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3.14 - Polar Function Graphs

Overview

A polar function r=f(θ)r = f(\theta) takes an angle as its input and gives a radius as its output. Plotting all of those (r,θ)(r, \theta) pairs draws curves that would be messy to write with xx and yy, like circles through the origin, roses, and limaçons. The key skill is connecting the ordinary graph of rr versus θ\theta to the curve it draws in the polar plane.

What the graph of a polar function shows

The graph of r=f(θ)r = f(\theta) is every point with polar coordinates (f(θ),θ)(f(\theta), \theta). Each input is an angle measured from the polar axis, and each output is a signed radius.
Picture a ray spinning counterclockwise around the origin as θ\theta increases. At each angle, f(θ)f(\theta) tells you where the point sits on the line through that ray: f(θ)f(\theta) units out along the ray if it's positive, or ∣f(θ)∣|f(\theta)| units in the opposite direction if it's negative.
  • A change in the input is a change in angle, so the point moves to a different ray.
  • A change in the output is a change in signed radius, so the point moves toward or away from the origin along the line.
  • An output of 0 puts the point at the origin, whatever the angle.

Example 1: Graphing r=4cos⁡θr = 4\cos\theta from a table

Make a table of values for 0≤θ≤π0 \le \theta \le \pi and plot the points.
θ\theta
r=4cos⁡θr = 4\cos\theta
Where the point is
00
44
4 units along the polar axis: (4,0)(4, 0)
π4\frac{\pi}{4}
22≈2.832\sqrt{2} \approx 2.83
on the π4\frac{\pi}{4} ray: (2,2)(2, 2)
π2\frac{\pi}{2}
00
the origin
3π4\frac{3\pi}{4}
−22≈−2.83-2\sqrt{2} \approx -2.83
opposite the 3π4\frac{3\pi}{4} ray, in Quadrant IV: (2,−2)(2, -2)
π\pi
−4-4
opposite the π\pi ray, back at (4,0)(4, 0)
3.14 - Polar Function Graphs
For 0≤θ≤π20 \le \theta \le \frac{\pi}{2}, rr is positive and the point sweeps along the top half of a circle, from (4,0)(4, 0) into the origin (black). For π2<θ≤π\frac{\pi}{2} < \theta \le \pi, rr is negative, so each point lands on the opposite side of the origin, and the bottom half gets drawn (red).
The graph is a circle with center (2,0)(2, 0) and radius 2, traced once for 0≤θ≤π0 \le \theta \le \pi. As θ\theta continues from π\pi to 2π2\pi, the same circle is traced again. (Multiplying both sides by rr gives r2=4rcos⁡θr^2 = 4r\cos\theta, which is x2+y2=4xx^2 + y^2 = 4x, or (x−2)2+y2=4(x - 2)^2 + y^2 = 4 in rectangular form.)

From the graph of rr versus θ\theta to the polar graph

AP questions often show the graph of r=f(θ)r = f(\theta) on ordinary axes, with θ\theta on the horizontal axis and rr on the vertical axis, then ask about the polar curve. Read that graph from left to right. At each angle, ask two questions: how big is rr, and is it positive or negative?

Example 2: The limaçon r=1+2cos⁡θr = 1 + 2\cos\theta (AP-style)

The figure shows r=1+2cos⁡θr = 1 + 2\cos\theta graphed both ways, with matching points labeled. The red parts are where r<0r < 0.
3.14 - Polar Function Graphs
Point
θ\theta
rr
Location in the plane
AA
00
33
(3,0)(3, 0), on the polar axis
BB
π2\frac{\pi}{2}
11
(0,1)(0, 1)
CC
2π3\frac{2\pi}{3}
00
the origin
DD
π\pi
−1-1
(1,0)(1, 0), since a negative rr points opposite the π\pi ray
EE
4π3\frac{4\pi}{3}
00
the origin
FF
3π2\frac{3\pi}{2}
11
(0,−1)(0, -1)
GG
2π2\pi
33
(3,0)(3, 0) again
Now follow the curve in three stages:
  1. A to C (0≤θ≤2π30 \le \theta \le \frac{2\pi}{3}): rr is positive and shrinks from 3 to 0. The point swings from (3,0)(3, 0) up through Quadrants I and II and into the origin. This is the top of the big loop.
  1. C to E (2π3<θ<4π3\frac{2\pi}{3} < \theta < \frac{4\pi}{3}): rr is negative. The rays point into Quadrants II and III, but the points are plotted on the opposite side, in Quadrants IV and I. This traces the small inner loop, and D=(1,0)D = (1, 0) is its point farthest from the origin.
  1. E to G (4π3≤θ≤2π\frac{4\pi}{3} \le \theta \le 2\pi): rr is positive again and grows from 0 to 3, tracing the bottom of the big loop through Quadrants III and IV back to (3,0)(3, 0).
This curve is called a limaçon with an inner loop. The inner loop exists only because rr goes negative.

