10.4 Polar Coordinates: Graphs (Interactive)
The planets move through space in elliptical, periodic orbits about the sun, as shown in Figure 1. They are in constant motion, so fixing an exact position of any planet is valid only for a moment. In other words, we can fix only a planet’s instantaneous position. This is one application of polar coordinates, represented as \((r,\theta).\) We interpret \(r\) as the distance from the center of the sun and \(\theta\) as the planet’s angular bearing, or its direction from the center of the sun. In this section, we will focus on the polar system and the graphs that are generated directly from polar coordinates.

Figure 1 Planets follow elliptical paths as they orbit around the Sun. (credit: modification of work by NASA/JPL-Caltech)
10.4.1 Testing Polar Equations for Symmetry
Just as a rectangular equation such as \(y = x^{2}\) describes the relationship between \(x\) and \(y\) on a Cartesian grid, a polar equation describes a relationship between \(r\) and \(\theta\) on a polar grid. Recall that the coordinate pair \((r,\theta)\) indicates that we move counterclockwise from the polar axis (positive \(x\)-axis) by an angle of \(\theta,\) and extend a ray from the pole (origin) \(r\) units in the direction of \(\theta.\) All points that satisfy the polar equation are on the graph.
Symmetry is a property that helps us recognize and plot the graph of any equation. If an equation has a graph that is symmetric with respect to an axis, it means that if we folded the graph in half over that axis, the portion of the graph on one side would coincide with the portion on the other side. By performing three tests, we will see how to apply the properties of symmetry to polar equations. Further, we will use symmetry (in addition to plotting key points, zeros, and maximums of \(\left. r \right)\) to determine the graph of a polar equation.
In the first test, we consider symmetry with respect to the line \(\theta = \frac{\pi}{2}\) (\(y\)-axis). We replace \((r,\theta)\) with \((-r, - \theta)\) to determine if the new equation is equivalent to the original equation. For example, suppose we are given the equation \(r = 2\sin\;\theta;\)
\[\begin{array}{ll} {r = 2\sin\;\theta} & \\ {-r = 2\sin(-\theta)\begin{array}{llll} & & & \end{array}} & {\text{Replace}\;(r,\theta)\;\text{with~}(-r,-\theta).} \\ {-r = -2\sin\;\theta} & {\text{Identity:~}\sin(-\theta) = -\sin\;\theta.} \\ {r = 2\sin\;\theta} & {\text{Multiply~both~sides~by}-1.} \end{array}\]
This equation exhibits symmetry with respect to the line \(\theta = \frac{\pi}{2}.\)
In the second test, we consider symmetry with respect to the polar axis ( \(x\)-axis). We replace \((r,\theta)\) with \(\left( {r, - \theta} \right)\) or \(\left( {- r,\pi - \theta} \right)\) to determine equivalency between the tested equation and the original. For example, suppose we are given the equation \(r = 1 - 2\cos\;\theta.\)
\[\begin{array}{ll} {r = 1 - 2\cos\;\theta} & \\ {r = 1 - 2\cos(-\theta)\begin{array}{llll} & & & \end{array}} & {\text{Replace~}(r,\theta)\;\text{with}\;(r,-\theta).} \\ {r = 1 - 2\cos\;\theta} & \text{Even/Odd~identity} \end{array}\]
The graph of this equation exhibits symmetry with respect to the polar axis.
In the third test, we consider symmetry with respect to the pole (origin). We replace \((r,\theta)\) with \(\left( {- r,\theta} \right)\) to determine if the tested equation is equivalent to the original equation. For example, suppose we are given the equation \(r = 2\sin(3\theta\operatorname{).}\)
\[\begin{matrix} {r = 2\sin(3\theta)} \\ {- r = 2\sin(3\theta)} \end{matrix}\]
The equation has failed the symmetry test, but that does not mean that it is not symmetric with respect to the pole. Passing one or more of the symmetry tests verifies that symmetry will be exhibited in a graph. However, failing the symmetry tests does not necessarily indicate that a graph will not be symmetric about the line \(\theta = \frac{\pi}{2},\) the polar axis, or the pole. In these instances, we can confirm that symmetry exists by plotting reflecting points across the apparent axis of symmetry or the pole. Testing for symmetry is a technique that simplifies the graphing of polar equations, but its application is not perfect.
10.4.2 Graphing Polar Equations by Plotting Points
