Skip to main content
\(\newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\) \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\) \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\) \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\) \( \newcommand{\Span}{\mathrm{span}}\)
Mathematics LibreTexts

11.5: Graphs of Polar Equations

In this section, we discuss how to graph equations in polar coordinates on the rectangular coordinate plane. Since any given point in the plane has infinitely many different representations in polar coordinates, our `Fundamental Graphing Principle' in this section is not as clean as it was for graphs of rectangular equations on page \pageref{fgp}. We state it below for completeness.

Note: The Fundamental Graphing Principle for Polar Equations

The graph of an equation in polar coordinates is the set of points which satisfy the equation. That is, a point \(P(r,\theta)\) is on the graph of an equation if and only if there is a representation of \(P\), say \(\left(r',\theta'\right)\), such that \(r'\) and \(\theta'\) satisfy the equation.

Our first example focuses on the some of the more structurally simple polar equations.

Example \(\PageIndex{1}\):

\label{rthetaconstant} Graph the following polar equations.

  1. \(r = 4\)
  2. \(r = -3\sqrt{2}\)
  3. \(\theta = \frac{5\pi}{4}\)
  4. \(\theta = -\frac{3\pi}{2}\)

Solution

In each of these equations, only one of the variables \(r\) and \(\theta\) is present making the other variable free.\footnote{See the discussion in Example \ref{eqnconversionex} number \ref{risneg3}.} This makes these graphs easier to visualize than others.

  1. In the equation \(r=4\), \(\theta\) is free. The graph of this equation is, therefore, all points which have a polar coordinate representation \((4,\theta)\), for any choice of \(\theta\). Graphically this translates into tracing out all of the points \(4\) units away from the origin. This is exactly the definition of circle, centered at the origin, with a radius of \(4\).

 

 

Once again we have \(\theta\) being free in the equation \(r = -3\sqrt{2}\). Plotting all of the points of the form \((-3\sqrt{2}, \theta)\) gives us a circle of radius \(3\sqrt{2}\) centered at the origin.

 

 

In the equation \(\theta = \frac{5\pi}{4}\), \(r\) is free, so we plot all of the points with polar representation \(\left(r, \frac{5\pi}{4}\right)\). What we find is that we are tracing out the line which contains the terminal side of \(\theta = \frac{5\pi}{4}\) when plotted in standard position.

 

 

In \(\theta = \frac{5\pi}{4}\), \(r\) is free & \hspace{.75in} The graph of \(\theta = \frac{5\pi}{4}\) \\

 

 

As in the previous example, the variable \(r\) is free in the equation \(\theta = -\frac{3\pi}{2}\). Plotting \(\left(r, -\frac{3\pi}{2}\right)\) for various values of \(r\) shows us that we are tracing out the \(y\)-axis.

 

 

In \(\theta = -\frac{3\pi}{2}\), \(r\) is free & \hspace{.75in} The graph of \(\theta = -\frac{3\pi}{2}\) \\

Hopefully, our experience in Example \ref{rthetaconstant} makes the following result clear.

Note: Graphs of Constant \(r\) and \(\theta\) 

Suppose \(a\) and \(\alpha\) are constants, \(a \neq 0\).

  • The graph of the polar equation \(r = a\) on the Cartesian plane is a circle centered at the origin of radius \(|a|\).
  • The graph of the polar equation \(\theta = \alpha\) on the Cartesian plane is the line containing the terminal side of \(\alpha\) when plotted in standard position.

Suppose we wish to graph \(r = 6\cos(\theta)\). A reasonable way to start is to treat \(\theta\) as the independent variable, \(r\) as the dependent variable, evaluate \(r = f(\theta)\) at some `friendly' values of \(\theta\) and plot the resulting points.\footnote{For a review of these concepts and this process, see Sections \ref{FunctionNotation} and \ref{GraphsofFunctions}.} We generate the table below.

\[ \begin{array}{|r||r|r|} \hline \theta & r = 6\cos(\theta) & (r,\theta) \\ \hline 0 & 6 & (6,0) \\ \hline \frac{\pi}{4} & 3\sqrt{2} & \left(3\sqrt{2}, \frac{\pi}{4}\right) \\ \hline \frac{\pi}{2} & 0 & \left(0,\frac{\pi}{2}\right) \\ \hline \frac{3\pi}{4} & -3\sqrt{2} & \left(-3\sqrt{2}, \frac{3\pi}{4}\right) \\ \hline \pi & -6 & (-6,\pi) \\ \hline \frac{5\pi}{4} & -3\sqrt{2} & \left(-3\sqrt{2}, \frac{5\pi}{4}\right) \\ \hline \frac{3\pi}{2} & 0 & \left(0, \frac{3\pi}{2} \right) \\ \hline \frac{7\pi}{4} & 3\sqrt{2} & \left(3\sqrt{2}, \frac{7\pi}{4}\right) \\ \hline 2\pi & 6 & (6,2\pi) \\ \hline \end{array} \]

