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Chapter 10: Parametric Equations and Polar
Coordinates
Section 10.1: Curves Defined by Parametric Equations
Alea Wittig
SUNY Albany
Imagine a partical moving across a curve C, which does not pass
the Vertical Line Test.
The x and y coordinates of C are functions of time, t.
Parametric Equations
▶ Suppose x and y are both given as functions of third variable
t, called a parameter, by equations
x = f (t) y = g(t)
called parametric equations.
▶ As t varies, the point
(x, y) = (f (t), g(t))
varies and traces out a curve C called a parametric curve.
▶ Note: t does not always represent time.
Example 1
1/4
Sketch and identify the curve defined by the parametric equations
x = t2
− 2t y = t + 1
Example 1
2/4
▶ We start by making a table of points corresponding to
t = −2, −1, 0, 1, 2, 3, 4, . . .
▶ Choose both negative and positive values of t.
▶ Choosing integers for t also makes the computation of x and y
easier.
t x = t2 − 2t y = t + 1
−2 8 −1
−1 3 0
0 0 1
1 −1 2
2 0 3
3 3 4
4 8 5
Example 1
3/4
▶ Now we can plot points.
▶ Then connect the points
starting at t = 2 and
ending at t = 4
▶ We mark the curve with
arrows to show the
direction.
▶ One of the key differences
between a parametric curve
and a cartesian curve is
that parametric curves have
direction.
Example 1
4/4
▶ We notice that the curve looks like a transformation of the
curve y = ±
√
x
▶ Let’s check this by first solving for t in terms of y:
y = t + 1 =⇒ t = y − 1
▶ Then plugging this into the equation for x to eliminate the
parameter t:
x = t2
− 2t
= (y − 1)2
− 2(y − 1)
= y2
− 2y + 1 − 2y + 2
= y2
− 4y + 3
= (y − 2)2
− 1 =⇒
y = 2 ±
√
x + 1 ✓
Eliminating the Parameter
▶ The process used in example 1 to find a Cartesian equation in
x and y is called eliminating the parameter.
▶ In this process we are able to see the shape of the curve but
we lose information:
▶ where the particle is at any given time
▶ direction of motion
Restrictions on the Parameter
▶ Some parametric curves/equations may also have a restriction
on parameter t.
eg x = t2
− 2t, y = t + 1 for 0 ≤ t ≤ 2
is the parabola in Ex 1 that starts at (0, 1) and ends at (0, 3)
▶ In general, the curve with parametric equations
x = f (t) y = g(t) a ≤ t ≤ b
has initial point (f (a), g(a)) and terminal point
(f (b), g(b)).
Example 2
1/3
What curve is represented by the following parametric equations?
x = cos t y = sin t 0 ≤ t ≤ 2π
Example 2
2/3
t x = cos t y = sin t
0 1 0
π
6
√
3
2
1
2
π
4
√
2
2
√
2
2
π
3
1
2
√
3
2
π
2 0 1
.
.
.
.
.
.
.
.
.
π −1 0
.
.
.
.
.
.
.
.
.
3π
2 0 −1
.
.
.
.
.
.
.
.
.
2π 1 0
▶ We start by making a table
of points corresponding to
t = 0, π
6 , π
4 , π
3 , π
2 , . . . 2π
▶ We choose values of t that
will make computing x and
y easy.
▶ Initial point (1, 0)
▶ Terminal point (1, 0)
Example 2
3/3
▶ Plotting the points we have what appears to be the unit circle,
traversed counterclockwise one time.
▶ We can verify this by eliminating the parameter
▶ Using the trig identity we have:
cos2
θ + sin2
θ = 1
=⇒ x2
+ y2
= 1 ✓
Example 3
1/4
What curve is represented by the following parametric equations?
x = sin 2t y = cos 2t 0 ≤ t ≤ 2π
Example 3
2/4
▶ Again using the trig identity
cos2
θ + sin2
θ = 1 for all θ
=⇒ cos2
(2t) + sin2
(2t) = 1 for all t
=⇒ y2
+ x2
= 1
▶ So the curve represented is the unit circle but let’s investigate
this more:
▶ cos (2t) and sin (2t) each complete one full period from t = 0
to t = π.
▶ They complete two periods from t = 0 to t = 2π so the circle
is traversed twice.