To graph in the rectangular coordinate system we construct a table of \(x\) and \(y\) values. To graph in the polar coordinate system we construct a table of \(\theta\) and \(r\) values. We enter values of \(\theta\) into a polar equation and calculate \(r.\) However, using the properties of symmetry and finding key values of \(\theta\) and \(r\) means fewer calculations will be needed.
Finding Zeros and Maxima
To find the zeros of a polar equation, we solve for the values of \(\theta\) that result in \(r = 0.\) Recall that, to find the zeros of polynomial functions, we set the equation equal to zero and then solve for \(x.\) We use the same process for polar equations. Set \(r = 0,\) and solve for \(\theta.\)
For many of the forms we will encounter, the maximum value of a polar equation is found by substituting those values of \(\theta\) into the equation that result in the maximum value of the trigonometric functions. Consider \(r = 5\cos\;\theta;\) the maximum distance between the curve and the pole is 5 units. The maximum value of the cosine function is 1 when \(\theta = 0,\) so our polar equation is \(5\cos\;\theta,\) and the value \(\theta = 0\) will yield the maximum \(|r|.\)
Similarly, the maximum value of the sine function is 1 when \(\theta = \frac{\pi}{2},\) and if our polar equation is \(r = 5\sin\;\theta,\) the value \(\theta = \frac{\pi}{2}\) will yield the maximum \(|r|.\) We may find additional information by calculating values of \(r\) when \(\theta = 0.\) These points would be polar axis intercepts, which may be helpful in drawing the graph and identifying the curve of a polar equation.
Investigating Circles
Now we have seen the equation of a circle in the polar coordinate system. In the last two examples, the same equation was used to illustrate the properties of symmetry and demonstrate how to find the zeros, maximum values, and plotted points that produced the graphs. However, the circle is only one of many shapes in the set of polar curves.
There are five classic polar curves: cardioids, limaҫons, lemniscates, rose curves, and Archimedes’ spirals. We will briefly touch on the polar formulas for the circle before moving on to the classic curves and their variations.
Investigating Cardioids
While translating from polar coordinates to Cartesian coordinates may seem simpler in some instances, graphing the classic curves is actually less complicated in the polar system. The next curve is called a cardioid, as it resembles a heart. This shape is often included with the family of curves called limaçons, but here we will discuss the cardioid on its own.
Investigating Limaçons
The word limaçon is Old French for “snail,” a name that describes the shape of the graph. As mentioned earlier, the cardioid is a member of the limaçon family, and we can see the similarities in the graphs. The other images in this category include the one-loop limaçon and the two-loop (or inner-loop) limaçon. One-loop limaçons are sometimes referred to as dimpled limaçons when \(1 < \frac{a}{b} < 2\) and convex limaçons when \(\frac{a}{b} \geq 2.\)
Another type of limaçon, the inner-loop limaçon, is named for the loop formed inside the general limaçon shape. It was discovered by the German artist Albrecht Dürer(1471-1528), who revealed a method for drawing the inner-loop limaçon in his 1525 book Underweysung der Messing. A century later, the father of mathematician Blaise Pascal, Étienne Pascal(1588-1651), rediscovered it.
Investigating Lemniscates
The lemniscate is a polar curve resembling the infinity symbol \(\infty\) or a figure 8. Centered at the pole, a lemniscate is symmetrical by definition.
Investigating Rose Curves
The next type of polar equation produces a petal-like shape called a rose curve. Although the graphs look complex, a simple polar equation generates the pattern.
Investigating the Archimedes’ Spiral
The final polar equation we will discuss is the Archimedes’ spiral, named for its discoverer, the Greek mathematician Archimedes (c. 287 BCE-c. 212 BCE), who is credited with numerous discoveries in the fields of geometry and mechanics.
10.4.3 Summary of Curves
We have explored a number of seemingly complex polar curves in this section. Figure 20 and Figure 21 summarize the graphs and equations for each of these curves.