Despite having nine ordered pairs, we get only four distinct points on the graph. For this reason, we employ a slightly different strategy. We graph one cycle of \(r = 6\cos(\theta)\) on the \(\theta r\)-plane\footnote{The graph looks exactly like \(y = 6\cos(x)\) in the \(xy\)-plane, and for good reason. At this stage, we are just graphing the relationship between \(r\) and \(\theta\) before we interpret them as polar coordinates \((r,\theta)\) on the \(xy\)-plane.} and use it to help graph the equation on the \(xy\)-plane. We see that as \(\theta\) ranges from \(0\) to \(\frac{\pi}{2}\), \(r\) ranges from \(6\) to \(0\). In the \(xy\)-plane, this means that the curve starts \(6\) units from the origin on the positive \(x\)-axis (\)\theta = 0\)) and gradually returns to the origin by the time the curve reaches the \(y\)-axis (\)\theta = \frac{\pi}{2}\)). The arrows drawn in the figure below are meant to help you visualize this process. In the \(\theta r\)-plane, the arrows are drawn from the \(\theta\)-axis to the curve \(r = 6\cos(\theta)\). In the \(xy\)-plane, each of these arrows starts at the origin and is rotated through the corresponding angle \(\theta\), in accordance with how we plot polar coordinates. It is a less-precise way to generate the graph than computing the actual function values, but it is markedly faster.

Next, we repeat the process as \(\theta\) ranges from \(\frac{\pi}{2}\) to \(\pi\). Here, the \(r\) values are all negative. This means that in the \(xy\)-plane, instead of graphing in Quadrant II, we graph in Quadrant IV, with all of the angle rotations starting from the negative \(x\)-axis.

 

As \(\theta\) ranges from \(\pi\) to \(\frac{3\pi}{2}\), the \(r\) values are still negative, which means the graph is traced out in Quadrant I instead of Quadrant III. Since the \(|r|\) for these values of \(\theta\) match the \(r\) values for \(\theta\) in \(\left[0, \frac{\pi}{2} \right]\), we have that the curve begins to retrace itself at this point. Proceeding further, we find that when \(\frac{3\pi}{2} \leq \theta \leq 2\pi\), we retrace the portion of the curve in Quadrant IV that we first traced out as \(\frac{\pi}{2} \leq \theta \leq \pi\). The reader is invited to verify that plotting any range of \(\theta\) outside the interval \(\left[ 0, \pi \right]\) results in retracting some portion of the curve.\footnote{The graph of \(r=6\cos(\theta)\) looks suspiciously like a circle, for good reason. See number \ref{ris6costheta} in Example \ref{eqnconversionex}.} We present the final graph below.

Example \(\PageIndex{1}\):\label{polargraphex}

Graph the following polar equations.

  1. \label{limacon01} \(r = 4 - 2\sin(\theta)\)
  2. \label{limacon02} \(r = 2 + 4 \cos(\theta)\)
  3. \label{rose} \(r = 5\sin(2\theta)\)
  4. \label{lemniscate} \(r^2 = 16 \cos(2\theta)\)

Solution

We first plot the fundamental cycle of \(r = 4 - 2\sin(\theta)\) on the \(\theta r\)-axes. To help us visualize what is going on graphically, we divide up \([0,2\pi]\) into the usual four subintervals \(\left[0, \frac{\pi}{2}\right]\), \(\left[\frac{\pi}{2}, \pi\right]\), \(\left[\pi, \frac{3\pi}{2}\right]\) and \(\left[\frac{3\pi}{2}, 2\pi \right]\), and proceed as we did above. As \(\theta\) ranges from \(0\) to \(\frac{\pi}{2}\), \(r\) decreases from \(4\) to \(2\). This means that the curve in the \(xy\)-plane starts \(4\) units from the origin on the positive \(x\)-axis and gradually pulls in towards the origin as it moves towards the positive \(y\)-axis.

 

Next, as \(\theta\) runs from \(\frac{\pi}{2}\) to \(\pi\), we see that \(r\) increases from \(2\) to \(4\). Picking up where we left off, we gradually pull the graph away from the origin until we reach the negative \(x\)-axis.

 

Over the interval \(\left[\pi, \frac{3\pi}{2}\right]\), we see that \(r\) increases from \(4\) to \(6\). On the \(xy\)-plane, the curve sweeps out away from the origin as it travels from the negative \(x\)-axis to the negative \(y\)-axis.

 

Finally, as \(\theta\) takes on values from \(\frac{3\pi}{2}\) to \(2\pi\), \(r\) decreases from \(6\) back to \(4\). The graph on the \(xy\)-plane pulls in from the negative \(y\)-axis to finish where we started.

 

We leave it to the reader to verify that plotting points corresponding to values of \(\theta\) outside the interval \([0,2\pi]\) results in retracing portions of the curve, so we are finished.

 

The first thing to note when graphing \(r = 2 + 4\cos(\theta)\) on the \(\theta r\)-plane over the interval \([0,2\pi]\) is that the graph crosses through the \(\theta\)-axis. This corresponds to the graph of the curve passing through the origin in the \(xy\)-plane, and our first task is to determine when this happens. Setting \(r=0\) we get \(2 + 4\cos(\theta) = 0\), or \(\cos(\theta) = -\frac{1}{2}\). Solving for \(\theta\) in \([0,2\pi]\) gives \(\theta = \frac{2\pi}{3}\) and \(\theta = \frac{4\pi}{3}\). Since these values of \(\theta\) are important geometrically, we break the interval \([0,2\pi]\) into six subintervals: \(\left[0,\frac{\pi}{2}\right]\), \(\left[\frac{\pi}{2},\frac{2\pi}{3}\right]\), \(\left[\frac{2\pi}{3},\pi\right]\), \(\left[\pi,\frac{4\pi}{3}\right]\), \(\left[\frac{4\pi}{3}, \frac{3\pi}{2}\right]\) and \(\left[\frac{3\pi}{2}, 2\pi\right]\). As \(\theta\) ranges from \(0\) to \(\frac{\pi}{2}\), \(r\) decreases from \(6\) to \(2\). Plotting this on the \(xy\)-plane, we start \(6\) units out from the origin on the positive \(x\)-axis and slowly pull in towards the positive \(y\)-axis.

