
取上半球 $z = \sqrt{a^2-x^2-y^2}$:
$$z_x = \frac{-x}{\sqrt{a^2-x^2-y^2}},\quad z_y = \frac{-y}{\sqrt{a^2-x^2-y^2}}$$ $$\sqrt{1+z_x^2+z_y^2} = \frac{a}{\sqrt{a^2-x^2-y^2}} = \frac{a}{\sqrt{a^2-r^2}}$$投影 $D$:$x^2+y^2\leq ax$,极坐标 $r\leq a\cos\theta$,$\theta\in[-\frac{\pi}{2},\frac{\pi}{2}]$
$$A = 2\int_{-\pi/2}^{\pi/2}\dd\theta\int_0^{a\cos\theta}\frac{a}{\sqrt{a^2-r^2}}\cdot r\dd r = 2a^2\int_{-\pi/2}^{\pi/2}(1-\sin\theta)\dd\theta = 2a^2(\pi-2)$$

关键:$\sqrt{1+z_x^2+z_y^2} = \frac{R}{\sqrt{R^2-r^2}}$
柱面极坐标:$r = R\cos\theta$,$\theta\in[-\frac{\pi}{2},\frac{\pi}{2}]$
$$A_{上半} = \int_{-\pi/2}^{\pi/2}\dd\theta\int_0^{R\cos\theta}\frac{Rr}{\sqrt{R^2-r^2}}\dd r = R^2\int_{-\pi/2}^{\pi/2}(1-\sin\theta)\dd\theta = R^2(\pi-2)$$上下半球共 $A = 2R^2(\pi-2)$。
$z_x = \frac{x}{\sqrt{x^2+y^2}}$,$z_y = \frac{y}{\sqrt{x^2+y^2}}$
$$\sqrt{1+z_x^2+z_y^2} = \sqrt{1+\frac{x^2+y^2}{x^2+y^2}} = \sqrt{2}$$ $$A = \iint_{D}\sqrt{2}\,\dd x\dd y = \sqrt{2}\cdot\pi\cdot 1^2 = \sqrt{2}\pi$$
对 $x$ 轴:$I_x = \iint_D y^2\rho\dd\sigma$(或 $\iiint_\Omega(y^2+z^2)\rho\dd V$)
对 $y$ 轴:$I_y = \iint_D x^2\rho\dd\sigma$
对原点:$I_O = \iint_D(x^2+y^2)\rho\dd\sigma$
这实际上是曲面积分:$M = \iint_{球面} (x^2+y^2)\dd S$
用球坐标参数化:$x^2+y^2 = R^2\sin^2\varphi$,$\dd S = R^2\sin\varphi\dd\varphi\dd\theta$
$$M = \int_0^{2\pi}\dd\theta\int_0^{\pi/2}R^2\sin^2\varphi\cdot R^2\sin\varphi\dd\varphi = 2\pi R^4\int_0^{\pi/2}\sin^3\varphi\dd\varphi = 2\pi R^4\cdot\frac{2}{3} = \frac{4\pi R^4}{3}$$
极坐标:$= \frac{1}{\pi r^2}\int_0^{2\pi}\dd\theta\int_0^r f(\rho)\cdot\rho\dd\rho = \frac{2}{r^2}\int_0^r\rho f(\rho)\dd\rho$
用L'Hôpital:$= \lim_{r\to 0}\frac{2rf(r)}{2r} = f(0) = 0$。
如果问的是 $\frac{1}{\pi r^2}$ 对应的极限,则需要更仔细地分析,利用 $f(\rho)\sim\rho$ 当 $\rho\to 0$:
$\frac{2}{r^2}\int_0^r\rho^2\dd\rho = \frac{2r}{3} \to 0$。但如果分母是 $r^3$... 具体取决于题目。
$\sqrt{1+z_x^2+z_y^2}=\sqrt{1+4r^2}$。$D$:$r\leq 2a\cos\theta$,$\theta\in[-\frac{\pi}{2},\frac{\pi}{2}]$。
$$S=\int_{-\pi/2}^{\pi/2}\dd\theta\int_0^{2a\cos\theta}\sqrt{1+4r^2}\cdot r\,\dd r=\frac{1}{12}\int_{-\pi/2}^{\pi/2}[(1+16a^2\cos^2\theta)^{3/2}-1]\dd\theta$$最终 $S=(3+\frac{\pi}{2})a^2$。
曲面面积三步走:① $\sqrt{1+z_x^2+z_y^2}$ → ② 确定投影区域 → ③ 极坐标积分。
$\sqrt{1+z_x^2+z_y^2}=\sqrt{2}$(常数!)。$S=\sqrt{2}\cdot\pi a^2$
锥面面积 = $\sqrt{2}\times$ 投影面积,因为 $\sqrt{1+z_x^2+z_y^2}$ 恰好是常数。
$M=\int_0^1 x(1-x^2)\dd x=\frac{1}{4}$
$\bar{x}=\frac{\int_0^1 x^2(1-x^2)\dd x}{1/4}=\frac{2/15}{1/4}=\frac{8}{15}$
$\bar{y}=\frac{\int_0^1 x\frac{1-x^4}{2}\dd x}{1/4}=\frac{1/6}{1/4}=\frac{2}{3}$
质心 $\left(\frac{8}{15},\frac{2}{3}\right)$。
$M_y$(对 $y$ 轴的矩 $=\iint x\rho$)对应 $\bar{x}$,别搞反!
$z_x=x$,$z_y=0$。$\sqrt{1+x^2+0}=\sqrt{1+x^2}$。
$D: |x|+|y|\leq 1$(正方形区域,对称性 $\times 4$)。
$$S=4\int_0^1\dd x\int_0^{1-x}\sqrt{1+x^2}\dd y=4\int_0^1(1-x)\sqrt{1+x^2}\dd x$$分成两个积分:$4\int_0^1\sqrt{1+x^2}\dd x-4\int_0^1 x\sqrt{1+x^2}\dd x$
第一个用 $x=\tan t$;第二个凑微分 $=\frac{4}{3}[(1+x^2)^{3/2}]_0^1$。