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Family Table Math

Area in Polar Coordinates

For y=f(x)y = f(x), you found area by stacking thin rectangles. Polar curves sweep out from the pole like the hands of a clock, so the natural slices are thin pie wedges instead. That gives a new area formula. Once you have it, the main skill is choosing the right θ\theta-limits, which means knowing exactly how the curve is traced (see polar coordinates and derivatives).

A sector (pie wedge) of a circle with radius rr and angle Δθ\Delta\theta (in radians) has area 12r2Δθ\dfrac{1}{2}r^2\Delta\theta. For a polar curve r=f(θ)r = f(\theta), the radius changes with θ\theta, but over a tiny angle it’s nearly constant. Add up the thin wedges and let Δθ→0\Delta\theta \to 0:

A=∫αβ12r2 dθ=12∫αβ(f(θ))2 dθA = \int_\alpha^\beta \frac{1}{2}r^2\, d\theta = \frac{1}{2}\int_\alpha^\beta \big( f(\theta) \big)^2\, d\theta

This is the area swept out by the segment from the pole to the curve as θ\theta goes from α\alpha to β\beta. The formula needs radians, and the region should be swept out exactly once (no overlaps).

  • For a whole closed curve, use one full trip around it: often 00 to 2π2\pi, but a circle like r=2asin⁡θr = 2a\sin\theta and a rose with an odd number of petals are each traced once on [0,π][0, \pi].
  • For one petal or loop, find the angles where r=0r = 0 on either side of it. The petal starts and ends at the pole.
  • Use symmetry when it helps: find half (or one petal) and multiply.

Squaring rr often produces sin⁡2\sin^2 or cos⁡2\cos^2. To integrate them, use the power-reducing identities:

sin⁡2θ=1−cos⁡(2θ)2,cos⁡2θ=1+cos⁡(2θ)2\sin^2\theta = \frac{1 - \cos(2\theta)}{2}, \qquad \cos^2\theta = \frac{1 + \cos(2\theta)}{2}
The three-petal rose r = 2 sin 3 theta. The petal traced from theta = 0 to theta = pi/3 is shaded; its tip is at theta = pi/6, distance 2 from the pole. −2 −1 1 2 3 −2 −1 1 2 θ = π/3 tip at θ = π/6 r = 2 sin 3θ x y
One petal of r=2sin⁡3θr = 2\sin 3\theta (Example 2) is swept out as θ\theta goes from 00 to π3\frac{\pi}{3}, starting and ending at the pole.

If R(θ)≥r(θ)≥0R(\theta) \ge r(\theta) \ge 0 for α≤θ≤β\alpha \le \theta \le \beta, the area between them (outside rr, inside RR) is

A=12∫αβ((R(θ))2−(r(θ))2) dθA = \frac{1}{2}\int_\alpha^\beta \Big( \big( R(\theta) \big)^2 - \big( r(\theta) \big)^2 \Big)\, d\theta

That’s outer area minus inner area. Note it is R2−r2R^2 - r^2, not (R−r)2(R - r)^2.

To find where two polar curves cross, solve f(θ)=g(θ)f(\theta) = g(\theta). But that can miss points! The pole is a common point whenever each curve passes through it, even if they reach it at different angles (for example, r=2sin⁡θr = 2\sin\theta is at the pole when θ=0\theta = 0, but r=2cos⁡θr = 2\cos\theta is there when θ=π2\theta = \frac{\pi}{2}). Sketch the curves to see which intersections matter.

Polar area usually appears on the calculator-active section. Write the integral with its limits and the 12\frac{1}{2}, then evaluate numerically and give 33 decimal places. If the intersection angles aren’t nice, find them with your calculator and store them (don’t round to 33 decimals before integrating).

Find the area enclosed by r=4sin⁡θr = 4\sin\theta.

Solution. This circle has radius 22, so we expect π(2)2=4π\pi(2)^2 = 4\pi. It is traced once for 0≤θ≤π0 \le \theta \le \pi (then rr goes negative and the circle is traced again).