Figure 20

Figure 21
Section Exercises
Verbal
1. Describe the three types of symmetry in polar graphs, and compare them to the symmetry of the Cartesian plane.
Solution (click to reveal)
Symmetry with respect to the polar axis is similar to symmetry about the \(x\)-axis, symmetry with respect to the pole is similar to symmetry about the origin, and symmetric with respect to the line \(\theta = \frac{\pi}{2}\) is similar to symmetry about the \(y\)-axis.
2. Which of the three types of symmetries for polar graphs correspond to the symmetries with respect to the \(x\)-axis, \(y\)-axis, and origin?
3. What are the steps to follow when graphing polar equations?
Solution (click to reveal)
Test for symmetry; find zeros, intercepts, and maxima; make a table of values. Decide the general type of graph, cardioid, limaçon, lemniscate, etc., then plot points at \(\theta = 0,\;\frac{\pi}{2},\) \(\pi\) and \(\frac{3\pi}{2},\) and sketch the graph.
4. Describe the shapes of the graphs of cardioids, limaçons, and lemniscates.
5. What part of the equation determines the shape of the graph of a polar equation?
Solution (click to reveal)
The shape of the polar graph is determined by whether or not it includes a sine, a cosine, and constants in the equation.
Graphical
For the following exercises, test the equation for symmetry.
6. \(r = 5\cos\; 3\theta\)
7. \(r = 3 - 3\cos\;\theta\)
Solution (click to reveal)
symmetric with respect to the polar axis
8. \(r = 3 + 2\sin\;\theta\)
9. \(r = 3\sin\; 2\theta\)
Solution (click to reveal)
symmetric with respect to the polar axis, symmetric with respect to the line \(\theta = \frac{\pi}{2},\) symmetric with respect to the pole
10. \(r = 4\)
11. \(r = 2\theta\)
Solution (click to reveal)
symmetric with respect to the line \(\theta = \frac{\pi}{2}\)
12. \(r = 4\cos\;\frac{\theta}{2}\)
13. \(r = \frac{2}{\theta}\)
Solution (click to reveal)
Symmetric with respect to line \(\theta = \frac{\pi}{2}\) (y-axis)
14. \(r = 3\sqrt{1 - \cos^{2}\theta}\)
15. \(r = \sqrt{5\sin\; 2\theta}\)
Solution (click to reveal)
symmetric with respect to the pole
For the following exercises, graph the polar equation. Identify the name of the shape.
16. \(r = 3\cos\;\theta\)
17. \(r = 4\sin\;\theta\)
Solution (click to reveal)
circle

18. \(r = 2 + 2\cos\;\theta\)
19. \(r = 2 - 2\cos\;\theta\)
Solution (click to reveal)
cardioid

20. \(r = 5 - 5\sin\;\theta\)
21. \(r = 3 + 3\sin\;\theta\)
Solution (click to reveal)
cardioid

22. \(r = 3 + 2\sin\;\theta\)
23. \(r = 7 + 4\sin\;\theta\)
Solution (click to reveal)
one-loop/dimpled limaçon

24. \(r = 4 + 3\cos\;\theta\)
25. \(r = 5 + 4\cos\;\theta\)
Solution (click to reveal)
one-loop/dimpled limaçon

26. \(r = 10 + 9\cos\;\theta\)
27. \(r = 1 + 3\sin\;\theta\)
Solution (click to reveal)
inner loop/two-loop limaçon

28. \(r = 2 + 5\sin\;\theta\)
29. \(r = 5 + 7\sin\;\theta\)
Solution (click to reveal)
inner loop/two-loop limaçon

30. \(r = 2 + 4\cos\;\theta\)
31. \(r = 5 + 6\cos\;\theta\)
Solution (click to reveal)
inner loop/two-loop limaçon

32. \(r^{2} = 36\cos\left( {2\theta} \right)\)
33. \(r^{2} = 10\cos\left( {2\theta} \right)\)
Solution (click to reveal)
lemniscate

34. \(r^{2} = 4\sin\left( {2\theta} \right)\)
35. \(r^{2} = 10\sin\left( {2\theta} \right)\)
Solution (click to reveal)
lemniscate

36. \(r = 3\text{sin}(2\theta)\)
37. \(r = 3\text{cos}(2\theta)\)
Solution (click to reveal)
rose curve

38. \(r = 5\text{sin}(3\theta)\)
39. \(r = 4\text{sin}(4\theta)\)
Solution (click to reveal)
rose curve

40. \(r = 4\text{sin}(5\theta)\)
41. \(r = -\theta\)
Solution (click to reveal)
Archimedes’ spiral

42. \(r = 2\theta\)
43. \(r = - 3\theta\)
Solution (click to reveal)
Archimedes’ spiral

Technology
For the following exercises, use a graphing calculator to sketch the graph of the polar equation.
44. \(r = \frac{1}{\theta}\)
45. \(r = \frac{1}{\sqrt{\theta}}\)
Solution (click to reveal)

46. \(r = 2\sin\;\theta\tan\;\theta,\) a cissoid
47. \(r = 2\sqrt{1 - \sin^{2}\theta}\), a hippopede
Solution (click to reveal)

48. \(r = 5 + \cos\left( {4\theta} \right)\)
49. \(r = 2 - \sin\left( {2\theta} \right)\)
Solution (click to reveal)

50. \(r = \theta^{2}\)
51. \(r = \theta + 1\)
Solution (click to reveal)

52. \(r = \theta\sin\;\theta\)
53. \(r = \theta\cos\;\theta\)
Solution (click to reveal)

