10.4: Polar Coordinates - Graphs
- Test polar equations for symmetry.
- Graph polar equations by plotting points.
Keplar's First Law of Planetary Motion argues that the planets move through space in elliptical, periodic orbits about the sun, as shown in Figure \(\PageIndex{1}\). 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 sun and \(\theta\) as the planet’s angular bearing, or its direction from a fixed point on the sun. In this section, we will focus on the polar system and the graphs that are generated directly from polar coordinates.
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 \(r\)) to determine the graph of a polar equation.
In the first test, we consider symmetry with respect to the line \(\theta=\dfrac{\pi}{2}\) (\(y\)-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 \(r=2 \sin \theta\);
\[\begin{align*} r&= 2 \sin \theta \\ -r&= 2 \sin -\theta \qquad \text{Replace } (r,\theta) \text{ with }(-r,-\theta). \\ -r&= -2 \sin \theta \qquad \text{Identity: }\sin(-\theta)=-\sin \theta. \\ r&= 2 \sin \theta \qquad \text{Multiply both sides by }-1 \end{align*}\]
This equation exhibits symmetry with respect to the line \(\theta=\dfrac{\pi}{2}\).
In the second test, we consider symmetry with respect to the polar axis (\(x\)-axis). We replace \((r,\theta)\) with \((r,−\theta)\) or \((−r,\pi−\theta)\) to determine equivalency between the tested equation and the original. For example, suppose we are given the equation \(r=1−2 \cos \theta\).
\[\begin{align*} r&= 1-2 \cos \theta \\ r&= 1-2 \cos(-\theta)\qquad \text{Replace }(r,\theta) \text{ with }(r,-\theta). \\ r&= 1-2 \cos \theta \qquad \text{Even/Odd identity} \end{align*}\]
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 \((−r,\theta)\) to determine if the tested equation is equivalent to the original equation. For example, suppose we are given the equation \(r=2 \sin(3\theta)\).
\(r=2 \sin(3\theta)\)
\(−r=2 \sin(3\theta)\)
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 \(\theta=\dfrac{\pi}{2}\), 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.
A polar equation describes a curve on the polar grid. The graph of a polar equation can be evaluated for three types of symmetry, as shown in Figure \(\PageIndex{2}\).
- Substitute the appropriate combination of components for \((r,\theta)\): \((−r,−\theta)\) for \(\theta=\dfrac{\pi}{2}\) symmetry; \((r,−\theta)\) for polar axis symmetry; and \((−r,\theta)\) for symmetry with respect to the pole.
- If the resulting equations are equivalent in one or more of the tests, the graph produces the expected symmetry.
Test the equation \(r=2 \sin \theta\) for symmetry.
Solution
Test for each of the three types of symmetry.
| 1) Replacing \((r,\theta)\) with \((−r,−\theta)\) yields the same result. Thus, the graph is symmetric with respect to the line \(\theta=\dfrac{\pi}{2}\). |
\(−r=2 \sin(−\theta)\) \(−r=−2 \sin \theta\) Even-odd identity \(r=2 \sin \theta\) Multiply by \(−1\) Passed |
| 2) Replacing \(\theta\) with \(−\theta\) does not yield the same equation. Therefore, the graph fails the test and may or may not be symmetric with respect to the polar axis. |
\(r=2 \sin(−\theta)\) \(r=−2 \sin \theta\) Even-odd identity \(r=−2 \sin \theta ≠ 2 \sin \theta\) Failed |
| 3) Replacing \(r\) with \(–r\) changes the equation and fails the test. The graph may or may not be symmetric with respect to the pole. |
\(−r=2 \sin \theta\) \(r=−2 \sin \theta ≠2 \sin \theta\) Failed |
Analysis
Using a graphing calculator, we can see that the equation \(r=2 \sin \theta\) is a circle centered at \((0,1)\) with radius \(r=1\) and is indeed symmetric to the line \(\theta=\dfrac{\pi}{2}\). We can also see that the graph is not symmetric with the polar axis or the pole. See Figure \(\PageIndex{3}\).
Test the equation for symmetry: \(r=−2 \cos \theta\).