A=12∫0π16sin⁡2θ dθ=8∫0π1−cos⁡(2θ)2 dθ=4[θ−sin⁡(2θ)2]0π=4πA = \frac{1}{2}\int_0^{\pi} 16\sin^2\theta\, d\theta = 8\int_0^{\pi} \frac{1 - \cos(2\theta)}{2}\, d\theta = 4\left[ \theta - \frac{\sin(2\theta)}{2} \right]_0^{\pi} = 4\pi

Using 00 to 2π2\pi would give 8π8\pi, counting the circle twice.

Find the area of one petal of r=2sin⁡(3θ)r = 2\sin(3\theta).

Solution. r=0r = 0 when sin⁡(3θ)=0\sin(3\theta) = 0: at θ=0\theta = 0 and next at θ=π3\theta = \dfrac{\pi}{3}. Between them r>0r \gt 0, so one petal is traced for 0≤θ≤π30 \le \theta \le \dfrac{\pi}{3} (see the figure).

A=12∫0π/34sin⁡2(3θ) dθ=2∫0π/31−cos⁡(6θ)2 dθ=[θ−sin⁡(6θ)6]0π/3=π3−sin⁡(2π)6=π3\begin{aligned} A &= \frac{1}{2}\int_0^{\pi/3} 4\sin^2(3\theta)\, d\theta = 2\int_0^{\pi/3} \frac{1 - \cos(6\theta)}{2}\, d\theta \\ &= \left[ \theta - \frac{\sin(6\theta)}{6} \right]_0^{\pi/3} = \frac{\pi}{3} - \frac{\sin(2\pi)}{6} = \frac{\pi}{3} \end{aligned}

The whole rose has 33 petals, so its total area is π\pi.

Example 3: Inside one curve, outside another

Section titled “Example 3: Inside one curve, outside another”

Find the area of the region inside r=4cos⁡θr = 4\cos\theta and outside r=2r = 2.

Solution. Intersections: 4cos⁡θ=24\cos\theta = 2 gives cos⁡θ=12\cos\theta = \dfrac{1}{2}, so θ=±π3\theta = \pm\dfrac{\pi}{3}. Between these angles, the circle r=4cos⁡θr = 4\cos\theta is the outer curve.

The circle r = 4 cos theta and the circle r = 2 cross at theta = pi/3 and theta = -pi/3. The shaded region is inside r = 4 cos theta and outside r = 2. −2 −1 1 2 3 4 −2 −1 1 2 θ = π/3 θ = −π/3 r = 4 cos θ r = 2 x y
The region inside r=4cos⁡θr = 4\cos\theta and outside r=2r = 2, between θ=−π3\theta = -\frac{\pi}{3} and θ=π3\theta = \frac{\pi}{3}.

The region is symmetric about the xx-axis, so double the integral from 00:

A=2⋅12∫0π/3(16cos⁡2θ−4)dθ=∫0π/3(8+8cos⁡(2θ)−4) dθ=[4θ+4sin⁡(2θ)]0π/3=4π3+4⋅32=4π3+23≈7.653\begin{aligned} A &= 2 \cdot \frac{1}{2}\int_0^{\pi/3} \left( 16\cos^2\theta - 4 \right) d\theta = \int_0^{\pi/3} \big( 8 + 8\cos(2\theta) - 4 \big)\, d\theta \\ &= \Big[ 4\theta + 4\sin(2\theta) \Big]_0^{\pi/3} = \frac{4\pi}{3} + 4 \cdot \frac{\sqrt{3}}{2} = \frac{4\pi}{3} + 2\sqrt{3} \approx 7.653 \end{aligned}

Example 4: Inside both curves (don’t forget the pole)

Section titled “Example 4: Inside both curves (don’t forget the pole)”

Find the area of the region inside both r=2sin⁡θr = 2\sin\theta and r=2cos⁡θr = 2\cos\theta.

Solution. Both are circles of radius 11, one centred at (0,1)(0, 1) and one at (1,0)(1, 0). Solving 2sin⁡θ=2cos⁡θ2\sin\theta = 2\cos\theta gives θ=π4\theta = \dfrac{\pi}{4}, the point (1,1)(1, 1). They also both pass through the pole: that’s the other corner of the overlap.