▶ Initial point is
t = 0; x = sin 0 = 0, y = cos 0 = 1, → (0, 1)
▶ Terminal point is
t = 2π; x = sin 4π = 0, y = cos 4π = 1, → (0, 1)
Example 3
3/4
▶ Plotting a few values for t: t = 0, π
6 , π
4 , π
3 , π
2 , we see that
the circle is being traversed clockwise.
t 2t x = sin 2t y = cos 2t
0 0 0 1
π
6
π
3
√
3
2
1
2
π
4
π
2 1 0
π
3
2π
3
√
3
2 −1
2
π
2 π 0 −1
Example 3
4/4
▶ So the curve represented by parametric equations
x = sin 2t y = cos 2t 0 ≤ t ≤ 2π
is the unit circle traversed clockwise two times with initial and
terminal point (0, 1).
Example 4
1/5
Each of the following parametric equations has the Cartesian
equation x = y3. Graph the curve.
(a) x = t3, y = t
(b) x = −t3, y = −t
(c) x = t3/2, y =
√
t
(d) x = e−3t, y = e−t
Example 4
2/5
(a) x = t3, y = t
▶ Clearly x = y3.
▶ Plotting some points:
t x y
−2 −8 −2
−1 −1 −1
0 0 0
1 1 1
2 8 2
▶ The curve is traversed left
to right.
Example 4
3/5
(b) x = −t3, y = −t
▶ x = −t3 = (−t)3 = y3.
▶ Plotting some points:
t x y
−2 8 2
−1 1 1
0 0 0
1 −1 −1
2 −8 −2
▶ The curve is traversed from
right to left.
Example 4
4/5
(c) x = t3/2, y =
√
t
▶ Clearly x = y3.
▶ Plotting some points:
t x y
−2 undef undef
−1 undef undef
0 0 0
1 1 1
2
√
8
√
2
▶ traversed from left to right.
▶ not defined for t < 0.
▶ x ≥ 0 and y ≥ 0 for all
values of t.
Example 4
5/5
(d) x = e−3t, y = e−t
▶ Clearly x = y3.
▶ Plotting some points:
t x y
−2 e6 e2
−1 e3 e
0 1 1
1 1 1
2 1
e6
1
e2
▶ The curve is traversed from
right to left.
▶ x > 0 and y > 0 for all
values of t.

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Section 10.1

  • 1. Chapter 10: Parametric Equations and Polar Coordinates Section 10.1: Curves Defined by Parametric Equations Alea Wittig SUNY Albany
  • 2. Imagine a partical moving across a curve C, which does not pass the Vertical Line Test. The x and y coordinates of C are functions of time, t.
  • 3. Parametric Equations ▶ Suppose x and y are both given as functions of third variable t, called a parameter, by equations x = f (t) y = g(t) called parametric equations. ▶ As t varies, the point (x, y) = (f (t), g(t)) varies and traces out a curve C called a parametric curve. ▶ Note: t does not always represent time.
  • 4. Example 1 1/4 Sketch and identify the curve defined by the parametric equations x = t2 − 2t y = t + 1
  • 5. Example 1 2/4 ▶ We start by making a table of points corresponding to t = −2, −1, 0, 1, 2, 3, 4, . . . ▶ Choose both negative and positive values of t. ▶ Choosing integers for t also makes the computation of x and y easier. t x = t2 − 2t y = t + 1 −2 8 −1 −1 3 0 0 0 1 1 −1 2 2 0 3 3 3 4 4 8 5
  • 6. Example 1 3/4 ▶ Now we can plot points. ▶ Then connect the points starting at t = 2 and ending at t = 4 ▶ We mark the curve with arrows to show the direction. ▶ One of the key differences between a parametric curve and a cartesian curve is that parametric curves have direction.
  • 7. Example 1 4/4 ▶ We notice that the curve looks like a transformation of the curve y = ± √ x ▶ Let’s check this by first solving for t in terms of y: y = t + 1 =⇒ t = y − 1 ▶ Then plugging this into the equation for x to eliminate the parameter t: x = t2 − 2t = (y − 1)2 − 2(y − 1) = y2 − 2y + 1 − 2y + 2 = y2 − 4y + 3 = (y − 2)2 − 1 =⇒ y = 2 ± √ x + 1 ✓
  • 8. Eliminating the Parameter ▶ The process used in example 1 to find a Cartesian equation in x and y is called eliminating the parameter. ▶ In this process we are able to see the shape of the curve but we lose information: ▶ where the particle is at any given time ▶ direction of motion
  • 9. Restrictions on the Parameter ▶ Some parametric curves/equations may also have a restriction on parameter t. eg x = t2 − 2t, y = t + 1 for 0 ≤ t ≤ 2 is the parabola in Ex 1 that starts at (0, 1) and ends at (0, 3) ▶ In general, the curve with parametric equations x = f (t) y = g(t) a ≤ t ≤ b has initial point (f (a), g(a)) and terminal point (f (b), g(b)).
