第5章 5.22

(1)

r=2sin⁡θr=6sin⁡θr = 2\sin\theta \qquad r = 6\sin\theta

S=12⋅2∫0π/2(6sin⁡θ)2 dθ−12⋅2∫0π/2(2sin⁡θ)2 dθ=36[12θ−14sin⁡2θ]0π2−4[12θ−14sin⁡2θ]0π2S = \frac{1}{2}\cdot 2\int_0^{\pi/2}(6\sin\theta)^2\,d\theta - \frac{1}{2}\cdot 2\int_0^{\pi/2}(2\sin\theta)^2\,d\theta = 36\left[\frac{1}{2}\theta-\frac{1}{4}\sin2\theta\right]_0^{\frac{\pi}{2}} - 4\left[\frac{1}{2}\theta-\frac{1}{4}\sin2\theta\right]_0^{\frac{\pi}{2}}

=9π−π=8π=9\pi-\pi=8\pi

(2)

r=a(1+cos⁡θ)r=2acos⁡θr=a(1+\cos\theta) \qquad r=2a\cos\theta

S=12⋅2∫0π(2acos⁡θ)2 dθ−12⋅2∫0π{a(1+cos⁡θ)}2 dθS=\frac{1}{2}\cdot 2\int_0^\pi (2a\cos\theta)^2\,d\theta-\frac{1}{2}\cdot 2\int_0^\pi \{a(1+\cos\theta)\}^2\,d\theta

=∫0π4a2 1+cos⁡2θ2 dθ−∫0πa2(1+2cos⁡θ+1+cos⁡2θ2)dθ=\int_0^\pi 4a^2\,\frac{1+\cos2\theta}{2}\,d\theta-\int_0^\pi a^2\left(1+2\cos\theta+\frac{1+\cos2\theta}{2}\right)d\theta

=[4a2(12+14sin⁡2θ)]0π−[a2(θ+2sin⁡θ+12θ+14sin⁡2θ)]0π=2πa2−πa2−π2a2=π2a2=\left[4a^2\left(\frac{1}{2}+\frac{1}{4}\sin2\theta\right)\right]_0^\pi-\left[a^2\left(\theta+2\sin\theta+\frac{1}{2}\theta+\frac{1}{4}\sin2\theta\right)\right]_0^\pi=2\pi a^2-\pi a^2-\frac{\pi}{2}a^2=\frac{\pi}{2}a^2

解説: r31bn1z