The overlap is a lens. For 0≤θ≤π40 \le \theta \le \dfrac{\pi}{4} its boundary is r=2sin⁡θr = 2\sin\theta (the smaller rr); for π4≤θ≤π2\dfrac{\pi}{4} \le \theta \le \dfrac{\pi}{2} it’s r=2cos⁡θr = 2\cos\theta. By symmetry the two halves are equal:

A=2⋅12∫0π/44sin⁡2θ dθ=2∫0π/4(1−cos⁡(2θ)) dθ=2[θ−sin⁡(2θ)2]0π/4=2(π4−12)=π2−1≈0.571\begin{aligned} A &= 2 \cdot \frac{1}{2}\int_0^{\pi/4} 4\sin^2\theta\, d\theta = 2\int_0^{\pi/4} \big( 1 - \cos(2\theta) \big)\, d\theta \\ &= 2\left[ \theta - \frac{\sin(2\theta)}{2} \right]_0^{\pi/4} = 2\left( \frac{\pi}{4} - \frac{1}{2} \right) = \frac{\pi}{2} - 1 \approx 0.571 \end{aligned}

Forgetting the one-half. The formula is 12∫r2 dθ\frac{1}{2}\int r^2\, d\theta. Without the 12\frac{1}{2}, every answer is doubled.

Forgetting to square r. 12∫r dθ\frac{1}{2}\int r\, d\theta is not an area. Square the whole expression: (1+cos⁡θ)2=1+2cos⁡θ+cos⁡2θ(1 + \cos\theta)^2 = 1 + 2\cos\theta + \cos^2\theta, not 1+cos⁡2θ1 + \cos^2\theta.

Using (R − r)² for the region between curves. The area between is 12∫(R2−r2)dθ\frac{1}{2}\int \left( R^2 - r^2 \right) d\theta: outer area minus inner area. Squaring the difference gives a different (wrong) number.

Going around twice. Circles through the pole and odd-petal roses are traced once on an interval of length π\pi. Integrating over [0,2π][0, 2\pi] counts them twice. Check a sketch or a table of values.

Missing the pole as an intersection. Solving f(θ)=g(θ)f(\theta) = g(\theta) only finds crossings at the same angle. If both curves pass through the pole, it’s also an intersection, as in Example 4.

Degree mode. The formula assumes radians. In degree mode the calculator’s integral is meaningless.

1. (Warm-up) Use the polar area formula to find the area inside r=3r = 3. Check with the circle area formula.

SolutionA=12∫02π9 dθ=92(2π)=9πA = \frac{1}{2}\int_0^{2\pi} 9\, d\theta = \frac{9}{2}(2\pi) = 9\pi

Check: π(3)2=9π\pi(3)^2 = 9\pi.

2. (Warm-up) Find the area swept out by the spiral r=θr = \theta for 0≤θ≤π0 \le \theta \le \pi.

SolutionA=12∫0πθ2 dθ=12[θ33]0π=π36≈5.168A = \frac{1}{2}\int_0^{\pi} \theta^2\, d\theta = \frac{1}{2}\left[ \frac{\theta^3}{3} \right]_0^{\pi} = \frac{\pi^3}{6} \approx 5.168

3. (Warm-up) One petal of r=cos⁡(2θ)r = \cos(2\theta) is traced for −π4≤θ≤π4-\dfrac{\pi}{4} \le \theta \le \dfrac{\pi}{4}. Write the integral for its area, then evaluate it.

SolutionA=12∫−π/4π/4cos⁡2(2θ) dθ=12∫−π/4π/41+cos⁡(4θ)2 dθ=14[θ+sin⁡(4θ)4]−π/4π/4=14⋅π2=π8A = \frac{1}{2}\int_{-\pi/4}^{\pi/4} \cos^2(2\theta)\, d\theta = \frac{1}{2}\int_{-\pi/4}^{\pi/4} \frac{1 + \cos(4\theta)}{2}\, d\theta = \frac{1}{4}\left[ \theta + \frac{\sin(4\theta)}{4} \right]_{-\pi/4}^{\pi/4} = \frac{1}{4} \cdot \frac{\pi}{2} = \frac{\pi}{8}

4. (Core) Find the area enclosed by the cardioid r=2+2cos⁡θr = 2 + 2\cos\theta.

Solution

The cardioid is traced once for 0≤θ≤2π0 \le \theta \le 2\pi.