  • 10. Example 2 1/3 What curve is represented by the following parametric equations? x = cos t y = sin t 0 ≤ t ≤ 2π
  • 11. Example 2 2/3 t x = cos t y = sin t 0 1 0 π 6 √ 3 2 1 2 π 4 √ 2 2 √ 2 2 π 3 1 2 √ 3 2 π 2 0 1 . . . . . . . . . π −1 0 . . . . . . . . . 3π 2 0 −1 . . . . . . . . . 2π 1 0 ▶ We start by making a table of points corresponding to t = 0, π 6 , π 4 , π 3 , π 2 , . . . 2π ▶ We choose values of t that will make computing x and y easy. ▶ Initial point (1, 0) ▶ Terminal point (1, 0)
  • 12. Example 2 3/3 ▶ Plotting the points we have what appears to be the unit circle, traversed counterclockwise one time. ▶ We can verify this by eliminating the parameter ▶ Using the trig identity we have: cos2 θ + sin2 θ = 1 =⇒ x2 + y2 = 1 ✓
  • 13. Example 3 1/4 What curve is represented by the following parametric equations? x = sin 2t y = cos 2t 0 ≤ t ≤ 2π
  • 14. Example 3 2/4 ▶ Again using the trig identity cos2 θ + sin2 θ = 1 for all θ =⇒ cos2 (2t) + sin2 (2t) = 1 for all t =⇒ y2 + x2 = 1 ▶ So the curve represented is the unit circle but let’s investigate this more: ▶ cos (2t) and sin (2t) each complete one full period from t = 0 to t = π. ▶ They complete two periods from t = 0 to t = 2π so the circle is traversed twice. ▶ Initial point is t = 0; x = sin 0 = 0, y = cos 0 = 1, → (0, 1) ▶ Terminal point is t = 2π; x = sin 4π = 0, y = cos 4π = 1, → (0, 1)
  • 15. Example 3 3/4 ▶ Plotting a few values for t: t = 0, π 6 , π 4 , π 3 , π 2 , we see that the circle is being traversed clockwise. t 2t x = sin 2t y = cos 2t 0 0 0 1 π 6 π 3 √ 3 2 1 2 π 4 π 2 1 0 π 3 2π 3 √ 3 2 −1 2 π 2 π 0 −1
  • 16. Example 3 4/4 ▶ So the curve represented by parametric equations x = sin 2t y = cos 2t 0 ≤ t ≤ 2π is the unit circle traversed clockwise two times with initial and terminal point (0, 1).
  • 17. Example 4 1/5 Each of the following parametric equations has the Cartesian equation x = y3. Graph the curve. (a) x = t3, y = t (b) x = −t3, y = −t (c) x = t3/2, y = √ t (d) x = e−3t, y = e−t
  • 18. Example 4 2/5 (a) x = t3, y = t ▶ Clearly x = y3. ▶ Plotting some points: t x y −2 −8 −2 −1 −1 −1 0 0 0 1 1 1 2 8 2 ▶ The curve is traversed left to right.
  • 19. Example 4 3/5 (b) x = −t3, y = −t ▶ x = −t3 = (−t)3 = y3. ▶ Plotting some points: t x y −2 8 2 −1 1 1 0 0 0 1 −1 −1 2 −8 −2 ▶ The curve is traversed from right to left.
  • 20. Example 4 4/5 (c) x = t3/2, y = √ t ▶ Clearly x = y3. ▶ Plotting some points: t x y −2 undef undef −1 undef undef 0 0 0 1 1 1 2 √ 8 √ 2 ▶ traversed from left to right. ▶ not defined for t < 0. ▶ x ≥ 0 and y ≥ 0 for all values of t.
  • 21. Example 4 5/5 (d) x = e−3t, y = e−t ▶ Clearly x = y3. ▶ Plotting some points: t x y −2 e6 e2 −1 e3 e 0 1 1 1 1 1 2 1 e6 1 e2 ▶ The curve is traversed from right to left. ▶ x > 0 and y > 0 for all values of t.