let us describe curves using a third variable, t. This opens up new ways to represent and analyze shapes in the xy-plane, going beyond traditional Cartesian coordinates.
In this section, we'll learn how to define, manipulate, and apply parametric equations. We'll explore their uses in modeling real-world phenomena like cycloids, , and particle trajectories.
Parametric Equations and Curves
Defining Parametric Equations and Curves
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Parametric equations represent a curve in the xy-plane using two equations, x=f(t) and y=g(t), where t is the
The parameter t is an independent variable that determines the position of a point on the curve
As t varies, the point (x,y)=(f(t),g(t)) traces out a in the plane
A parametric curve is a curve in the plane that is defined by parametric equations
The curve is the path traced out by the point (x,y) as the parameter t varies over a given interval
Examples of parametric curves include circles, ellipses, and cycloids
Manipulating Parametric Equations
Eliminating the parameter involves solving the parametric equations for t and substituting one equation into the other to obtain a Cartesian equation in x and y
This process can be used to convert parametric equations into a more familiar form
For example, the parametric equations x=cost and y=sint, 0≤t≤2π, represent a circle with radius 1 centered at the origin
Squaring and adding the equations yields x2+y2=1, the Cartesian equation of the circle
Parametric equations can be manipulated algebraically, such as adding, subtracting, or multiplying the equations, to transform the curve or simplify the equations
These manipulations can help reveal properties of the curve or make it easier to graph
Applications of Parametric Equations
Modeling Cycloids
A is the curve traced by a point on the rim of a circular wheel as the wheel rolls along a straight line without slipping
Parametric equations for a cycloid are x=a(t−sint) and y=a(1−cost), where a is the radius of the wheel
Cycloids have applications in physics, such as modeling the path of a pendulum or the shape of a rope hanging under its own weight (catenary)
Describing Projectile Motion
Projectile motion can be modeled using parametric equations, where x=v0tcosθ and y=v0tsinθ−21gt2
v0 is the initial velocity, θ is the angle of projection, g is the acceleration due to gravity, and t is time
These equations describe the path of a projectile, such as a ball thrown or a bullet fired, assuming no air resistance
The equations can be used to determine the range, height, and time of flight of the projectile
Analyzing Particle Motion
Parametric equations are useful for describing the motion of a particle in the plane
The position of the particle at time t is given by the coordinates (x(t),y(t))
The velocity and acceleration of the particle can be found by differentiating the position equations with respect to t
Parametric equations can model various types of , such as circular motion, harmonic motion, or more complex paths
For example, the equations x=cos(2t) and y=sin(3t) describe a particle moving in a figure-eight pattern, known as a Lissajous curve