(2+2cos⁡θ)2=4+8cos⁡θ+4cos⁡2θ=4+8cos⁡θ+2+2cos⁡(2θ)(2 + 2\cos\theta)^2 = 4 + 8\cos\theta + 4\cos^2\theta = 4 + 8\cos\theta + 2 + 2\cos(2\theta)A=12∫02π(6+8cos⁡θ+2cos⁡(2θ)) dθ=12[6θ+8sin⁡θ+sin⁡(2θ)]02π=12(12π)=6πA = \frac{1}{2}\int_0^{2\pi} \big( 6 + 8\cos\theta + 2\cos(2\theta) \big)\, d\theta = \frac{1}{2}\Big[ 6\theta + 8\sin\theta + \sin(2\theta) \Big]_0^{2\pi} = \frac{1}{2}(12\pi) = 6\pi

5. (Core) Find the area of one petal of r=3cos⁡(2θ)r = 3\cos(2\theta), and the total area of the rose.

Solution

r=0r = 0 at θ=±π4\theta = \pm\dfrac{\pi}{4}, so one petal is traced for −π4≤θ≤π4-\dfrac{\pi}{4} \le \theta \le \dfrac{\pi}{4}:

A=12∫−π/4π/49cos⁡2(2θ) dθ=94[θ+sin⁡(4θ)4]−π/4π/4=94⋅π2=9π8A = \frac{1}{2}\int_{-\pi/4}^{\pi/4} 9\cos^2(2\theta)\, d\theta = \frac{9}{4}\left[ \theta + \frac{\sin(4\theta)}{4} \right]_{-\pi/4}^{\pi/4} = \frac{9}{4} \cdot \frac{\pi}{2} = \frac{9\pi}{8}

With n=2n = 2 there are 44 petals, so the total area is 4⋅9π8=9π24 \cdot \dfrac{9\pi}{8} = \dfrac{9\pi}{2}.

6. (Core) Find the area of the region inside the cardioid r=1+cos⁡θr = 1 + \cos\theta and outside the circle r=1r = 1.

Solution

Intersections: 1+cos⁡θ=11 + \cos\theta = 1 gives cos⁡θ=0\cos\theta = 0, so θ=±π2\theta = \pm\dfrac{\pi}{2}. For −π2≤θ≤π2-\dfrac{\pi}{2} \le \theta \le \dfrac{\pi}{2}, cos⁡θ≥0\cos\theta \ge 0 and the cardioid is outside the circle.

A=12∫−π/2π/2((1+cos⁡θ)2−1) dθ=12∫−π/2π/2(2cos⁡θ+cos⁡2θ)dθ=12[2sin⁡θ+θ2+sin⁡(2θ)4]−π/2π/2=12(4+π2)=2+π4≈2.785\begin{aligned} A &= \frac{1}{2}\int_{-\pi/2}^{\pi/2} \Big( (1 + \cos\theta)^2 - 1 \Big)\, d\theta = \frac{1}{2}\int_{-\pi/2}^{\pi/2} \left( 2\cos\theta + \cos^2\theta \right) d\theta \\ &= \frac{1}{2}\left[ 2\sin\theta + \frac{\theta}{2} + \frac{\sin(2\theta)}{4} \right]_{-\pi/2}^{\pi/2} = \frac{1}{2}\left( 4 + \frac{\pi}{2} \right) = 2 + \frac{\pi}{4} \approx 2.785 \end{aligned}

7. (Core) (Calculator active.) Let RR be the region in the first quadrant that is inside the circle r=4cos⁡θr = 4\cos\theta and outside the spiral r=1+θr = 1 + \theta (for θ≥0\theta \ge 0).

  • (a) Find the value of θ\theta where the curves intersect in the first quadrant.
  • (b) Find the area of RR.
Solution

(a) Solve 4cos⁡θ=1+θ4\cos\theta = 1 + \theta with a calculator (radian mode): θ=a≈1.037\theta = a \approx 1.037. Store the full value.

(b) At θ=0\theta = 0 the circle (r=4r = 4) is outside the spiral (r=1r = 1), and it stays outside until θ=a\theta = a. So

A=12∫0a((4cos⁡θ)2−(1+θ)2) dθ≈4.658A = \frac{1}{2}\int_0^{a} \Big( (4\cos\theta)^2 - (1 + \theta)^2 \Big)\, d\theta \approx 4.658

8. (Challenge) The limaçon r=1+2cos⁡θr = 1 + 2\cos\theta has an inner loop. Find the exact area inside the inner loop.