 

On the interval \(\left[\frac{\pi}{2}, \frac{2\pi}{3}\right]\), \(r\) decreases from \(2\) to \(0\), which means the graph is heading into (and will eventually cross through) the origin. Not only do we reach the origin when \(\theta = \frac{2\pi}{3}\), a theorem from Calculus\footnote{The `tangents at the pole' theorem from second semester Calculus.} states that the curve hugs the line \(\theta = \frac{2\pi}{3}\) as it approaches the origin.

 

On the interval \(\left[\frac{2\pi}{3}, \pi\right]\), \(r\) ranges from \(0\) to \(-2\). Since \(r \leq 0\), the curve passes through the origin in the \(xy\)-plane, following the line \(\theta = \frac{2\pi}{3}\) and continues upwards through Quadrant IV towards the positive \(x\)-axis.\footnote{Recall that one way to visualize plotting polar coordinates \((r,\theta)\) with \(r<0\) is to start the rotation from the left side of the pole - in this case, the negative \(x\)-axis. Rotating between \(\frac{2\pi}{3}\) and \(\pi\) radians from the negative \(x\)-axis in this case determines the region between the line \(\theta = \frac{2\pi}{3}\) and the \(x\)-axis in Quadrant IV.} Since \(|r|\) is increasing from \(0\) to \(2\), the curve pulls away from the origin to finish at a point on the positive \(x\)-axis.

 

\end{center}

Next, as \(\theta\) progresses from \(\pi\) to \(\frac{4\pi}{3}\), \(r\) ranges from \(-2\) to \(0\). Since \(r \leq 0\), we continue our graph in the first quadrant, heading into the origin along the line \(\theta = \frac{4\pi}{3}\).

 

On the interval \(\left[\frac{4\pi}{3}, \frac{3\pi}{2}\right]\), \(r\) returns to positive values and increases from \(0\) to \(2\). We hug the line \(\theta = \frac{4\pi}{3}\) as we move through the origin and head towards the negative \(y\)-axis.

 

As we round out the interval, we find that as \(\theta\) runs through \(\frac{3\pi}{2}\) to \(2\pi\), \(r\) increases from \(2\) out to \(6\), and we end up back where we started, \(6\) units from the origin on the positive \(x\)-axis.

 

As usual, we start by graphing a fundamental cycle of \(r = 5\sin(2\theta)\) in the \(\theta r\)-plane, which in this case, occurs as \(\theta\) ranges from \(0\) to \(\pi\). We partition our interval into subintervals to help us with the graphing, namely \(\left[0, \frac{\pi}{4}\right]\), \(\left[\frac{\pi}{4}, \frac{\pi}{2}\right]\), \(\left[\frac{\pi}{2},\frac{3\pi}{4}\right]\) and \(\left[\frac{3\pi}{4}, \pi \right]\). As \(\theta\) ranges from \(0\) to \(\frac{\pi}{4}\), \(r\) increases from \(0\) to \(5\). This means that the graph of \(r = 5\sin(2\theta)\) in the \(xy\)-plane starts at the origin and gradually sweeps out so it is \(5\) units away from the origin on the line \(\theta = \frac{\pi}{4}\).

 

Next, we see that \(r\) decreases from \(5\) to \(0\) as \(\theta\) runs through \(\left[\frac{\pi}{4}, \frac{\pi}{2}\right]\), and furthermore, \(r\) is heading negative as \(\theta\) crosses \(\frac{\pi}{2}\). Hence, we draw the curve hugging the line \(\theta = \frac{\pi}{2}\) (the \(y\)-axis) as the curve heads to the origin.

 

 

 

Even though we have finished with one complete cycle of \(r = 5\sin(2\theta)\), if we continue plotting beyond \(\theta = \pi\), we find that the curve continues into the third quadrant! Below we present a graph of a second cycle of \(r = 5\sin(2\theta)\) which continues on from the first. The boxed labels on the \(\theta\)-axis correspond to the portions with matching labels on the curve in the \(xy\)-plane.