- Answer
-
The equation fails the symmetry test with respect to the line \(\theta=\dfrac{\pi}{2}\) and with respect to the pole. It passes the polar axis symmetry test.
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 \(\theta=\dfrac{\pi}{2}\), and if our polar equation is \(r=5 \sin \theta\), the value \(\theta=\dfrac{\pi}{2}\) 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.
Using the equation in Example \(\PageIndex{1}\), find the zeros and maximum \(| r |\) and, if necessary, the polar axis intercepts of \(r=2 \sin \theta\).
Solution
To find the zeros, set \(r\) equal to zero and solve for \(\theta\).
\[\begin{align*} 2 \sin \theta &= 0 \\ \sin \theta &= 0 \\ \theta &= {\sin}^{-1} 0 \\ \theta &= n\pi \qquad \text{where n is an integer} \end{align*}\]
Substitute any one of the \(\theta\) values into the equation. We will use \(0\).
\[\begin{align*} r&= 2 \sin(0) \\ r&= 0 \end{align*}\]
The points \((0,0)\) and \((0,\pm n\pi)\) are the zeros of the equation. They all coincide, so only one point is visible on the graph. This point is also the only polar axis intercept.
To find the maximum value of the equation, look at the maximum value of the trigonometric function \(\sin \theta\), which occurs when \(\theta=\dfrac{\pi}{2}\pm 2k\pi\) resulting in \(\sin\left(\dfrac{\pi}{2}\right)=1\). Substitute \(\dfrac{\pi}{2}\) for \(\theta\).
\[\begin{align*} r&= 2 \sin\left(\dfrac{\pi}{2}\right) \\ r&= 2(1) \\ r&= 2 \end{align*}\]
Analysis
The point \(\left(2,\dfrac{\pi}{2}\right)\) will be the maximum value on the graph. Let’s plot a few more points to verify the graph of a circle. See Table \(\PageIndex{1}\) and Figure \(\PageIndex{4}\).
| \(\theta\) | \(r=2 \sin \theta\) | \(r\) |
|---|---|---|
| \(0\) | \(r=2 \sin(0)=0\) | \(0\) |
| \(\dfrac{\pi}{6}\) | \(r=2 \sin\left(\dfrac{\pi}{6}\right)=1\) | \(1\) |
| \(\dfrac{\pi}{3}\) | \(r=2 \sin\left(\dfrac{\pi}{3}\right)≈1.73\) | \(1.73\) |
| \(\dfrac{pi}{2}\) | \(r=2 \sin\left(\dfrac{\pi}{2}\right)=2\) | \(2\) |
| \(\dfrac{2\pi}{3}\) | \(r=2 \sin\left(\dfrac{2\pi}{3}\right)≈1.73\) | \(1.73\) |
| \(\dfrac{5\pi}{6}\) | \(r=2 \sin\left(\dfrac{5\pi}{6}\right)=1\) | \(1\) |
| \(\pi\) | \(r=2 \sin(\pi)=0\) | \(0\) |
Without converting to Cartesian coordinates, test the given equation for symmetry and find the zeros and maximum values of \(| r |\): \(r=3 \cos \theta\).
- Answer
-
Tests will reveal symmetry about the polar axis. The zero is \(\left(0,\dfrac{\pi}{2}\right)\), and the maximum value is \((3,0)\).
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.
Some of the formulas that produce the graph of a circle in polar coordinates are given by \(r=a \cos \theta\) and \(r=a \sin \theta\), wherea a is the diameter of the circle or the distance from the pole to the farthest point on the circumference. The radius is \(\dfrac{|a|}{2}\), or one-half the diameter. For \(r=a \cos \theta\), the center is \(\left(\dfrac{a}{2},0\right)\). For \(r=a \sin \theta\), the center is \(\left(\dfrac{a}{2},\pi\right)\). Figure \(\PageIndex{5}\) shows the graphs of these four circles.
Sketch the graph of \(r=4 \cos \theta\).
Solution
First, testing the equation for symmetry, we find that the graph is symmetric about the polar axis. Next, we find the zeros and maximum \(| r |\) for \(r=4 \cos \theta\). First, set \(r=0\), and solve for \(\theta\). Thus, a zero occurs at \(\theta=\dfrac{\pi}{2}\pm k\pi\). A key point to plot is \(\left(0,\dfrac{\pi}{2}\right)\).
