Ma · Mathematics

How to Integrate This Double Integral in Polar Coordinates

Published By the 9to5Science editorial team

At a glance

  1. 1. Read the region

    The upper curve is the circle (x − 1)² + y² = 1, with x restricted to at least 1.

  2. 2. Convert the boundaries

    The circle gives r = 2 cos θ; x ≥ 1 gives r ≥ sec θ.

  3. 3. Find the angle range

    The radial bounds meet when sec θ = 2 cos θ, so 0 ≤ θ ≤ π/4.

  4. 4. Integrate with the Jacobian

    Replace the integrand and area element by r⁻³ dr dθ, then evaluate.

Interpreting the integral as

∫12∫02x−x21(x2+y2)2 dy dx,\int_1^2\int_0^{\sqrt{2x-x^2}}\frac{1}{(x^2+y^2)^2}\,dy\,dx,

the key is to describe its region in polar coordinates before changing the integrand. The upper boundary is part of a circle, while the lower bound x≥1x\ge1 cuts away the portion near the origin. Those two boundaries determine both the radial limits and the angular range.

Identify the region

The condition on yy implies

y2≤2x−x2,y^2\le 2x-x^2,

so

x2+y2≤2x⟺(x−1)2+y2≤1.x^2+y^2\le2x \quad\Longleftrightarrow\quad (x-1)^2+y^2\le1.

This is the disk centered at (1,0)(1,0) with radius 11. Since yy runs from zero to the upper semicircle, only the upper half is included. The outer integral further restricts the region to x≥1x\ge1. The bound x≤2x\le2 is already satisfied throughout this disk.

In polar coordinates, x=rcos⁡θx=r\cos\theta and y=rsin⁡θy=r\sin\theta. The circle boundary becomes

r2≤2rcos⁡θ,r^2\le2r\cos\theta,

or r≤2cos⁡θr\le2\cos\theta for points in this region. The vertical boundary x=1x=1 becomes rcos⁡θ=1r\cos\theta=1, so points to its right satisfy r≥sec⁡θr\ge\sec\theta.

Determine the angular limits

The ray at angle θ\theta intersects the region only if its lower radial bound does not exceed its upper radial bound:

sec⁡θ≤2cos⁡θ.\sec\theta\le2\cos\theta.

For angles in the upper half-plane and with x≥1x\ge1, cos⁡θ>0\cos\theta>0. Multiplying by cos⁡θ\cos\theta gives 1≤2cos⁡2θ1\le2\cos^2\theta, hence cos⁡θ≥1/2\cos\theta\ge1/\sqrt2. The region is above the xx-axis, so θ≥0\theta\ge0. Therefore,

0≤θ≤π4,sec⁡θ≤r≤2cos⁡θ.0\le\theta\le\frac{\pi}{4}, \qquad \sec\theta\le r\le2\cos\theta.

At θ=π/4\theta=\pi/4, the two radial boundaries meet. This gives the corner point where the line x=1x=1 meets the circle.

Transform and evaluate the integral

Since x2+y2=r2x^2+y^2=r^2, the integrand is r−4r^{-4}. The polar area element is dA=r dr dθdA=r\,dr\,d\theta, so the transformed integrand is r−3r^{-3}—not r−4r^{-4}.

Thus the integral is

I=∫0π/4∫sec⁡θ2cos⁡θr−3 dr dθ=∫0π/4[−12r2]sec⁡θ2cos⁡θ dθ=12∫0π/4(cos⁡2θ−14cos⁡2θ) dθ.\begin{aligned} I&=\int_0^{\pi/4}\int_{\sec\theta}^{2\cos\theta}r^{-3}\,dr\,d\theta\\ &=\int_0^{\pi/4}\left[-\frac{1}{2r^2}\right]_{\sec\theta}^{2\cos\theta}\,d\theta\\ &=\frac12\int_0^{\pi/4}\left(\cos^2\theta-\frac{1}{4\cos^2\theta}\right)\,d\theta. \end{aligned}

Evaluate the two terms using ∫cos⁡2θ dθ=θ/2+sin⁡(2θ)/4\int\cos^2\theta\,d\theta=\theta/2+\sin(2\theta)/4 and ∫sec⁡2θ dθ=tan⁡θ\int\sec^2\theta\,d\theta=\tan\theta:

I=12(π8+14)−18(1)=π16.\begin{aligned} I&=\frac12\left(\frac{\pi}{8}+\frac14\right)-\frac18(1)\\ &=\boxed{\frac{\pi}{16}}. \end{aligned}

The constants cancel because the contribution 1/81/8 from the cosine-squared integral is exactly offset by the secant-squared term.

Common mistakes

  • Using the disk’s full radial range. The circle gives r≤2cos⁡θr\le2\cos\theta, but the original condition x≥1x\ge1 also requires r≥sec⁡θr\ge\sec\theta.
  • Choosing the wrong angle range. The upper-half condition gives θ≥0\theta\ge0; requiring the two radial bounds to overlap gives θ≤π/4\theta\le\pi/4.
  • Forgetting the Jacobian. The area element contributes a factor of rr, changing r−4r^{-4} into r−3r^{-3}.
  • Treating x≤2x\le2 as another active boundary. The circle already has rightmost point (2,0)(2,0), so this limit does not further restrict the region.

If the missing upper limit in the written integral was intended to be something other than 2x−x2\sqrt{2x-x^2}, the region and answer may differ. For the displayed interpretation, the value is π/16\pi/16.

References

  1. Calculus: Early Transcendentals — James Stewart

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