 

 

 

Graphing \(r^2 = 16 \cos(2\theta)\) is complicated by the \(r^2\), so we solve to get \(r = \pm \sqrt{16 \cos(2\theta)} = \pm 4 \sqrt{\cos(2\theta)}\). How do we sketch such a curve? First off, we sketch a fundamental period of \(r = \cos(2\theta)\) which we have dotted in the figure below. When \(\cos(2\theta) < 0\), \(\sqrt{\cos(2\theta)}\) is undefined, so we don't have any values on the interval \(\left(\frac{\pi}{4}, \frac{3\pi}{4}\right)\). On the intervals which remain, \(\cos(2\theta)\) ranges from \(0\) to \(1\), inclusive. Hence, \(\sqrt{\cos(2\theta)}\) ranges from \(0\) to \(1\) as well.\footnote{Owing to the relationship between \(y = x\) and \(y = \sqrt{x}\) over \([0,1]\), we also know \(\sqrt{\cos(2\theta)} \geq \cos(2\theta)\) wherever the former is defined.} From this, we know \(r = \pm 4 \sqrt{\cos(2\theta)}\) ranges continuously from \(0\) to \(\pm 4\), respectively. Below we graph both \(r = 4\sqrt{\cos(2\theta)}\) and \(r = -4\sqrt{\cos(2\theta)}\) on the \(\theta r\) plane and use them to sketch the corresponding pieces of the curve \(r^2 = 16\cos(2\theta)\) in the \(xy\)-plane. As we have seen in earlier examples, the lines \(\theta = \frac{\pi}{4}\) and \(\theta = \frac{3\pi}{4}\), which are the zeros of the functions \(r = \pm 4 \sqrt{\cos(2\theta)}\), serve as guides for us to draw the curve as is passes through the origin.

 

As we plot points corresponding to values of \(\theta\) outside of the interval \([0,\pi]\), we find ourselves retracing parts of the curve,\footnote{In this case, we could have generated the entire graph by using just the plot \(r = 4\sqrt{\cos(2\theta)}\), but graphed over the interval \([0,2\pi]\) in the \(\theta r\)-plane. We leave the details to the reader.} so our final answer is below.

A few remarks are in order. First, there is no relation, in general, between the period of the function \(f(\theta)\) and the length of the interval required to sketch the complete graph of \(r = f(\theta)\) in the \(xy\)-plane. As we saw on page \pageref{circletangenttoyaxis}, despite the fact that the period of \(f(\theta) = 6\cos(\theta)\) is \(2\pi\), we sketched the complete graph of \(r = 6\cos(\theta)\) in the \(xy\)-plane just using the values of \(\theta\) as \(\theta\) ranged from \(0\) to \(\pi\). In Example \ref{polargraphex}, number \ref{rose}, the period of \(f(\theta) = 5\sin(2\theta)\) is \(\pi\), but in order to obtain the complete graph of \(r = 5\sin(2\theta)\), we needed to run \(\theta\) from \(0\) to \(2\pi\). While many of the \index{lima\c{c}on} \index{polar rose} \index{lemniscate} `common' polar graphs can be grouped into families,\footnote{Numbers \ref{limacon01} and \ref{limacon02} in Example \ref{polargraphex} are examples of `\href{http://en.wikipedia.org/wiki/Limacon...lima\c{c}ons}},' number \ref{rose} is an example of a `\href{http://en.wikipedia.org/wiki/Rose_(m...nderline{polar rose}},' and number \ref{lemniscate} is the famous `\href{http://en.wikipedia.org/wiki/Lemnisc...ine{Lemniscate of Bernoulli}}.'} the authors truly feel that taking the time to work through each graph in the manner presented here is the best way to not only understand the polar coordinate system, but also prepare you for what is needed in Calculus. Second, the symmetry seen in the examples is also a common occurrence when graphing polar equations. In addition to the usual kinds of symmetry discussed up to this point in the text (symmetry about each axis and the origin), it is possible to talk about \textit{rotational} symmetry. We leave the discussion of symmetry to the Exercises. In our next example, we are given the task of finding the intersection points of polar curves. According to the Fundamental Graphing Principle for Polar Equations on page \pageref{fgpp}, in order for a point \(P\) to be on the graph of a polar equation, it must have a \textit{representation} \(P(r,\theta)\) which satisfies the equation. What complicates matters in polar coordinates is that any given point has infinitely many representations. As a result, if a point \(P\) is on the graph of two different polar equations, it is entirely possible that the representation \(P(r,\theta)\) which satisfies one of the equations does not satisfy the other equation. Here, more than ever, we need to rely on the Geometry as much as the Algebra to find our solutions.

Example \(\PageIndex{1}\):

\label{polargraphintex} Find the points of intersection of the graphs of the following polar equations.

  1. \label{circcardint} \(r =2\sin(\theta)\) and \(r = 2 - 2\sin(\theta)\)
  2. \(r = 2\) and \(r = 3\cos(\theta)\)
  3. \label{circroseint} \(r=3\) and \(r = 6\cos(2\theta)\)
  4. \label{samepolarcurveex} \(r = 3\sin\left(\frac{\theta}{2}\right)\) and \(r = 3\cos\left(\frac{\theta}{2}\right)\)

 Solution

Following the procedure in Example \ref{polargraphex}, we graph \(r = 2\sin(\theta)\) and find it to be a circle centered at the point with rectangular coordinates \((0,1)\) with a radius of \(1\). The graph of \(r = 2-2\sin(\theta)\) is a special kind of lima\c{c}on called a \index{cardioid} `\href{http://en.wikipedia.org/wiki/Cardioi...ote{Presumably, the name is derived from its resemblance to a stylized human heart.}

 

 

 