To find the maximum value of \(r\), note that the maximum value of the cosine function is \(1\) when \(\theta=0\pm 2k\pi\). Substitute \(\theta=0\) into the equation:
\[\begin{align*} r&= 4 \cos \theta\\ r&= 4 \cos(0)\\ r&= 4(1)\\ &= 4 \end{align*}\]
The maximum value of the equation is \(4\). A key point to plot is \((4, 0)\).
As \(r=4 \cos \theta\) is symmetric with respect to the polar axis, we only need to calculate \(r\)-values for \(θ\) over the interval \([0, \pi]\). Points in the upper quadrant can then be reflected to the lower quadrant. Make a table of values similar to Table \(\PageIndex{2}\). The graph is shown in Figure \(\PageIndex{6}\).
| \(\theta\) | \(0\) | \(\dfrac{\pi}{6}\) | \(\dfrac{\pi}{4}\) | \(\dfrac{\pi}{3}\) | \(\dfrac{\pi}{2}\) | \(\dfrac{2\pi}{3}\) | \(\dfrac{3\pi}{4}\) | \(\dfrac{5\pi}{6}\) | \(\pi\) |
|---|---|---|---|---|---|---|---|---|---|
| \(r\) | \(4\) | \(3.46\) | \(2.83\) | \(2\) | \(0\) | \(−2\) | \(−2.83\) | \(−3.46\) | \(4\) |
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.
The formulas that produce the graphs of a cardioid are given by \(r=a\pm b \cos \theta\) and \(r=a\pm b \sin \theta\) where \(a>0\), \(b>0\), and \(\dfrac{a}{b}=1\). The cardioid graph passes through the pole, as we can see in Figure \(\PageIndex{7}\).
- Check equation for the three types of symmetry.
- Find the zeros. Set \(r=0\).
- Find the maximum value of the equation according to the maximum value of the trigonometric expression.
- Make a table of values for \(r\) and \(\theta\).
- Plot the points and sketch the graph.
Sketch the graph of \(r=2+2 \cos \theta\).
Solution
First, testing the equation for symmetry, we find that the graph of this equation will be symmetric about the polar axis. Next, we find the zeros and maximums. Setting \(r=0\), we have \(\theta=\pi+2k\pi\). The zero of the equation is located at \((0,\pi)\). The graph passes through this point.
The maximum value of \(r=2+2 \cos \theta\) occurs when \(\cos \theta\) is a maximum, which is when \(\cos \theta=1\) or when \(\theta=0\). Substitute \(\theta=0\) into the equation, and solve for \(r\).
\[\begin{align*} r&= 2+2 \cos(0)\\ r&= 2+2(1)\\ &= 4 \end{align*}\]
The point \((4,0)\) is the maximum value on the graph.
We found that the polar equation is symmetric with respect to the polar axis, but as it extends to all four quadrants, we need to plot values over the interval \([0, \pi]\). The upper portion of the graph is then reflected over the polar axis. Next, we make a table of values, as in Table \(\PageIndex{3}\), and then we plot the points and draw the graph. See Figure \(\PageIndex{8}\).
| θ | 0 | \(\dfrac{π}{4}\) | \(\dfrac{π}{2}\) | \(\dfrac{2π}{3}\) | \(π\) |
|---|---|---|---|---|---|
| r | 4 | 3.41 | 2 | 1 | 0 |
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 \(1<\dfrac{a}{b}<2\) and convex limaçons when \(\dfrac{a}{b}≥2\).
The formulas that produce the graph of a dimpled one-loop limaçon are given by \(r=a\pm b \cos \theta\) and \(r=a\pm b \sin \theta\) where \(a>0\), \(b>0\), and \(1<ab<2\). All four graphs are shown in Figure \(\PageIndex{9}\).
- Test the equation for symmetry. Remember that failing a symmetry test does not mean that the shape will not exhibit symmetry. Often the symmetry may reveal itself when the points are plotted.
- Find the zeros.
- Find the maximum values according to the trigonometric expression.
- Make a table.
- Plot the points and sketch the graph.