Restricting the domain

To draw only part of a polar graph, choose an interval of θ\theta whose endpoints are the angles where that part starts and stops. Find those angles from the radius you want at each end. Often the part starts or stops at the origin, so you solve f(θ)=0f(\theta) = 0.

Example 3: Tracing only the inner loop

For r=1+2cos⁡θr = 1 + 2\cos\theta, give an interval of θ\theta that traces just the inner loop.
The inner loop starts and ends at the origin, where r=0r = 0:
1+2cos⁡θ=0⇒cos⁡θ=−12⇒θ=2π3 or 4π31 + 2\cos\theta = 0 \quad\Rightarrow\quad \cos\theta = -\frac{1}{2} \quad\Rightarrow\quad \theta = \frac{2\pi}{3} \text{ or } \frac{4\pi}{3}
Between these angles rr is negative (for example, r=−1r = -1 at θ=π\theta = \pi), which is exactly the inner loop. Answer: 2π3≤θ≤4π3\frac{2\pi}{3} \le \theta \le \frac{4\pi}{3}.

Rose curves

Graphs of r=asin⁡(nθ)r = a\sin(n\theta) and r=acos⁡(nθ)r = a\cos(n\theta), where n≥2n \ge 2 is a whole number, are called roses. Each petal has length ∣a∣|a|, the largest value of ∣r∣|r|.
  • If nn is odd, there are nn petals, and the whole rose is traced once for 0≤θ≤π0 \le \theta \le \pi.
  • If nn is even, there are 2n2n petals, and it takes 0≤θ≤2π0 \le \theta \le 2\pi to trace them all.
3.14 - Polar Function Graphs
r=3sin⁡2θr = 3\sin 2\theta has n=2n = 2, so it has 4 petals of length 3. r=2cos⁡3θr = 2\cos 3\theta has n=3n = 3, so it has 3 petals of length 2, with tips in the directions θ=0\theta = 0, 2π3\frac{2\pi}{3}, and 4π3\frac{4\pi}{3}.

Example 4: Which angles trace which petal?

For r=3sin⁡2θr = 3\sin 2\theta, find an interval of θ\theta that traces only the petal in Quadrant II.
Check the sign of rr on each quarter turn:
Interval
Sign of rr
Petal traced
0≤θ≤π20 \le \theta \le \frac{\pi}{2}
positive
Quadrant I
π2≤θ≤π\frac{\pi}{2} \le \theta \le \pi
negative
Quadrant IV (opposite Quadrant II)
π≤θ≤3π2\pi \le \theta \le \frac{3\pi}{2}
positive
Quadrant III
3π2≤θ≤2π\frac{3\pi}{2} \le \theta \le 2\pi
negative
Quadrant II (opposite Quadrant IV)
Answer: 3π2≤θ≤2π\frac{3\pi}{2} \le \theta \le 2\pi. The obvious guess, π2≤θ≤π\frac{\pi}{2} \le \theta \le \pi, traces the Quadrant IV petal instead, because rr is negative there.

Common polar graphs

The CED doesn't require these names, but recognizing the shapes helps you check your work quickly.
Equation
Graph
r=ar = a
circle centered at the origin with radius ∣a∣|a|
r=acos⁡θr = a\cos\theta
circle through the origin, centered at (a2,0)\left(\frac{a}{2}, 0\right)
r=asin⁡θr = a\sin\theta
circle through the origin, centered at (0,a2)\left(0, \frac{a}{2}\right)
r=asin⁡(nθ)r = a\sin(n\theta) or r=acos⁡(nθ)r = a\cos(n\theta)
rose: nn petals if nn is odd, 2n2n petals if nn is even
r=a+bcos⁡θr = a + b\cos\theta or r=a+bsin⁡θr = a + b\sin\theta, with a,b>0a, b > 0
limaçon: inner loop if a<ba < b, cardioid (heart shape) if a=ba = b, dimpled if b<a<2bb < a < 2b, convex if a≥2ba \ge 2b
3.14 - Polar Function Graphs
The four limaçons above all have b=2b = 2 and are drawn on the same scale. The cosine versions are symmetric about the x-axis. The sine versions are the same shapes turned to be symmetric about the y-axis.

Common mistakes

  • Plotting a negative rr along the ray. A negative radius goes the opposite way, through the origin.
  • Assuming you always need 0≤θ≤2π0 \le \theta \le 2\pi. Some graphs, like r=4cos⁡θr = 4\cos\theta and r=2cos⁡3θr = 2\cos 3\theta, are fully traced by 0≤θ≤π0 \le \theta \le \pi, and going further just retraces them.
  • Miscounting rose petals. An even nn gives 2n2n petals, not nn.
  • Treating the graph of rr versus θ\theta as a picture of the curve. It looks nothing like the polar graph. It's a tool for reading rr at each angle.

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