第8章 8.6

(1)

0≤r≤2acos⁡θ0 \leq r \leq 2a\cos\theta x=rcos⁡θx = r\cos\theta y=rsin⁡θy = r\sin\theta から

∫−π2π2∫02acos⁡θr2⋅r dr dθ=∫−π2π2[14r4]02acos⁡θdθ=∫−π2π24a4cos⁡4θ dθ=2∫0π24a4cos⁡4θ dθ\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \int_0^{2a\cos\theta} r^2 \cdot r \, dr\, d\theta = \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \left[\frac{1}{4}r^4\right]_0^{2a\cos\theta} d\theta = \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} 4a^4 \cos^4\theta \, d\theta = 2\int_0^{\frac{\pi}{2}} 4a^4 \cos^4\theta \, d\theta

=8a4⋅34⋅12⋅π2=32πa4= 8a^4 \cdot \frac{3}{4} \cdot \frac{1}{2} \cdot \frac{\pi}{2} = \frac{3}{2}\pi a^4

(2)

0≤r≤a(1+cos⁡θ)0 \leq r \leq a(1+\cos\theta) x=rcos⁡θx = r\cos\theta y=rsin⁡θy = r\sin\theta から

∫02π∫0a(1+cos⁡θ)r2⋅r dr dθ=∫02π[14r4]0a(1+cos⁡θ)dθ=∫02π14a4(1+cos⁡θ)4 dθ\int_0^{2\pi} \int_0^{a(1+\cos\theta)} r^2 \cdot r \, dr\, d\theta = \int_0^{2\pi} \left[\frac{1}{4}r^4\right]_0^{a(1+\cos\theta)} d\theta = \int_0^{2\pi} \frac{1}{4}a^4(1+\cos\theta)^4 \, d\theta

=14a4∫02π(1+4cos⁡θ+6cos⁡2θ+4cos⁡3θ+cos⁡4θ) dθ= \frac{1}{4}a^4 \int_0^{2\pi} (1 + 4\cos\theta + 6\cos^2\theta + 4\cos^3\theta + \cos^4\theta)\, d\theta

0∼2π0 \sim 2\pi の範囲において、cos⁡θ\cos\theta、cos⁡3θ\cos^3\theta は期間数であるため、積分は 00 となる

=14a4∫02π(1+6cos⁡2θ+cos⁡4θ) dθ=a4∫0π2(1+6cos⁡2θ+cos⁡4θ) dθ= \frac{1}{4}a^4 \int_0^{2\pi} (1 + 6\cos^2\theta + \cos^4\theta)\, d\theta = a^4 \int_0^{\frac{\pi}{2}} (1 + 6\cos^2\theta + \cos^4\theta)\, d\theta

=a4{[θ]0π2+6⋅12⋅π2+34⋅12⋅π2}=a4(π2+32π+316π)=a4⋅3516π=3532πa4= a^4 \left\{ [\theta]_0^{\frac{\pi}{2}} + 6 \cdot \frac{1}{2} \cdot \frac{\pi}{2} + \frac{3}{4} \cdot \frac{1}{2} \cdot \frac{\pi}{2} \right\} = a^4 \left(\frac{\pi}{2} + \frac{3}{2}\pi + \frac{3}{16}\pi\right) = a^4 \cdot \frac{35}{16}\pi = \frac{35}{32}\pi a^4

解説: r31bn1z