第8章 8.4

(1)

∫0π∫0acos⁡θrsin⁡θ drdθ=∫0π[12r2sin⁡θ]0acos⁡θdθ=∫0π12a2cos⁡2θ⋅sin⁡θdθ\int_0^{\pi} \int_0^{a\cos\theta} r\sin\theta \, dr d\theta = \int_0^{\pi} \left[\frac{1}{2} r^2 \sin\theta\right]_0^{a\cos\theta} d\theta = \int_0^{\pi} \frac{1}{2} a^2 \cos^2\theta \cdot \sin\theta d\theta

cos⁡θ=t\cos\theta = t とおくと −sin⁡θdθ=dt-\sin\theta d\theta = dt θ:0→π\theta : 0 \to \pi t:1→−1t : 1 \to -1 これから

=∫−1112a2t2dt=[16a2t3]−11=13a2= \int_{-1}^{1} \frac{1}{2} a^2 t^2 dt = \left[\frac{1}{6} a^2 t^3\right]_{-1}^{1} = \frac{1}{3} a^2

(2)

∫0π2∫acos⁡θar drdθ=∫0π2[12r2]acos⁡θadθ=∫0π212a2(1−cos⁡2θ)dθ=∫0π212a2sin⁡2θdθ\int_0^{\frac{\pi}{2}} \int_{a\cos\theta}^{a} r \, dr d\theta = \int_0^{\frac{\pi}{2}} \left[\frac{1}{2} r^2\right]_{a\cos\theta}^{a} d\theta = \int_0^{\frac{\pi}{2}} \frac{1}{2} a^2 (1-\cos^2\theta) d\theta = \int_0^{\frac{\pi}{2}} \frac{1}{2} a^2 \sin^2\theta d\theta

=12a2∫0π21−cos⁡2θ2dθ=12a2[12θ−14sin⁡2θ]0π2=π8a2= \frac{1}{2} a^2 \int_0^{\frac{\pi}{2}} \frac{1-\cos 2\theta}{2} d\theta = \frac{1}{2} a^2 \left[\frac{1}{2}\theta - \frac{1}{4}\sin 2\theta\right]_0^{\frac{\pi}{2}} = \frac{\pi}{8} a^2

(3)

∬Dr2sin⁡θ drdθD:0≤r≤2acos⁡θ0≤θ≤π2\iint_D r^2 \sin\theta \, dr d\theta \qquad D : 0 \le r \le 2a\cos\theta \quad 0 \le \theta \le \frac{\pi}{2}

∫0π2∫02acos⁡θr2sin⁡θ drdθ=∫0π2[13r3sin⁡θ]02acos⁡θdθ=∫0π283a3cos⁡3θ⋅sin⁡θdθ\int_0^{\frac{\pi}{2}} \int_0^{2a\cos\theta} r^2 \sin\theta \, dr d\theta = \int_0^{\frac{\pi}{2}} \left[\frac{1}{3} r^3 \sin\theta\right]_0^{2a\cos\theta} d\theta = \int_0^{\frac{\pi}{2}} \frac{8}{3} a^3 \cos^3\theta \cdot \sin\theta d\theta

cos⁡θ=t\cos\theta = t とおくと −sin⁡θdθ=dt-\sin\theta d\theta = dt θ:0→π2\theta : 0 \to \dfrac{\pi}{2} t:1→0t : 1 \to 0 これから

=∫0183a3t3dt=[23a3t4]01=23a3= \int_0^{1} \frac{8}{3} a^3 t^3 dt = \left[\frac{2}{3} a^3 t^4\right]_0^{1} = \frac{2}{3} a^3

解説: r31bn1z