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Calculus · real student question

A figure is bounded by the circles x² + y² − 7y = 0 and x² + y² − 9y = 0 and by the lines y = x/√3 and x = 0. Write the integral for its area in polar coordinates and find the area.

Question

A plane figure is bounded by the lines

x2+y2−7y=0,x2+y2−9y=0,y=x3,x=0.x^2+y^2-7y=0,\qquad x^2+y^2-9y=0,\qquad y=\frac{x}{\sqrt{3}},\qquad x=0.

Write the integral that gives its area in polar coordinates (r,φ)(r,\varphi), then evaluate it.

Step-by-step solution

  1. Convert the two circles to polar form. Substituting x=rcos⁡φx=r\cos\varphi, y=rsin⁡φy=r\sin\varphi turns x2+y2x^2+y^2 into r2r^2, so x2+y2−7y=0x^2+y^2-7y=0 becomes r2−7rsin⁡φ=0r^2-7r\sin\varphi=0, i.e. r(r−7sin⁡φ)=0r(r-7\sin\varphi)=0. Discarding the pole r=0r=0 gives r=7sin⁡φr=7\sin\varphi, and the same work on the second circle gives r=9sin⁡φr=9\sin\varphi. Both are circles through the origin with centres on the yy-axis, so in this region the radius runs from the smaller to the larger:

    7sin⁡φ≤r≤9sin⁡φ.7\sin\varphi \le r \le 9\sin\varphi.

  2. Convert the two straight lines to angles. A line through the origin is a single ray φ=const\varphi=\text{const} in polar coordinates. The line x=0x=0 is the yy-axis, so φ=π2\varphi=\tfrac{\pi}{2}. For y=x3y=\tfrac{x}{\sqrt3} substitute the polar forms: rsin⁡φ=rcos⁡φ3r\sin\varphi=\tfrac{r\cos\varphi}{\sqrt3}, so tan⁡φ=13\tan\varphi=\tfrac{1}{\sqrt3} and φ=π6\varphi=\tfrac{\pi}{6}. The angle therefore sweeps

    π6≤φ≤π2.\frac{\pi}{6}\le\varphi\le\frac{\pi}{2}.

  3. Assemble the area integral. The area element in polar coordinates is dS=r dr dφdS=r\,dr\,d\varphi — the extra factor rr is the Jacobian and is the single most common thing to forget here. With the limits found above,

    S=∫π/6π/2∫7sin⁡φ9sin⁡φr dr dφ.S=\int_{\pi/6}^{\pi/2}\int_{7\sin\varphi}^{9\sin\varphi} r\,dr\,d\varphi.

  4. Do the inner integral in rr. Because the integrand is just rr, the inner integral is a difference of squares, which is why the sin⁡2φ\sin^2\varphi factors out cleanly:

    ∫7sin⁡φ9sin⁡φr dr=(9sin⁡φ)2−(7sin⁡φ)22=81−492sin⁡2φ=16sin⁡2φ.\int_{7\sin\varphi}^{9\sin\varphi} r\,dr=\frac{(9\sin\varphi)^2-(7\sin\varphi)^2}{2}=\frac{81-49}{2}\sin^2\varphi=16\sin^2\varphi.

  5. Integrate in φ\varphi using the power-reduction identity. sin⁡2φ\sin^2\varphi has no elementary antiderivative on sight, so rewrite it as sin⁡2φ=1−cos⁡2φ2\sin^2\varphi=\tfrac{1-\cos 2\varphi}{2}:

    S=∫π/6π/216sin⁡2φ dφ=8∫π/6π/2(1−cos⁡2φ) dφ=8[φ−sin⁡2φ2]π/6π/2.S=\int_{\pi/6}^{\pi/2}16\sin^2\varphi\,d\varphi=8\int_{\pi/6}^{\pi/2}(1-\cos 2\varphi)\,d\varphi=8\left[\varphi-\frac{\sin 2\varphi}{2}\right]_{\pi/6}^{\pi/2}.

  6. Evaluate at the limits. At φ=π2\varphi=\tfrac{\pi}{2}: π2−sin⁡π2=π2\tfrac{\pi}{2}-\tfrac{\sin\pi}{2}=\tfrac{\pi}{2}. At φ=π6\varphi=\tfrac{\pi}{6}: π6−12sin⁡π3=π6−34\tfrac{\pi}{6}-\tfrac{1}{2}\sin\tfrac{\pi}{3}=\tfrac{\pi}{6}-\tfrac{\sqrt3}{4}. Subtracting and multiplying by 88:

    S=8(π2−π6+34)=8⋅π3+23=8π3+23≈11.84.S=8\left(\frac{\pi}{2}-\frac{\pi}{6}+\frac{\sqrt3}{4}\right)=8\cdot\frac{\pi}{3}+2\sqrt3=\frac{8\pi}{3}+2\sqrt3\approx 11.84.

    A numeric check of the same integral confirms 11.841711.8417, so the closed form is right.

Answer

S=∫π/6π/2∫7sin⁡φ9sin⁡φr dr dφ=8π3+23≈11.84S=\int_{\pi/6}^{\pi/2}\int_{7\sin\varphi}^{9\sin\varphi} r\,dr\,d\varphi=\frac{8\pi}{3}+2\sqrt{3}\approx 11.84

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