It appears as if there are three intersection points: one in the first quadrant, one in the second quadrant, and the origin. Our next task is to find polar representations of these points. In order for a point \(P\) to be on the graph of \(r = 2\sin(\theta)\), it must have a representation \(P(r,\theta)\) which satisfies \(r = 2\sin(\theta)\). If \(P\) is also on the graph of \(r = 2 - 2\sin(\theta)\), then \(P\) has a (possibly different) representation \(P(r',\theta')\) which satisfies \(r'=2\sin(\theta')\). We first try to see if we can find any points which have a single representation \(P(r,\theta)\) that satisfies both \(r = 2\sin(\theta)\) and \(r = 2-2\sin(\theta)\). Assuming such a pair \((r,\theta)\) exists, then equating\footnote{We are really using the technique of substitution to solve the system of equations \(\left\{ \begin{array}{rcl} r & = & 2\sin(\theta) \\ r & = & 2-2\sin(\theta) \\ \end{array} \right.\)} the expressions for \(r\) gives \(2\sin(\theta) = 2-2\sin(\theta)\) or \(\sin(\theta) = \frac{1}{2}\). From this, we get \(\theta = \frac{\pi}{6} + 2\pi k\) or \(\theta = \frac{5\pi}{6} + 2\pi k\) for integers \(k\). Plugging \(\theta = \frac{\pi}{6}\) into \(r = 2\sin(\theta)\), we get \(r = 2\sin\left(\frac{\pi}{6}\right) = 2\left(\frac{1}{2}\right) = 1\), which is also the value we obtain when we substitute it into \(r = 2-2\sin(\theta)\). Hence, \(\left(1, \frac{\pi}{6}\right)\) is one representation for the point of intersection in the first quadrant. For the point of intersection in the second quadrant, we try \(\theta = \frac{5\pi}{6}\). Both equations give us the point \(\left(1, \frac{5\pi}{6}\right)\), so this is our answer here. What about the origin? We know from Section \ref{IntroPolar} that the pole may be represented as \((0,\theta)\) for any angle \(\theta\). On the graph of \(r = 2\sin(\theta)\), we start at the origin when \(\theta =0\) and return to it at \(\theta = \pi\), and as the reader can verify, we are at the origin exactly when \(\theta = \pi k\) for integers \(k\). On the curve \(r = 2 - 2\sin(\theta)\), however, we reach the origin when \(\theta = \frac{\pi}{2}\), and more generally, when \(\theta = \frac{\pi}{2} + 2\pi k\) for integers \(k\). There is no integer value of \(k\) for which \(\pi k = \frac{\pi}{2} + 2\pi k\) which means while the origin is on both graphs, the point is never reached simultaneously. In any case, we have determined the three points of intersection to be \(\left(1, \frac{\pi}{6}\right)\), \(\left(1,\frac{5\pi}{6}\right)\) and the origin.

As before, we make a quick sketch of \(r = 2\) and \(r =3\cos(\theta)\) to get feel for the number and location of the intersection points. The graph of \(r=2\) is a circle, centered at the origin, with a radius of \(2\). The graph of \(r = 3\cos(\theta)\) is also a circle - but this one is centered at the point with rectangular coordinates \(\left(\frac{3}{2}, 0\right)\) and has a radius of \(\frac{3}{2}\).

 

 

 

We have two intersection points to find, one in Quadrant I and one in Quadrant IV. Proceeding as above, we first determine if any of the intersection points \(P\) have a representation \((r,\theta)\) which satisfies both \(r=2\) and \(r=3\cos(\theta)\). Equating these two expressions for \(r\), we get \(\cos(\theta) = \frac{2}{3}\). To solve this equation, we need the arccosine function. We get \(\theta = \arccos\left(\frac{2}{3}\right) + 2\pi k\) or \(\theta = 2\pi - \arccos\left(\frac{2}{3}\right) + 2\pi k\) for integers \(k\). From these solutions, we get \(\left(2, \arccos\left(\frac{2}{3}\right)\right)\) as one representation for our answer in Quadrant I, and \(\left(2, 2\pi - \arccos\left(\frac{2}{3}\right)\right)\) as one representation for our answer in Quadrant IV. The reader is encouraged to check these results algebraically and geometrically.

Proceeding as above, we first graph \(r = 3\) and \(r = 6\cos(2\theta)\) to get an idea of how many intersection points to expect and where they lie. The graph of \(r=3\) is a circle centered at the origin with a radius of \(3\) and the graph of \(r = 6\cos(2\theta)\) is another four-leafed rose.\footnote{See Example \ref{polargraphex} number \ref{rose}.}

 

 

 