For the following exercises, use a graphing utility to graph each pair of polar equations on a domain of \(\left\lbrack {0,4\pi} \right\rbrack\) and then explain the differences shown in the graphs.
54. \(r = \theta,r = - \theta\)
55. \(r = \theta,r = \theta + \sin\;\theta\)
Solution (click to reveal)
They are both spirals, but not quite the same.
56. \(r = \sin\;\theta + \theta,r = \sin\;\theta - \theta\)
57. \(r = 2\sin\left( \frac{\theta}{2} \right),r = \theta\sin\left( \frac{\theta}{2} \right)\)
Solution (click to reveal)
Both graphs are curves with 2 loops. The equation with a coefficient of \(\theta\) has two loops on the left, the equation with a coefficient of 2 has two loops side by side. Graph these from 0 to \(4\pi\) to get a better picture.
58. \(r = \sin\left( {\cos(3\theta)} \right)\; r = \sin(3\theta)\)
59. On a graphing utility, graph \(r = \sin\left( {\frac{16}{5}\theta} \right)\) on \(\left\lbrack 0 \right.\), \(\left. 4\pi \right\rbrack\), \(\left\lbrack 0 \right.\), \(\left. 8\pi \right\rbrack\), \(\left\lbrack 0 \right.\), \(\left. 12\pi \right\rbrack\), and \(\left\lbrack 0 \right.\), \(\left. 16\pi \right\rbrack.\) Describe the effect of increasing the width of the domain.
Solution (click to reveal)
When the width of the domain is increased, more petals of the flower are visible.
60. On a graphing utility, graph and sketch \(r = \sin\;\theta + \left( {\sin\left( {\frac{5}{2}\theta} \right)} \right)^{3}\) on \(\left\lbrack {0,4\pi} \right\rbrack.\)
61. On a graphing utility, graph each polar equation. Explain the similarities and differences you observe in the graphs.
\[\begin{array}{l} {r_{1} = 3\sin(3\theta)} \\ {r_{2} = 2\sin(3\theta)} \\ {r_{3} = \sin(3\theta)} \end{array}\]
Solution (click to reveal)
The graphs are three-petal, rose curves. The larger the coefficient, the greater the curve’s distance from the pole.
62. On a graphing utility, graph each polar equation. Explain the similarities and differences you observe in the graphs.
\[\begin{array}{l} {r_{1} = 3 + 3\cos\;\theta} \\ {r_{2} = 2 + 2\cos\;\theta} \\ {r_{3} = 1 + \cos\;\theta} \end{array}\]
63. On a graphing utility, graph each polar equation. Explain the similarities and differences you observe in the graphs.
\[\begin{array}{l} {r_{1} = 3\theta} \\ {r_{2} = 2\theta} \\ {r_{3} = \theta} \end{array}\]
Solution (click to reveal)
The graphs are spirals. The smaller the coefficient, the tighter the spiral.
Extensions
For the following exercises, draw each polar equation on the same set of polar axes, and find the points of intersection.
64. \(r_{1} = 3 + 2\sin\;\theta,\; r_{2} = 2\)
65. \(r_{1} = 6 - 4\cos\;\theta,\; r_{2} = 4\)
Solution (click to reveal)
\(\left( {4,\frac{\pi}{3}} \right),\left( {4,\frac{5\pi}{3}} \right)\)
66. \(r_{1} = 1 + \sin\;\theta,\; r_{2} = 3\sin\;\theta\)
67. \(r_{1} = 1 + \cos\;\theta,\; r_{2} = 3\cos\;\theta\)
Solution (click to reveal)
\(\left( {\frac{3}{2},\frac{\pi}{3}} \right),\left( {\frac{3}{2},\frac{5\pi}{3}} \right)\)
68. \(r_{1} = \cos\left( {2\theta} \right),\; r_{2} = \sin\left( {2\theta} \right)\)
69. \(r_{1} = \sin^{2}\left( {2\theta} \right)\), \(r_{2} = 1 - \cos\left( {4\theta} \right)\)
Solution (click to reveal)
\(\left( {0,\frac{\pi}{2}} \right),\;\left( {0,\pi} \right),\;\left( {0,\frac{3\pi}{2}} \right),\;\left( {0,2\pi} \right)\)
70. \(r_{1} = \sqrt{3},\; r_{2} = 2\sin(\theta)\)
71. \(r_{1}{}^{2} = \sin\;\theta,r_{2}{}^{2} = \cos\;\theta\)
Solution (click to reveal)
\(= \frac{\pi}{4}\) and \(\sqrt{\text{sin}\frac{\pi}{4}} = \sqrt{\frac{\sqrt{2}}{2}} = \frac{\sqrt[4]{8}}{2}\)
72. \(r_{1} = 1 + \cos\;\theta\), \(r_{2} = 1 - \sin\;\theta\)