1. Parametric Equations Plane Curves

2. Parametric Equations Let x = f(t) and g(t), where f and g are two functions whose common domain is some interval I. The collection of points defined by (x, y) = (f(t), g(t)) is called a plane curve.

3. Parametric Equations The equations x = f(t)y = g(t) where t is in I, are called parametric equations of the curve. The variable t is called a parameter.

4. Parametric Equations Parametric equations are used to describe movement along a curve. Arrows are drawn along the curve in order to show direction or orientation along the curve as t varies from a to b.

5. Discussing a Curve Discuss the curve defined by the parametric equations x = 3t 2 y = 2t -2 ≤ t ≤ 2

6. Graphing Parametric Equations Using a Graphing Calculator 1. Set the mode to PARametric. 2. Enter x(t) and y(t). 3. Select the viewing window. In addition to setting Xmin, Xmax, Xscl, and so on, the viewing window in parametric mode requires values for the parameter t and an increment setting for t (Tstep) 4. Graph

7. Graphing Parametric Equations Using a Graphing Calculator Graph x = 2 cos ty = 3 sin t 0 ≤ t ≤ 

8. Finding the Rectangular Equation of a Curve Find the rectangular equation of the curve whose parametric equations are x = a cos ty = a sin t where a > 0 is a constant.

9. Finding the Rectangular Equation of a Curve When given trig functions, we use the identity cos 2 t + sin 2 t = 1 (x/a) 2 + (y/a) 2 = 1 x 2 + y 2 = a 2 As the parameter t increases, the corresponding points are traced in a counterclockwise direction around the circle.

10. Finding the Rectangular Equation of a Curve If the function is not a trig function: 1. Solve both equations for t 2. Set the two equations equal to each other (transitive property of equality) 3. Solve for y.

11. Projectile Motion We can use parametric equations to describe the motion of an object (curvilinear motion). When an object is propelled upward at an inclination  to the horizontal with initial speed v 0, the resulting motion is called projectile motion.

12. Projectile Motion Parametric equations of a projectile: x = (v 0 cos  )t y = -½gt 2 + (v 0 sin  )t + h where t is the time and g is the constant acceleration due to gravity (32 ft/sec 2 or 9.8 m/sec 2 ).

13. Projectile Motion Examples p. 724 and 725. Talladega 500 example

14. Finding Parametric Equations Find parametric equations for the equation: y = x 2 – 4 Remember there are two equations. Let x = t y = t 2 – 4 (Yes it is that easy)