It appears as if there are eight points of intersection - two in each quadrant. We first look to see if there any points \(P(r,\theta)\) with a representation that satisfies both \(r=3\) and \(r = 6\cos(2\theta)\). For these points, \(6\cos(2\theta) = 3\) or \(\cos(2\theta) = \frac{1}{2}\). Solving, we get \(\theta = \frac{\pi}{6} + \pi k\) or \(\theta = \frac{5\pi}{6} + \pi k\) for integers \(k\). Out of all of these solutions, we obtain just four distinct points represented by \(\left(3, \frac{\pi}{6}\right)\), \(\left(3, \frac{5\pi}{6} \right)\), \(\left(3, \frac{7\pi}{6}\right)\) and \(\left(3, \frac{11\pi}{6} \right)\). To determine the coordinates of the remaining four points, we have to consider how the representations of the points of intersection can differ. We know from Section \ref{IntroPolar} that if \((r,\theta)\) and \((r', \theta')\) represent the same point and \(r \neq 0\), then either \(r = r'\) or \(r = -r'\). If \(r = r'\), then \(\theta' = \theta + 2\pi k\), so one possibility is that an intersection point \(P\) has a representation \((r,\theta)\) which satisfies \(r=3\) and another representation \((r, \theta + 2\pi k)\) for some integer, \(k\) which satisfies \(r = 6\cos(2\theta)\). At this point,\footnote{The authors have chosen to replace \(\theta\) with \(\theta + 2\pi k\) in the equation \(r = 6\cos(2\theta)\) for illustration purposes only. We could have just as easily chosen to do this substitution in the equation \(r = 3\). Since there is no \(\theta\) in \(r=3\), however, this case would reduce to the previous case instantly. The reader is encouraged to follow this latter procedure in the interests of efficiency.}f we replace every occurrence of \(\theta\) in the equation \(r=6\cos(2\theta)\) with \((\theta + 2\pi k)\) and then see if, by equating the resulting expressions for \(r\), we get any more solutions for \(\theta\). Since \(\cos(2(\theta + 2\pi k)) = \cos(2\theta + 4\pi k) = \cos(2\theta)\) for every integer \(k\), however, the equation \(r = 6\cos(2(\theta + 2\pi k))\) reduces to the same equation we had before, \(r = 6\cos(2\theta)\), which means we get no additional solutions. Moving on to the case where \(r = -r'\), we have that \(\theta' = \theta + (2k+1)\pi\) for integers \(k\). We look to see if we can find points \(P\) which have a representation \((r,\theta)\) that satisfies \(r=3\) and another, \((-r, \theta + (2k+1)\pi)\), that satisfies \(r = 6\cos(2\theta)\). To do this, we substitute\footnote{Again, we could have easily chosen to substitute these into \(r=3\) which would give \(-r=3\), or \(r=-3\).} \((-r)\) for \(r\) and \((\theta + (2k+1)\pi)\) for \(\theta\) in the equation \(r = 6\cos(2\theta)\) and get \(-r = 6\cos(2(\theta + (2k+1)\pi))\). Since \(\cos(2(\theta + (2k+1)\pi)) = \cos(2\theta + (2k+1)(2\pi)) = \cos(2\theta)\) for all integers \(k\), the equation \(-r = 6\cos(2(\theta + (2k+1)\pi))\) reduces to \(-r = 6\cos(2\theta)\), or \(r = -6\cos(2\theta)\). Coupling this equation with \(r=3\) gives \(-6\cos(2\theta) = 3\) or \(\cos(2\theta) = -\frac{1}{2}\). We get \(\theta = \frac{\pi}{3} + \pi k\) or \(\theta = \frac{2\pi}{3} + \pi k\). From these solutions, we obtain\footnote{We obtain these representations by substituting the values for \(\theta\) into \(r = 6\cos(2\theta)\), once again, for illustration purposes. Again, in the interests of efficiency, we could `plug' these values for \(\theta\) into \(r=3\) (where there is no \(\theta\)) and get the list of points: \(\left(3, \frac{\pi}{3}\right)\), \(\left(3, \frac{2\pi}{3}\right)\), \(\left(3, \frac{4\pi}{3}\right)\) and \(\left(3, \frac{5\pi}{3}\right)\). While it is not true that \(\left(3, \frac{\pi}{3}\right)\) represents the same point as \(\left(-3, \frac{\pi}{3}\right)\), we still get the same \textit{set} of solutions.} the remaining four intersection points with representations \(\left(-3, \frac{\pi}{3}\right)\), \(\left(-3, \frac{2\pi}{3}\right)\), \(\left(-3, \frac{4\pi}{3}\right)\) and \(\left(-3, \frac{5\pi}{3}\right)\), which we can readily check graphically.

As usual, we begin by graphing \(r = 3\sin\left(\frac{\theta}{2}\right)\) and \(r = 3\cos\left(\frac{\theta}{2}\right)\). Using the techniques presented in Example \ref{polargraphex}, we find that we need to plot both functions as \(\theta\) ranges from \(0\) to \(4\pi\) to obtain the complete graph. To our surprise and/or delight, it appears as if these two equations describe the \textit{same} curve!

 

 

 

