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早稲田大学 創造理工学研究科 経営システム工学専攻 2021年7月実施 数理基礎 問題B

Author

思齐塾, 祭音Myyura

Description

日本語

小問B1

実数空間 (real space)で連続(continuous)である関数 (function) f(x)f(x) の定積分 (definite integral) における次の式を示せ。

0π2f(cosθ)dθ=0π2f(sinθ)dθ\int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_0^{\frac{\pi}{2}} f(\sin\theta) d\theta

小問B2

次の定積分について、

021x2+1dx\int_0^2 \frac{1}{\sqrt{x^2 + 1}} dx

x=12(y1y),(y>0)x = \frac{1}{2}(y - \frac{1}{y}), (y > 0) と置換(substitute) して計算せよ。

小問B3

領域(domain)Dを以下のように設定する。

D={(x,y)1x+y1,1xy1}D = \{(x,y)| -1 \leq x + y \leq 1, -1 \leq x - y \leq 1\}

次の二重積分(double integral)を求めよ。

D1(x+y)2dxdy\iint_{D} \sqrt{1-(x+y)^2} dxdy

题目描述

小问B1

f(x)f(x) 是实数域上的连续函数。证明定积分恒等式

0π2f(cosθ)dθ=0π2f(sinθ)dθ.\int_0^{\frac{\pi}{2}}f(\cos\theta)\,d\theta =\int_0^{\frac{\pi}{2}}f(\sin\theta)\,d\theta.

小问B2

对定积分

021x2+1dx,\int_0^2\frac{1}{\sqrt{x^2+1}}\,dx,

使用指定代换

x=12(y1y),y>0,x=\frac12\left(y-\frac1y\right),\qquad y>0,

完成计算。

小问B3

定义区域

D={(x,y)1x+y1, 1xy1}.D=\{(x,y)\mid-1\leq x+y\leq1,\ -1\leq x-y\leq1\}.

求二重积分

D1(x+y)2dxdy.\iint_D\sqrt{1-(x+y)^2}\,dx\,dy.

Kai

小問B1

Let's prove the identity:

0π2f(cosθ)dθ=0π2f(sinθ)dθ\int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_0^{\frac{\pi}{2}} f(\sin\theta) d\theta

We can use the substitution u=π2θu = \frac{\pi}{2} - \theta , then du=dθdu = -d\theta . When θ=0\theta = 0 , u=π2u = \frac{\pi}{2} , and when θ=π2\theta = \frac{\pi}{2} , u=0u = 0 . Thus,

0π2f(cosθ)dθ=π20f(cos(π2u))(du)=0π2f(cos(π2u))du\int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_{\frac{\pi}{2}}^0 f(\cos(\frac{\pi}{2}-u)) (-du) = \int_0^{\frac{\pi}{2}} f(\cos(\frac{\pi}{2}-u)) du

Since cos(π2u)=sinu\cos(\frac{\pi}{2} - u) = \sin u , we have

0π2f(cos(π2u))du=0π2f(sinu)du\int_0^{\frac{\pi}{2}} f(\cos(\frac{\pi}{2}-u)) du = \int_0^{\frac{\pi}{2}} f(\sin u) du

Replacing uu with θ\theta , we get

0π2f(sinu)du=0π2f(sinθ)dθ\int_0^{\frac{\pi}{2}} f(\sin u) du = \int_0^{\frac{\pi}{2}} f(\sin \theta) d\theta

Therefore,

0π2f(cosθ)dθ=0π2f(sinθ)dθ\int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_0^{\frac{\pi}{2}} f(\sin\theta) d\theta

Thus, the identity is proved.

小問B2

Let x=12(y1y)x = \frac{1}{2}(y - \frac{1}{y}) . Then dx=12(1+1y2)dy=12(y2+1y2)dydx = \frac{1}{2}(1 + \frac{1}{y^2}) dy = \frac{1}{2}(\frac{y^2 + 1}{y^2}) dy . Also, x2=14(y22+1y2)x^2 = \frac{1}{4}(y^2 - 2 + \frac{1}{y^2}) . Then, x2+1=14(y22+1y2)+1=14(y2+2+1y2)=14(y+1y)2x^2 + 1 = \frac{1}{4}(y^2 - 2 + \frac{1}{y^2}) + 1 = \frac{1}{4}(y^2 + 2 + \frac{1}{y^2}) = \frac{1}{4}(y + \frac{1}{y})^2 . So, x2+1=12(y+1y)\sqrt{x^2 + 1} = \frac{1}{2}(y + \frac{1}{y}) . Then, 1x2+1=2y+1y=2yy2+1\frac{1}{\sqrt{x^2 + 1}} = \frac{2}{y + \frac{1}{y}} = \frac{2y}{y^2 + 1} . So, 1x2+1dx=2yy2+112y2+1y2dy=1ydy\frac{1}{\sqrt{x^2 + 1}} dx = \frac{2y}{y^2 + 1} \cdot \frac{1}{2} \frac{y^2 + 1}{y^2} dy = \frac{1}{y} dy .

