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Modelling with Parametric Equations Simplified Revision Notes

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9.2.3 Modelling with Parametric Equations

Modelling with parametric equations involves representing real-world scenarios where the relationships between variables are best described using a third parameter. This method is particularly useful in situations where the motion or path of an object is considered over time, or when dealing with curves that are difficult to describe with a single function in Cartesian coordinates.

1. Understanding Parametric Equations

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Parametric equations define both xx and yy coordinates as functions of a third variable, often denoted as tt (which could represent time, angle, or another variable):

x=f(t),y=g(t)x = f(t), \quad y = g(t)

Here, tt is the parameter, and as tt changes, the coordinates x(t),y(t)x(t), y(t) trace out a curve in the plane.

2. Applications and Modelling Scenarios

a) Projectile Motion

Projectile motion is a classic example where parametric equations are used to model the path of an object under the influence of gravity.

Scenario: A projectile is launched with an initial velocity v0v_0 at an angle θ\theta to the horizontal. The goal is to model its trajectory.

Equations:

  • Horizontal Motion:

x(t)=v0cos(θ)tx(t) = v_0 \cos(\theta) \cdot t

This describes the horizontal distance travelled over time tt, where v0cos(θ)v_0 \cos(\theta) is the horizontal component of the initial velocity.

  • Vertical Motion:

y(t)=v0sin(θ)t12gt2y(t) = v_0 \sin(\theta) \cdot t - \frac{1}{2}gt^2

This describes the height over time, where v0sin(θ)v_0 \sin(\theta) is the vertical component of the initial velocity, and gg is the acceleration due to gravity. Interpretation:

  • x(t)x(t) and y(t)y(t) together define the position of the projectile at any time tt.
  • The resulting curve is a parabola, and the maximum height and range can be found by analysing these equations.
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📑Example Problem: Find the maximum height reached by a projectile launched with an initial velocity of 20 m/s at an angle of 30°.

Solution:

  • Horizontal component: x(t)=20cos(30)t=103tx(t) = 20 \cos(30^\circ) \cdot t = 10\sqrt{3} \cdot t
  • Vertical component: y(t)=20sin(30)t12×9.8×t2=10t4.9t2y(t) = 20 \sin(30^\circ) \cdot t - \frac{1}{2} \times 9.8 \times t^2 = 10t - 4.9t^2 To find the maximum height, set dydt=0\frac{dy}{dt} = 0 and solve for tt:

dydt=109.8t=0t=109.8:highlight[1.02seconds]\frac{dy}{dt} = 10 - 9.8t = 0 \quad \Rightarrow \quad t = \frac{10}{9.8} \approx :highlight[1.02 seconds]

Substitute t=1.02t = 1.02 into y(t)y(t):

y(1.02)=10(1.02)4.9(1.02)2:highlight[5.10metres]y(1.02) = 10(1.02) - 4.9(1.02)^2 \approx :highlight[5.10 metres]

The maximum height reached by the projectile is approximately 5.10 metres.

b) Circular Motion

Parametric equations are also ideal for modelling circular or elliptical motion, which is common in physics and engineering.

Scenario: A point moves in a circular path with radius rr, centred at the origin, as time progresses.

Equations:

  • Horizontal Component:

x(t)=rcos(ωt)x(t) = r \cos(\omega t)

Here, ω\omega is the angular velocity.

  • Vertical Component:

y(t)=rsin(ωt)y(t) = r \sin(\omega t)

Interpretation:

  • x(t)x(t) and y(t)y(t) together describe the coordinates of a point moving in a circle.
  • The parameter tt typically represents time, and ω\omega dictates the speed at which the point travels around the circle.
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📑Example Problem: A point moves in a circle of radius 5 units with an angular velocity of 2 radians per second. Find the position of the point at t=π2t = \frac{\pi}{2} seconds.

Solution:

  • x(t)=5cos(2t)x(t) = 5 \cos(2t)
  • y(t)=5sin(2t)y(t) = 5 \sin(2t) At t=π2t = \frac{\pi}{2} :

x(π2)=5cos(2×π2)=5cos(π)=5x\left(\frac{\pi}{2}\right) = 5 \cos\left(2 \times \frac{\pi}{2}\right) = 5 \cos(\pi) = -5

y(π2)=5sin(2×π2)=5sin(π)=0y\left(\frac{\pi}{2}\right) = 5 \sin\left(2 \times \frac{\pi}{2}\right) = 5 \sin(\pi) = 0

The position of the point at t=π2t = \frac{\pi}{2} seconds is (-5, 0).

c) Ellipse

Elliptical motion, such as planetary orbits, can also be modelled with parametric equations.

Scenario: A point moves along an elliptical path where the semi-major axis is aa and the semi-minor axis is bb.

Equations:

  • Horizontal Component:

x(t)=acos(t)x(t) = a \cos(t)

  • Vertical Component:

y(t)=bsin(t)y(t) = b \sin(t)

Interpretation:

  • The curve is an ellipse centred at the origin, with axes lengths determined by aa and bb.
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📑Example Problem: Model the orbit of a planet with a semi-major axis of 10 units and a semi-minor axis of 6 units.

Solution:

  • x(t)=10cos(t)x(t) = 10 \cos(t)
  • y(t)=6sin(t)y(t) = 6 \sin(t) This set of equations models the elliptical orbit of the planet.

3. Summary

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Modelling with parametric equations is a powerful technique for describing motion and curves in various applications:

  • Projectile motion: Captures the trajectory of an object under gravity.
  • Circular and elliptical motion: Describes the movement of objects in orbits or rotations.
  • Complex curves: Parametric equations allow the representation of curves that are difficult or impossible to describe with a single Cartesian equation.
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