To verify this incredible claim,\footnote{A quick sketch of \(r = 3\sin\left(\frac{\theta}{2}\right)\) and \(r= 3\cos\left(\frac{\theta}{2}\right)\) in the \(\theta r\)-plane will convince you that, viewed as functions of \(r\), these are two different animals.} we need to show that, in fact, the graphs of these two equations intersect at all points on the plane. Suppose \(P\) has a representation \((r,\theta)\) which satisfies both \(r = 3\sin\left(\frac{\theta}{2}\right)\) and \(r = 3\cos\left(\frac{\theta}{2}\right)\). Equating these two expressions for \(r\) gives the equation \(3\sin\left(\frac{\theta}{2}\right) = 3\cos\left(\frac{\theta}{2}\right)\). While normally we discourage dividing by a variable expression (in case it could be \(0\)), we note here that if \(3\cos\left(\frac{\theta}{2}\right) = 0\), then for our equation to hold, \( 3\sin\left(\frac{\theta}{2}\right) = 0\) as well. Since no angles have both cosine and sine equal to zero, we are safe to divide both sides of the equation \(3\sin\left(\frac{\theta}{2}\right) = 3\cos\left(\frac{\theta}{2}\right)\) by \(3\cos\left(\frac{\theta}{2}\right)\) to get \(\tan\left(\frac{\theta}{2}\right) = 1\) which gives \(\theta = \frac{\pi}{2} + 2\pi k\) for integers \(k\). From these solutions, however, we get only \textit{one} intersection point which can be represented by \(\left( \frac{3\sqrt{2}}{2}, \frac{\pi}{2}\right)\). We now investigate other representations for the intersection points. Suppose \(P\) is an intersection point with a representation \((r,\theta)\) which satisfies \(r = 3\sin\left(\frac{\theta}{2}\right)\) and the same point \(P\) has a different representation \((r, \theta + 2\pi k)\) for some integer \(k\) which satisfies \(r = 3\cos\left(\frac{\theta}{2}\right)\). Substituting into the latter, we get \(r = 3\cos\left(\frac{1}{2} \left[ \theta + 2\pi k\right]\right) = 3\cos\left(\frac{\theta}{2} + \pi k\right)\). Using the sum formula for cosine, we expand \(3\cos\left(\frac{\theta}{2} + \pi k\right) = 3\cos\left(\frac{\theta}{2}\right) \cos(\pi k) - 3\sin\left(\frac{\theta}{2}\right)\sin\left(\pi k\right) = \pm 3\cos\left(\frac{\theta}{2}\right)\), since \(\sin(\pi k) = 0\) for all integers \(k\), and \(\cos\left(\pi k\right) = \pm 1\) for all integers \(k\). If \(k\) is an even integer, we get the same equation \(r = 3\cos\left(\frac{\theta}{2}\right)\) as before. If \(k\) is odd, we get \(r = -3\cos\left(\frac{\theta}{2}\right)\). This latter expression for \(r\) leads to the equation \(3\sin\left(\frac{\theta}{2}\right) = -3\cos\left(\frac{\theta}{2}\right)\), or \(\tan\left(\frac{\theta}{2}\right) = -1\). Solving, we get \(\theta = -\frac{\pi}{2} + 2\pi k\) for integers \(k\), which gives the intersection point \(\left(\frac{3\sqrt{2}}{2},-\frac{\pi}{2}\right)\). Next, we assume \(P\) has a representation \((r,\theta)\) which satisfies \(r=3\sin\left(\frac{\theta}{2}\right)\) and a representation \((-r, \theta + (2k+1)\pi)\) which satisfies \(r = 3\cos\left(\frac{\theta}{2}\right)\) for some integer \(k\). Substituting \((-r)\) for \(r\) and \((\theta + (2k+1)\pi)\) in for \(\theta\) into \(r = 3\cos\left(\frac{\theta}{2}\right)\) gives \(-r = 3\cos\left(\frac{1}{2}\left[ \theta + (2k+1)\pi\right]\right)\). Once again, we use the sum formula for cosine to get

\[ \begin{array}{rcl} \cos\left(\frac{1}{2}\left[ \theta + (2k+1)\pi\right]\right) & = & \cos\left(\frac{\theta}{2} + \frac{(2k+1)\pi}{2} \right) \\ & = & \cos\left(\frac{\theta}{2}\right) \cos\left(\frac{(2k+1)\pi}{2}\right) - \sin\left(\frac{\theta}{2}\right) \sin\left(\frac{(2k+1)\pi}{2}\right) \\ & = & \pm \sin\left(\frac{\theta}{2}\right) \\ \end{array}\]

where the last equality is true since \(\cos\left(\frac{(2k+1)\pi}{2}\right) = 0\) and \(\sin\left(\frac{(2k+1)\pi}{2}\right) = \pm 1\) for integers \(k\). Hence, \(-r = 3\cos\left(\frac{1}{2}\left[ \theta + (2k+1)\pi\right]\right)\) can be rewritten as \(r = \pm 3 \sin\left(\frac{\theta}{2}\right)\). If we choose \(k = 0\), then \(\sin\left(\frac{(2k+1)\pi}{2}\right) = \sin\left(\frac{\pi}{2}\right)= 1\), and the equation \(-r = 3\cos\left(\frac{1}{2}\left[ \theta + (2k+1)\pi\right]\right)\) in this case reduces to \(-r = -3\sin\left(\frac{\theta}{2}\right)\), or \(r = 3\sin\left(\frac{\theta}{2}\right)\) which is the other equation under consideration! What this means is that if a polar representation \((r,\theta)\) for the point \(P\) satisfies \(r = 3\sin(\frac{\theta}{2})\), then the representation \((-r, \theta + \pi)\) for \(P\) automatically satisfies \(r = 3\cos\left(\frac{\theta}{2}\right)\). Hence the equations \(r = 3\sin(\frac{\theta}{2})\) and \(r = 3\cos(\frac{\theta}{2})\) determine the same set of points in the plane. \qed

Our work in Example \ref{polargraphintex} justifies the following.