Now, when x=0x=0 , 12(y1y)=0\frac{1}{2}(y - \frac{1}{y}) = 0 , which implies y1y=0y - \frac{1}{y} = 0 , so y2=1y^2 = 1 . Since y>0y > 0 , y=1y=1 . When x=2x=2 , 12(y1y)=2\frac{1}{2}(y - \frac{1}{y}) = 2 , which implies y1y=4y - \frac{1}{y} = 4 , so y24y1=0y^2 - 4y - 1 = 0 . Then y=4±16+42=4±202=4±252=2±5y = \frac{4 \pm \sqrt{16 + 4}}{2} = \frac{4 \pm \sqrt{20}}{2} = \frac{4 \pm 2\sqrt{5}}{2} = 2 \pm \sqrt{5} . Since y>0y > 0 , y=2+5y = 2 + \sqrt{5} . Therefore, the integral becomes:

12+51ydy=[lny]12+5=ln(2+5)ln(1)=ln(2+5)\int_1^{2+\sqrt{5}} \frac{1}{y} dy = \left[ \ln y \right]_1^{2+\sqrt{5}} = \ln(2+\sqrt{5}) - \ln(1) = \ln(2+\sqrt{5})

So, the answer is ln(2+5)\ln(2+\sqrt{5}) .

小問B3

Let u=x+yu = x + y and v=xyv = x - y . Then x=u+v2x = \frac{u+v}{2} and y=uv2y = \frac{u-v}{2} . The Jacobian is given by

(x,y)(u,v)=xuxvyuyv=12121212=1414=12\frac{\partial(x, y)}{\partial(u, v)} = \begin{vmatrix} \frac{\partial x}{\partial u} & \frac{\partial x}{\partial v} \\ \frac{\partial y}{\partial u} & \frac{\partial y}{\partial v} \end{vmatrix} = \begin{vmatrix} \frac{1}{2} & \frac{1}{2} \\ \frac{1}{2} & -\frac{1}{2} \end{vmatrix} = -\frac{1}{4} - \frac{1}{4} = -\frac{1}{2}

Therefore, (x,y)(u,v)=12\left| \frac{\partial(x, y)}{\partial(u, v)} \right| = \frac{1}{2} . The region D is transformed into the region R such that 1u1-1 \leq u \leq 1 and 1v1-1 \leq v \leq 1 . Then, the double integral becomes

D1(x+y)2dxdy=R1u2(x,y)(u,v)dudv=11111u212dudv\iint_{D} \sqrt{1-(x+y)^2} dxdy = \iint_{R} \sqrt{1-u^2} \left| \frac{\partial(x, y)}{\partial(u, v)} \right| dudv = \int_{-1}^{1} \int_{-1}^{1} \sqrt{1-u^2} \cdot \frac{1}{2} dudv
=12111u2du11dv=12(2)111u2du=111u2du= \frac{1}{2} \int_{-1}^{1} \sqrt{1-u^2} du \int_{-1}^{1} dv = \frac{1}{2} \cdot (2) \int_{-1}^{1} \sqrt{1-u^2} du = \int_{-1}^{1} \sqrt{1-u^2} du

Let u=sinθu = \sin\theta . Then du=cosθdθdu = \cos\theta d\theta . When u=1u = -1 , θ=π2\theta = -\frac{\pi}{2} . When u=1u = 1 , θ=π2\theta = \frac{\pi}{2} .

111u2du=π2π21sin2θcosθdθ=π2π2cos2θdθ=π2π21+cos(2θ)2dθ\int_{-1}^{1} \sqrt{1-u^2} du = \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \sqrt{1-\sin^2\theta} \cos\theta d\theta = \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \cos^2\theta d\theta = \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \frac{1+\cos(2\theta)}{2} d\theta
=12[θ+sin(2θ)2]π2π2=12[(π2+0)(π2+0)]=12(π)=π2= \frac{1}{2} \left[ \theta + \frac{\sin(2\theta)}{2} \right]_{-\frac{\pi}{2}}^{\frac{\pi}{2}} = \frac{1}{2} \left[ (\frac{\pi}{2} + 0) - (-\frac{\pi}{2} + 0) \right] = \frac{1}{2} (\pi) = \frac{\pi}{2}

Therefore, the double integral is π2\frac{\pi}{2} .