Graph the equation \(r=4−3 \sin \theta\).
Solution
First, testing the equation for symmetry, we find that it fails all three symmetry tests, meaning that the graph may or may not exhibit symmetry, so we cannot use the symmetry to help us graph it. However, this equation has a graph that clearly displays symmetry with respect to the line \(\theta=\dfrac{\pi}{2}\), yet it fails all the three symmetry tests. A graphing calculator will immediately illustrate the graph’s reflective quality.
Next, we find the zeros and maximum, and plot the reflecting points to verify any symmetry. Setting \(r=0\) results in \(\theta\) being undefined. What does this mean? How could \(\theta\) be undefined? The angle \(\theta\) is undefined for any value of \(\sin \theta>1\). Therefore, \(\theta\) is undefined because there is no value of \(\theta\) for which \(\sin \theta>1\). Consequently, the graph does not pass through the pole. Perhaps the graph does cross the polar axis, but not at the pole. We can investigate other intercepts by calculating \(r\) when \(\theta=0\).
\[\begin{align*} r(0)&= 4-3 \sin(0)\\ r&= 4-3\cdot 0\\ &= 4 \end{align*}\]
So, there is at least one polar axis intercept at \((4,0)\).
Next, as the maximum value of the sine function is \(1\) when \(\theta=\dfrac{\pi}{2}\), we will substitute \(\theta=\dfrac{\pi}{2}\) into the equation and solve for \(r\). Thus, \(r=1\).
Make a table of the coordinates similar to Table \(\PageIndex{4}\).
| \(\theta\) | \(0\) | \(\dfrac{\pi}{6}\) | \(\dfrac{\pi}{3}\) | \(\dfrac{\pi}{2}\) | \(\dfrac{2\pi}{3}\) | \(\dfrac{5\pi}{6}\) | \(\pi\) | \(\dfrac{7\pi}{6}\) | \(\dfrac{4\pi}{3}\) | \(\dfrac{3\pi}{2}\) | \(\dfrac{5\pi}{3}\) | \(\dfrac{11\pi}{6}\) | \(2\pi\) |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| \(r\) | \(4\) | \(2.5\) | \(1.4\) | \(1\) | \(1.4\) | \(2.5\) | \(4\) | \(5.5\) | \(6.6\) | \(7\) | \(6.6\) | \(5.5\) | \(4\) |
The graph is shown in Figure \(\PageIndex{10}\).
Analysis
This is an example of a curve for which making a table of values is critical to producing an accurate graph. The symmetry tests fail; the zero is undefined. While it may be apparent that an equation involving \(\sin \theta\) is likely symmetric with respect to the line \(\theta=\dfrac{\pi}{2}\), evaluating more points helps to verify that the graph is correct.
Sketch the graph of \(r=3−2 \cos \theta\).
- Answer
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.
The formulas that generate the inner-loop limaçons are given by \(r=a\pm b\cos \theta\) and \(r=a\pm b \sin \theta\) where \(a>0\), \(b>0\), and \(a<b\). The graph of the inner-loop limaçon passes through the pole twice: once for the outer loop, and once for the inner loop. See Figure 10.5.12 for the graphs.
Sketch the graph of \(r=2+5 \cos \theta\).
Solution
Testing for symmetry, we find that the graph of the equation is symmetric about the polar axis. Next, finding the zeros reveals that when \(r=0\), \(\theta=1.98\). The maximum \(| r |\) is found when \(\cos \theta=1\) or when \(\theta=0\). Thus, the maximum is found at the point \((7, 0)\).
Even though we have found symmetry, the zero, and the maximum, plotting more points will help to define the shape, and then a pattern will emerge. See Table \(\PageIndex{5}\).
| \(\theta\) | \(0\) | \(\dfrac{\pi}{6}\) | \(\dfrac{\pi}{3}\) | \(\dfrac{\pi}{2}\) | \(\dfrac{2\pi}{3}\) | \(\dfrac{5\pi}{6}\) | \(\pi\) | \(\dfrac{7\pi}{6}\) | \(\dfrac{4\pi}{3}\) | \(\dfrac{3\pi}{2}\) | \(\dfrac{5\pi}{3}\) | \(\dfrac{11\pi}{6}\) | \(2\pi\) |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| \(r\) | \(7\) | \(6.3\) | \(4.5\) | \(2\) | \(−0.5\) | \(−2.3\) | \(−3\) | \(−2.3\) | \(−0.5\) | \(2\) | \(4.5\) | \(6.3\) | \(7\) |
As expected, the values begin to repeat after \(\theta=\pi\). The graph is shown in Figure \(\PageIndex{13}\).