Note: Guidelines for Finding Points of Intersection of Graphs of Polar Equations

To find the points of intersection of the graphs of two polar equations \(E_{1}\) and \(E_{2}\):

  • Sketch the graphs of \(E_{1}\) and \(E_{2}\). Check to see if the curves intersect at the origin (pole).
  • Solve for pairs \((r,\theta)\) which satisfy both \(E_{1}\) and \(E_{2}\).
  • Substitute \((\theta + 2\pi k)\) for \(\theta\) in either one of \(E_{1}\) or \(E_{2}\) (but not both) and solve for pairs \((r,\theta)\) which satisfy both equations. Keep in mind that \(k\) is an integer.
  • Substitute \((-r)\) for \(r\) and \((\theta + (2k+1)\pi)\) for \(\theta\) in either one of \(E_{1}\) or \(E_{2}\) (but not both) and solve for pairs \((r,\theta)\) which satisfy both equations. Keep in mind that \(k\) is an integer.

Our last example ties together graphing and points of intersection to describe regions in the plane.

Example \(\PageIndex{1}\):\label{polarregionex}

Sketch the region in the \(xy\)-plane described by the following sets.

  1. \(\left\{ (r,\theta) \, | \, 0 \leq r \leq 5\sin(2\theta), \, 0 \leq \theta \leq \frac{\pi}{2} \right\}\)
  2. \(\left\{ (r,\theta) \, | \, 3 \leq r \leq 6 \cos(2\theta), \, 0 \leq \theta \leq \frac{\pi}{6} \right\}\)
  3. \(\left\{ (r,\theta) \, | \, 2+4\cos(\theta) \leq r \leq 0, \, \frac{2\pi}{3} \leq \theta \leq \frac{4\pi}{3} \right\}\)
  4. \( \left\{ (r,\theta) \, | \, 0\leq r \leq 2\sin(\theta), \, 0 \leq \theta \leq \frac{\pi}{6} \right\} \cup \left\{ (r,\theta) \, | \, 0\leq r \leq 2-2\sin(\theta), \, \frac{\pi}{6} \leq \theta \leq \frac{\pi}{2} \right\}\)

Solution

Our first step in these problems is to sketch the graphs of the polar equations involved to get a sense of the geometric situation. Since all of the equations in this example are found in either Example \ref{polargraphex} or Example \ref{polargraphintex}, most of the work is done for us.

  1. We know from Example \ref{polargraphex} number \ref{rose} that the graph of \(r = 5\sin(2\theta)\) is a rose. Moreover, we know from our work there that as \(0 \leq \theta \leq \frac{\pi}{2}\), we are tracing out the `leaf' of the rose which lies in the first quadrant. The inequality \(0 \leq r \leq 5\sin(2\theta)\) means we want to capture all of the points between the origin (\)r=0\)) and the curve \(r = 5\sin(2\theta)\) as \(\theta\) runs through \(\left[0, \frac{\pi}{2}\right]\). Hence, the region we seek is the leaf itself.

 

We know from Example \ref{polargraphintex} number \ref{circroseint} that \(r=3\) and \(r = 6\cos(2\theta)\) intersect at \(\theta = \frac{\pi}{6}\), so the region that is being described here is the set of points whose directed distance \(r\) from the origin is at least \(3\) but no more than \(6\cos(2\theta)\) as \(\theta\) runs from \(0\) to \(\frac{\pi}{6}\). In other words, we are looking at the points outside or on the circle (since \(r \geq 3\)) but inside or on the rose (since \(r \leq 6\cos(2\theta)\)). We shade the region below.

 

From Example \ref{polargraphex} number \ref{limacon02}, we know that the graph of \(r = 2+4\cos(\theta)\) is a lima\c{c}on whose `inner loop' is traced out as \(\theta\) runs through the given values \(\frac{2\pi}{3}\) to \(\frac{4\pi}{3}\). Since the values \(r\) takes on in this interval are non-positive, the inequality \(2+4\cos(\theta) \leq r \leq 0\) makes sense, and we are looking for all of the points between the pole \(r = 0\) and the lima\c{c}on as \(\theta\) ranges over the interval \(\left[\frac{2\pi}{3}, \frac{4\pi}{3}\right]\). In other words, we shade in the inner loop of the lima\c{c}on.

 

We have two regions described here connected with the union symbol `\)\cup\).' We shade each in turn and find our final answer by combining the two. In Example \ref{polargraphintex}, number \ref{circcardint}, we found that the curves \(r = 2\sin(\theta)\) and \(r = 2-2\sin(\theta)\) intersect when \(\theta = \frac{\pi}{6}\). Hence, for the first region, \( \left\{ (r,\theta) \, | \, 0\leq r \leq 2\sin(\theta), 0 \leq \theta \leq \frac{\pi}{6} \right\}\), we are shading the region between the origin (\)r=0\)) out to the circle (\)r = 2\sin(\theta)\)) as \(\theta\) ranges from \(0\) to \(\frac{\pi}{6}\), which is the angle of intersection of the two curves. For the second region, \(\left\{ (r,\theta) \, | \, 0\leq r \leq 2-2\sin(\theta), \frac{\pi}{6} \leq \theta \leq \frac{\pi}{2} \right\}\), \(\theta\) picks up where it left off at \(\frac{\pi}{6}\) and continues to \(\frac{\pi}{2}\). In this case, however, we are shading from the origin (\)r=0\)) out to the cardioid \(r = 2-2\sin(\theta)\) which pulls into the origin at \(\theta = \frac{\pi}{2}\). Putting these two regions together gives us our final answer.

 

Contributors

  • Carl Stitz, Ph.D. (Lakeland Community College) and Jeff Zeager, Ph.D. (Lorain County Community College)