Solution

The inner loop is traced while r≤0r \le 0, between the angles where r=0r = 0: cos⁡θ=−12\cos\theta = -\dfrac{1}{2}, so θ=2π3\theta = \dfrac{2\pi}{3} to 4π3\dfrac{4\pi}{3}. (Squaring makes the negative rr values harmless.)

(1+2cos⁡θ)2=1+4cos⁡θ+4cos⁡2θ=3+4cos⁡θ+2cos⁡(2θ)(1 + 2\cos\theta)^2 = 1 + 4\cos\theta + 4\cos^2\theta = 3 + 4\cos\theta + 2\cos(2\theta)A=12[3θ+4sin⁡θ+sin⁡(2θ)]2π/34π/3A = \frac{1}{2}\Big[ 3\theta + 4\sin\theta + \sin(2\theta) \Big]_{2\pi/3}^{4\pi/3}

At 4π3\dfrac{4\pi}{3}: 4π−23+324\pi - 2\sqrt{3} + \dfrac{\sqrt{3}}{2}. At 2π3\dfrac{2\pi}{3}: 2π+23−322\pi + 2\sqrt{3} - \dfrac{\sqrt{3}}{2}. The difference is 2π−332\pi - 3\sqrt{3}, so

A=π−332≈0.544A = \pi - \frac{3\sqrt{3}}{2} \approx 0.544

9. (Challenge) Find the area of the region inside both the circle r=6cos⁡θr = 6\cos\theta and the cardioid r=2+2cos⁡θr = 2 + 2\cos\theta.

Solution

Intersections: 6cos⁡θ=2+2cos⁡θ6\cos\theta = 2 + 2\cos\theta gives cos⁡θ=12\cos\theta = \dfrac{1}{2}, so θ=±π3\theta = \pm\dfrac{\pi}{3}. Both curves also pass through the pole.

Use the upper half and double it. For 0≤θ≤π30 \le \theta \le \dfrac{\pi}{3}, the cardioid is the inner curve (at θ=0\theta = 0: 4<64 \lt 6). For π3≤θ≤π2\dfrac{\pi}{3} \le \theta \le \dfrac{\pi}{2}, the circle is inner (it reaches the pole at θ=π2\theta = \frac{\pi}{2}).

A=2[12∫0π/3(2+2cos⁡θ)2 dθ+12∫π/3π/236cos⁡2θ dθ]A = 2\left[ \frac{1}{2}\int_0^{\pi/3} (2 + 2\cos\theta)^2\, d\theta + \frac{1}{2}\int_{\pi/3}^{\pi/2} 36\cos^2\theta\, d\theta \right]

First integral: (2+2cos⁡θ)2=6+8cos⁡θ+2cos⁡(2θ)(2 + 2\cos\theta)^2 = 6 + 8\cos\theta + 2\cos(2\theta), so

∫0π/3(2+2cos⁡θ)2 dθ=[6θ+8sin⁡θ+sin⁡(2θ)]0π/3=2π+43+32=2π+932\int_0^{\pi/3} (2 + 2\cos\theta)^2\, d\theta = \Big[ 6\theta + 8\sin\theta + \sin(2\theta) \Big]_0^{\pi/3} = 2\pi + 4\sqrt{3} + \frac{\sqrt{3}}{2} = 2\pi + \frac{9\sqrt{3}}{2}

Second integral:

∫π/3π/236cos⁡2θ dθ=18[θ+sin⁡(2θ)2]π/3π/2=18(π2−π3−34)=3π−932\int_{\pi/3}^{\pi/2} 36\cos^2\theta\, d\theta = 18\left[ \theta + \frac{\sin(2\theta)}{2} \right]_{\pi/3}^{\pi/2} = 18\left( \frac{\pi}{2} - \frac{\pi}{3} - \frac{\sqrt{3}}{4} \right) = 3\pi - \frac{9\sqrt{3}}{2}

Adding (the factor 2⋅12=12 \cdot \frac{1}{2} = 1): A=2π+932+3π−932=5π≈15.708A = 2\pi + \dfrac{9\sqrt{3}}{2} + 3\pi - \dfrac{9\sqrt{3}}{2} = 5\pi \approx 15.708.