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.
The formulas that generate the graph of a lemniscate are given by \(r^2=a^2 \cos 2\theta\) and \(r^2=a^2 \sin 2\theta\) where \(a≠0\). The formula \(r^2=a^2 \sin 2\theta\) is symmetric with respect to the pole. The formula \(r^2=a^2 \cos 2\theta\) is symmetric with respect to the pole, the line \(\theta=\dfrac{\pi}{2}\), and the polar axis. See Figure \(\PageIndex{14}\) for the graphs.
Sketch the graph of \(r^2=4 \cos 2\theta\).
Solution
The equation exhibits symmetry with respect to the line \(\theta=\dfrac{\pi}{2}\), the polar axis, and the pole.
Let’s find the zeros. It should be routine by now, but we will approach this equation a little differently by making the substitution \(u=2\theta\).
\[\begin{align*} 0 &= 4 \cos 2\theta \\ 0 &= 4 \cos u \\ 0 &= \cos u \\ {\cos}^{-1} 0 &= \dfrac{\pi}{2} \\ u &= \dfrac{\pi}{2} \qquad \text{Substitute } 2\theta \text{ back in for } u. \\ 2\theta &= \dfrac{\pi}{2} \\ \theta &= \dfrac{\pi}{4} \end{align*}\]
So, the point \(\left(0,\dfrac{\pi}{4}\right)\)is a zero of the equation.
Now let’s find the maximum value. Since the maximum of \(\cos u=1\) when \(u=0\), the maximum \(\cos 2\theta=1\) when \(2\theta=0\). Thus,
\[\begin{align*} r^2 &= 4 \cos(0) \\ r^2 &= 4(1)\\ r^2&= 4 \\ r&= \pm 4\\ &=2 \end{align*}\]
We have a maximum at \((2, 0)\). Since this graph is symmetric with respect to the pole, the line \(\theta=\dfrac{\pi}{2}\), and the polar axis, we only need to plot points in the first quadrant.
Make a table similar to Table \(\PageIndex{6}\).
| \(\theta\) | \(0\) | \(\dfrac{\pi}{6}\) | \(\dfrac{\pi}{4}\) | \(\dfrac{\pi}{3}\) | \(\dfrac{\pi}{2}\) |
|---|---|---|---|---|---|
| \(r\) | \(2\) | \(\sqrt{2}\) | \(0\) | \(\sqrt{2}\) | \(0\) |
Plot the points on the graph, such as the one shown in Figure \(\PageIndex{15}\).
Analysis
Making a substitution such as \(u=2\theta\) is a common practice in mathematics because it can make calculations simpler. However, we must not forget to replace the substitution term with the original term at the end, and then solve for the unknown.
Some of the points on this graph may not show up using the Trace function on the TI-84 graphing calculator, and the calculator table may show an error for these same points of \(r\). This is because there are no real square roots for these values of \(θ\). In other words, the corresponding \(r\)-values of \(\sqrt{4 \cos(2\theta)}\) are complex numbers because there is a negative number under the radical.
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.
The formulas that generate the graph of a rose curve are given by \(r=a \cos n\theta\) and \(r=a \sin n\theta\) where \(a≠0\). If \(n\) is even, the curve has \(2n\) petals. If \(n\) is odd, the curve has \(n\) petals. See Figure \(\PageIndex{16}\).
Sketch the graph of \(r=2 \cos 4\theta\).
Solution
Testing for symmetry, we find again that the symmetry tests do not tell the whole story. The graph is not only symmetric with respect to the polar axis, but also with respect to the line \(\theta=\dfrac{\pi}{2}\) and the pole.
