The previous section discussed a special class of parametric functions called polar functions. We know that \begin{align*} dx &= x'(t) dt\\ dy &= y'(t) dt, \end{align*}
and so we can compute the derivative of \(y\) with respect to \(x\) using differentials:
provided that \(x'(t) \ne 0\). With polar functions we have \begin{align*} x(\theta ) &= r(\theta ) \cdot \cos (\theta ) \\ y(\theta ) &= r(\theta ) \cdot \sin (\theta ), \end{align*}
so \begin{align*} \frac {dy}{dx} &= \frac {y'(\theta )}{x'(\theta )} \\ &= \frac {r'(\theta ) \sin (\theta )+r(\theta ) \cos (\theta )}{r'(\theta )\cos (\theta )-r(\theta )\sin (\theta )} \end{align*}
provided that \(x'(\theta )\ne 0\).
Consequently, \begin{align*} x'(\theta ) &= \answer [given]{-\sin (\theta ) + 2\cos ^2(\theta )-2\sin ^2(\theta )} \\ y'(\theta ) &= \answer [given]{\cos (\theta ) + 4\sin (\theta )\cos (\theta )} \end{align*}
and therefore
Thus the equation of the line (in polarrectangular coordinates) tangent to the limaçon at \(\theta =\pi /4\) is
- \(\cos (\theta )=0\) or
- \(1+4\sin (\theta )=0\).
Let’s examine the case of \(\cos (\theta ) = 0\) first, and restrict to the situation where \(\theta \) is between \(0\) and \(2\pi \). If \(\theta \) is in the interval \([0,\pi ]\), then \(\cos (\theta )=0\) when \(\theta =\answer [given]{\pi /2}\). If \(\theta \) is in the interval \([\pi ,2\pi ]\), then \(\cos (\theta )=0\) when \(\theta =\answer [given]{3\pi /2}\).
The corresponding points in rectangular coordinates are \begin{align*} x(\pi /2) &= \left (1+2\sin (\pi /2)\right )\cdot \cos (\pi /2)\\ &= 0,\\ y(\pi /2) &= \left (1+2\sin (\pi /2)\right )\cdot \sin (\pi /2)\\ &= 3, \end{align*}
meaning \((x,y) = (0,3)\), and \begin{align*} x(3\pi /2) &= \left (1+2\sin (3\pi /2)\right )\cdot \cos (3\pi /2)\\ &= 0,\\ y(3\pi /2) &= \left (1+2\sin (3\pi /2)\right )\cdot \sin (3\pi /2)\\ &= 1, \end{align*}
meaning \((x,y) = (0,1)\).
But the numerator was the product of \(\cos (\theta )\) and another term, namely \(1+4\sin (\theta )\) So the numerator is also zero when \begin{align*} 1+4\sin (\theta )&=0\\ 4\sin (\theta )&=-1\\ \sin (\theta )&=\frac {-1}{4}. \end{align*}
At this point we have a choice to make: We can either apply the arcsin function and solve for \(\theta \), or we can work with \(\sin (\theta )\) directly. Perhaps the easier route is to work with \(\sin (\theta )\) directly. To explore \(\sin (\theta )\), we may choose an algebraic method employing the Pythagorean identity, or a geometric method looking at the unit circle with the Pythagorean theorem. Let’s take the geometric route to compute \(\cos (\theta )\).
meaning \((x,y) = (\sqrt {15}/8, -1/8)\), and \begin{align*} x(\theta ) &= \left (1+2\sin (\theta )\right )\cdot \cos (\theta )\\ &= \left (1+2(-1/4)\right )\cdot (-\sqrt {15}/4)\\ &= -\sqrt {15}/8,\\ y(\theta ) &= \left (1+2\sin (\theta )\right )\cdot \sin (\theta )\\ &= \left (1+2(-1/4)\right )\cdot (-1/4)\\ &= -1/8, \end{align*}
meaning \((x,y) = (-\sqrt {15}/8, -1/8)\).
In summary, the graph of \(r(\theta ) = 1+2\sin (\theta )\) on the interval \([0,2\pi ]\) has horizontal tangent lines at the points
- \((x,y) = (0,\answer [given]{3})\),
- \((x,y) = (0,1)\),
- \((x,y) = (\sqrt {15}/8, -1/8)\), and
- \((x,y) = (-\sqrt {15}/8, -1/8)\).
You can confirm this by looking at the graph below:
We then set this equal to zero and note that the equation is quadratic equation in the variable \(\sin (\theta )\). The quadratic formula gives that \begin{align*} \sin (\theta ) &= \frac {-1\pm \sqrt {\answer [given]{33}}}{8}. \end{align*}
Now we can find cosine using either geometrically via the unit circle or algebraically with the Pythagorean identity. This time, let’s take the more algebraic route with the Pythagorean identity. When \(\sin (\theta ) =\frac {-1+\sqrt {33}}{8}\), then \begin{align*} \cos ^2(\theta ) + \sin ^2(\theta ) &= 1\\ \cos ^2(\theta ) + \left (\frac {-1+\sqrt {33}}{8}\right ) &= 1. \end{align*}
So
So
we see that the graph of \(r(\theta ) =1+2\sin (\theta )\) on \([0,2\pi ]\) has vertical tangent lines at
You can confirm this visually by looking at the graph below:
When the graph of the polar function \(r(\theta )\) intersects the origin (sometimes called the “pole”), then \(r(\alpha )=0\) for some angle \(\alpha \).
The answer to the question above leads us to an interesting point. It tells us the slope of the tangent line at the pole. When a polar graph touches the pole at \(\theta =\alpha \), the equation of the tangent line in polar coordinates at the pole is \(\theta =\alpha \).
Thus the equations of the tangent lines, in polarrectangular coordinates, are \begin{align*} \theta &=7\pi /6 \theta \\ \theta &= \answer [given]{11}\pi /6. \end{align*}
In rectangular form, the tangent lines are \(y=\tan (7\pi /6)x\) and \(y=\answer [given]{\tan (11\pi /6)}x\). You can confirm this by looking at the graph below: