common mistake

Solving for tt and giving it as the final answer when the question asks for coordinates.

Section 2

Constant velocity: straight-line motion

If an object starts at (x0,y0)(x_0,y_0) and moves with constant velocity (u,v)(u,v), then x=x0+ut,y=y0+vt.x=x_0+ut,\qquad y=y_0+vt. Given two positions at two times, find the velocity by dividing the displacement by the time taken. Example: from (1,8)(1,8) at t=0t=0 to (6,20)(6,20) at t=5t=5: the velocity is (55,125)=(1,2.4)\left(\frac55,\frac{12}{5}\right)=(1,2.4), so x=1+tx=1+t, y=8+2.4ty=8+2.4t. The speed is the size of the velocity, u2+v2\sqrt{u^2+v^2}. For (3,6)(3,6) the speed is 45=35\sqrt{45}=3\sqrt5. Constant velocity gives a straight line: eliminating tt gives yy as a linear function of xx.

Key termsvelocityspeeddisplacement
Common mistake

Using the total displacement as the velocity. Divide by the time taken.

Exam tip

Check your equations by substituting the second time and confirming you reach the second point.

Section 3

Projectiles and other curved paths

When the horizontal motion is steady and the vertical motion is accelerated, the model is of the form x=utx=ut, y=vt−12gt2y=vt-\frac12gt^2 (a projectile).

  • The ball lands when y=0y=0: factorise to get t=0t=0 (launch) and the landing time.
  • The greatest height occurs at the midpoint of the two times when y=0y=0, or by completing the square in tt. For y=9t−5t2=−5(t−0.9)2+4.05y=9t-5t^2=-5(t-0.9)^2+4.05 the maximum is 4.054.05 at t=0.9t=0.9.
  • The range is the value of xx at the landing time.
  • Eliminating tt gives the Cartesian path, here a parabola y=34x−5144x2y=\frac34x-\frac{5}{144}x^2. This model ignores air resistance and spin, so real paths fall slightly short.
Key termsprojectilerange
Exam tip

Express a quadratic in tt by completing the square to read off the maximum and when it occurs.

Section 4

Circular and periodic motion

Motion around a circle is modelled with sine and cosine: x=a+rsin⁡(ωt)x=a+r\sin(\omega t), y=b−rcos⁡(ωt)y=b-r\cos(\omega t) describes a point on a circle of radius rr with centre (a,b)(a,b). The period (time for one full revolution) is 2πω\frac{2\pi}{\omega}. For a Ferris wheel seat x=15sin⁡(πt2)x=15\sin\left(\frac{\pi t}{2}\right), y=16−15cos⁡(πt2)y=16-15\cos\left(\frac{\pi t}{2}\right): the radius is 1515 m, the centre is 1616 m above the ground, the period is 44 minutes, the lowest height is 11 m and the greatest is 3131 m. The Cartesian path is x2+(y−16)2=225x^2+(y-16)^2=225. Use the greatest and least values of sin⁡\sin and cos⁡\cos (±1\pm1) to read off extreme values.

Key termsperiodradius
Common mistake

Reading the period as the coefficient of tt. The period is 2πω\frac{2\pi}{\omega}, not ω\omega.

Section 5

Two moving objects: collisions and closest approach

To decide whether two objects collide, they must be at the same place at the same time. Equate the xx-coordinates and solve for tt, then check whether the yy-coordinates agree at that same tt. Two paths can cross without a collision if the objects reach the crossing point at different times. Tug AA reaches (6,5)(6,5) at t=2t=2 while tug BB reaches it at t=4t=4. To find the closest approach, write the vector between the objects, (xB−xA, yB−yA)(x_B-x_A,\ y_B-y_A), form d2=(xB−xA)2+(yB−yA)2d^2=(x_B-x_A)^2+(y_B-y_A)^2, which is quadratic in tt, and find its minimum by completing the square or differentiating. Then square root. For d2=26t2−154t+245d^2=26t^2-154t+245 the minimum is at t=7726t=\frac{77}{26}. Criticise models too: constant velocity ignores acceleration and turning, and treating tugs as points ignores their size.

Key termscollisionclosest approach
Common mistake

Using a different parameter for each object when testing for a collision. They must have the same tt.

That's the notes covered.

Carry on to the next subtopic.

Exam questions on Parametric equations in modelling

  1. A drone moves in a straight line at constant velocity. Relative to a fixed origin it is at the point (2,10)(2,10) when t=0t=0 and at the point (14,34)(14,34) when t=4t=4, where tt is the time in seconds and distances are in metres.
    The drone reaches the line x=20x=20. Find the time at which this happens and the yy-coordinate of the drone at that time.2 marks
  2. A seat on a Ferris wheel moves so that at time tt minutes, t≥0t\ge0, its position is modelled by x=15sin⁡(πt2)x=15\sin\left(\frac{\pi t}{2}\right), y=16−15cos⁡(πt2)y=16-15\cos\left(\frac{\pi t}{2}\right), where xx is the horizontal distance in metres from the vertical line through the centre of the wheel and yy is the height in metres above the ground.
    Find a Cartesian equation for the path of the seat.2 marks
  3. A ball is kicked from the ground at time t=0t=0 seconds. Until it returns to the ground, its position in metres is modelled by x=12tx=12t, y=9t−5t2y=9t-5t^2, where xx is the horizontal distance from the kick and yy is the height above the ground.
    Find the time for which the ball is in the air, and the horizontal distance it travels in this time.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).