Now we will find the zeros. First make the substitution \(u=4\theta\).
\[\begin{align*} 0 &= 2 \cos 4\theta \\ 0 &= \cos 4\theta \\ 0 &= \cos u \\ {\cos}^{-1} 0 &=u \\ u &= \dfrac{\pi}{2} \\ 4\theta &= \dfrac{\pi}{2} \\ \theta &=\dfrac{\pi}{8} \end{align*}\]
The zero is \(\theta=\dfrac{\pi}{8}\). The point \(\left(0,\dfrac{\pi}{8}\right)\) is on the curve.
Next, we find the maximum \(| r |\). We know that the maximum value of \(\cos u=1\) when \(\theta=0\). Thus,
\[\begin{align*} r &=2 \cos(4\cdot 0) \\ r &=2 \cos(0) \\ r &=2(1)\\ &= 2 \end{align*}\]
The point \((2,0)\) is on the curve.
The graph of the rose curve has unique properties, which are revealed in Table \(\PageIndex{7}\).
| \(\theta\) | \(0\) | \(\dfrac{\pi}{8}\) | \(\dfrac{\pi}{4}\) | \(\dfrac{3\pi}{8}\) | \(\dfrac{\pi}{2}\) | \(5π8\) | \(3π4\) |
|---|---|---|---|---|---|---|---|
| \(r\) | \(2\) | \(0\) | \(−2\) | \(0\) | \(2\) | \(0\) | \(−2\) |
As \(r=0\) when \(\theta=\dfrac{\pi}{8}\), it makes sense to divide values in the table by \(\dfrac{\pi}{8}\) units. A definite pattern emerges. Look at the range of \(r\)-values: \(2, 0, −2, 0\) and so on. This represents the development of the curve one petal at a time. Starting at \(r=0\), each petal extends out a distance of \(r=2\), and then turns back to zero \(2n\) times for a total of eight petals. See the graph in Figure \(\PageIndex{17}\).
Analysis
When these curves are drawn, it is best to plot the points in order, as in the Table \(\PageIndex{7}\). This allows us to see how the graph hits a maximum (the tip of a petal), loops back crossing the pole, hits the opposite maximum, and loops back to the pole. The action is continuous until all the petals are drawn.
Sketch the graph of \(r=4 \sin(2\theta)\).
- Answer
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The graph is a rose curve, \(n\) even
Sketch the graph of \(r=2 \sin(5\theta)\).
Solution
The graph of the equation shows symmetry with respect to the line \(\theta=\dfrac{\pi}{2}\). Next, find the zeros and maximum. We will want to make the substitution \(u=5\theta\).
\[\begin{align*} 0 &=2 \sin(5\theta) \\ 0 &=\sin u \\ {\sin}^{-1} 0 &=0 \\ u &=0 \\ 5\theta &=0 \\ \theta &=0 \end{align*}\]
The maximum value is calculated at the angle where \(\sin \theta\) is a maximum. Therefore,
\[\begin{align*} r&= 2 \sin\left(5\cdot \dfrac{\pi}{2}\right) \\ r&= 2(1)\\ &= 2 \end{align*}\]
Thus, the maximum value of the polar equation is \(2\). This is the length of each petal. As the curve for \(n\) odd yields the same number of petals as \(n\), there will be five petals on the graph. See Figure \(\PageIndex{19}\).
Create a table of values similar to Table \(\PageIndex{8}\).
| \(\theta\) | \(0\) | \(\dfrac{\pi}{6}\) | \(\dfrac{\pi}{3}\) | \(\dfrac{\pi}{2}\) | \(\dfrac{2\pi}{3}\) | \(\dfrac{5\pi}{6}\) | \(\pi\) |
|---|---|---|---|---|---|---|---|
| \(r\) | \(0\0 | \(1\) | \(−1.73\) | \(2\) | \(−1.73\) | \(1\) | \(0\) |
Sketch the graph of \(r=3 \cos(3\theta)\).
- Answer
-
Rose curve, \(n\) odd
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.
The formula that generates the graph of the Archimedes’ spiral is given by \(r=\theta\) for \(\theta≥0\). As \(\theta\) increases, \(r\) increases at a constant rate in an ever-widening, never-ending, spiraling path. See Figure \(\PageIndex{21}\).
- Make a table of values for \(r\) and \(\theta\) over the given domain.
- Plot the points and sketch the graph.
Sketch the graph of \(r=\theta\) over \([0,2\pi]\).
Solution
As \(r\) is equal to \(\theta\), the plot of the Archimedes’ spiral begins at the pole at the point \((0, 0)\). While the graph hints of symmetry, there is no formal symmetry with regard to passing the symmetry tests. Further, there is no maximum value, unless the domain is restricted.
Create a table such as Table \(\PageIndex{9}\).
| \(\theta\) | \(\dfrac{\pi}{4}\) | \(\dfrac{\pi}{2}\) | \(\pi\) | \(\dfrac{3\pi}{2}\) | \(\dfrac{7\pi}{4}\) | \(2\pi\) |
|---|---|---|---|---|---|---|
| \(r\) | \(0.785\) | \(1.57\) | \(3.14\) | \(4.71\) | \(5.50\) | \(6.28\) |
Notice that the r-values are just the decimal form of the angle measured in radians. We can see them on a graph in Figure \(\PageIndex{22}\).
Analysis
The domain of this polar curve is \([ 0,2\pi ]\). In general, however, the domain of this function is \((−\infty,\infty)\). Graphing the equation of the Archimedes’ spiral is rather simple, although the image makes it seem like it would be complex.
Sketch the graph of \(r=−\theta\) over the interval \([ 0,4\pi ]\).
- Answer
Summary of Curves
We have explored a number of seemingly complex polar curves in this section. Figure \(\PageIndex{24}\) and Figure \(\PageIndex{25}\) summarize the graphs and equations for each of these curves.
Access these online resources for additional instruction and practice with graphs of polar coordinates.
- Graphing Polar Equations Part 1
- Graphing Polar Equations Part 2
- Animation: The Graphs of Polar Equations
- Graphing Polar Equations on the TI-84
Key Concepts
- It is easier to graph polar equations if we can test the equations for symmetry with respect to the line \(\theta=\dfrac{\pi}{2}\), the polar axis, or the pole.
- There are three symmetry tests that indicate whether the graph of a polar equation will exhibit symmetry. If an equation fails a symmetry test, the graph may or may not exhibit symmetry. See Example \(\PageIndex{1}\).
- Polar equations may be graphed by making a table of values for \(\theta\) and \(r\).
- The maximum value of a polar equation is found by substituting the value \(\theta\) that leads to the maximum value of the trigonometric expression.
- The zeros of a polar equation are found by setting \(r=0\) and solving for \(\theta\). See Example \(\PageIndex{2}\).
- Some formulas that produce the graph of a circle in polar coordinates are given by \(r=a \cos \theta\) and \(r=a \sin \theta\). See Example \(\PageIndex{3}\).
- The formulas that produce the graphs of a cardioid are given by \(r=a\pm b \cos \theta\) and \(r=a\pm b \sin \theta\), for \(a>0\), \(b>0\), and \(ab=1\). See Example \(\PageIndex{4}\).
- The formulas that produce the graphs of a one-loop limaçon are given by \(r=a\pm b \cos \theta\) and \(r=a\pm b \sin \theta\) for \(1<ab<2\). See Example \(\PageIndex{5}\).
- The formulas that produce the graphs of an inner-loop limaçon are given by \(r=a\pm b \cos \theta\) and \(r=a\pm b \sin \theta\) for \(a>0\), \(b>0\), and \(a<b\). See Example \(\PageIndex{6}\).
- The formulas that produce the graphs of a lemniscates are given by \(r^2=a^2 \cos 2\theta\) and \(r^2=a^2 \sin 2\theta\), where \(a≠0\).See Example \(\PageIndex{7}\).
- The formulas that produce the graphs of rose curves are given by \(r=a \cos n\theta\) and \(r=a \sin n\theta\), where \(a≠0\); if \(n\) is even, there are \(2n\) petals, and if \(n\) is odd, there aren n petals. See Example \(\PageIndex{8}\) and Example \(\PageIndex{9}\).
- The formula that produces the graph of an Archimedes’ spiral is given by \(r=\theta\), \(\theta≥0\). See Example \(\PageIndex{10}\).