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) f ( x ) の定積分 (definite integral) における次の式を示せ。
∫ 0 π 2 f ( cos θ ) d θ = ∫ 0 π 2 f ( sin θ ) d θ \int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_0^{\frac{\pi}{2}} f(\sin\theta) d\theta ∫ 0 2 π f ( cos θ ) d θ = ∫ 0 2 π f ( sin θ ) d θ
小問B2
次の定積分について、
∫ 0 2 1 x 2 + 1 d x \int_0^2 \frac{1}{\sqrt{x^2 + 1}} dx ∫ 0 2 x 2 + 1 1 d x
x = 1 2 ( y − 1 y ) , ( y > 0 ) x = \frac{1}{2}(y - \frac{1}{y}), (y > 0) x = 2 1 ( y − y 1 ) , ( 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 ) ∣ − 1 ≤ x + y ≤ 1 , − 1 ≤ x − y ≤ 1 } D = \{(x,y)| -1 \leq x + y \leq 1, -1 \leq x - y \leq 1\} D = {( x , y ) ∣ − 1 ≤ x + y ≤ 1 , − 1 ≤ x − y ≤ 1 }
次の二重積分(double integral)を求めよ。
∬ D 1 − ( x + y ) 2 d x d y \iint_{D} \sqrt{1-(x+y)^2} dxdy ∬ D 1 − ( x + y ) 2 d x d y
题目描述
小问B1
设 f ( x ) f(x) f ( x ) 是实数域上的连续函数。证明定积分恒等式
∫ 0 π 2 f ( cos θ ) d θ = ∫ 0 π 2 f ( sin θ ) d θ . \int_0^{\frac{\pi}{2}}f(\cos\theta)\,d\theta
=\int_0^{\frac{\pi}{2}}f(\sin\theta)\,d\theta. ∫ 0 2 π f ( cos θ ) d θ = ∫ 0 2 π f ( sin θ ) d θ .
小问B2
对定积分
∫ 0 2 1 x 2 + 1 d x , \int_0^2\frac{1}{\sqrt{x^2+1}}\,dx, ∫ 0 2 x 2 + 1 1 d x ,
使用指定代换
x = 1 2 ( y − 1 y ) , y > 0 , x=\frac12\left(y-\frac1y\right),\qquad y>0, x = 2 1 ( y − y 1 ) , y > 0 ,
完成计算。
小问B3
定义区域
D = { ( x , y ) ∣ − 1 ≤ x + y ≤ 1 , − 1 ≤ x − y ≤ 1 } . D=\{(x,y)\mid-1\leq x+y\leq1,\ -1\leq x-y\leq1\}. D = {( x , y ) ∣ − 1 ≤ x + y ≤ 1 , − 1 ≤ x − y ≤ 1 } .
求二重积分
∬ D 1 − ( x + y ) 2 d x d y . \iint_D\sqrt{1-(x+y)^2}\,dx\,dy. ∬ D 1 − ( x + y ) 2 d x d y .
Kai
小問B1
Let's prove the identity:
∫ 0 π 2 f ( cos θ ) d θ = ∫ 0 π 2 f ( sin θ ) d θ \int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_0^{\frac{\pi}{2}} f(\sin\theta) d\theta ∫ 0 2 π f ( cos θ ) d θ = ∫ 0 2 π f ( sin θ ) d θ
We can use the substitution u = π 2 − θ u = \frac{\pi}{2} - \theta u = 2 π − θ , then d u = − d θ du = -d\theta d u = − d θ . When θ = 0 \theta = 0 θ = 0 , u = π 2 u = \frac{\pi}{2} u = 2 π , and when θ = π 2 \theta = \frac{\pi}{2} θ = 2 π , u = 0 u = 0 u = 0 .
Thus,
∫ 0 π 2 f ( cos θ ) d θ = ∫ π 2 0 f ( cos ( π 2 − u ) ) ( − d u ) = ∫ 0 π 2 f ( cos ( π 2 − u ) ) d u \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 ∫ 0 2 π f ( cos θ ) d θ = ∫ 2 π 0 f ( cos ( 2 π − u )) ( − d u ) = ∫ 0 2 π f ( cos ( 2 π − u )) d u
Since cos ( π 2 − u ) = sin u \cos(\frac{\pi}{2} - u) = \sin u cos ( 2 π − u ) = sin u , we have
∫ 0 π 2 f ( cos ( π 2 − u ) ) d u = ∫ 0 π 2 f ( sin u ) d u \int_0^{\frac{\pi}{2}} f(\cos(\frac{\pi}{2}-u)) du = \int_0^{\frac{\pi}{2}} f(\sin u) du ∫ 0 2 π f ( cos ( 2 π − u )) d u = ∫ 0 2 π f ( sin u ) d u
Replacing u u u with θ \theta θ , we get
∫ 0 π 2 f ( sin u ) d u = ∫ 0 π 2 f ( sin θ ) d θ \int_0^{\frac{\pi}{2}} f(\sin u) du = \int_0^{\frac{\pi}{2}} f(\sin \theta) d\theta ∫ 0 2 π f ( sin u ) d u = ∫ 0 2 π f ( sin θ ) d θ
Therefore,
∫ 0 π 2 f ( cos θ ) d θ = ∫ 0 π 2 f ( sin θ ) d θ \int_0^{\frac{\pi}{2}} f(\cos\theta) d\theta = \int_0^{\frac{\pi}{2}} f(\sin\theta) d\theta ∫ 0 2 π f ( cos θ ) d θ = ∫ 0 2 π f ( sin θ ) d θ
Thus, the identity is proved.
小問B2
Let x = 1 2 ( y − 1 y ) x = \frac{1}{2}(y - \frac{1}{y}) x = 2 1 ( y − y 1 ) . Then d x = 1 2 ( 1 + 1 y 2 ) d y = 1 2 ( y 2 + 1 y 2 ) d y dx = \frac{1}{2}(1 + \frac{1}{y^2}) dy = \frac{1}{2}(\frac{y^2 + 1}{y^2}) dy d x = 2 1 ( 1 + y 2 1 ) d y = 2 1 ( y 2 y 2 + 1 ) d y .
Also, x 2 = 1 4 ( y 2 − 2 + 1 y 2 ) x^2 = \frac{1}{4}(y^2 - 2 + \frac{1}{y^2}) x 2 = 4 1 ( y 2 − 2 + y 2 1 ) .
Then, x 2 + 1 = 1 4 ( y 2 − 2 + 1 y 2 ) + 1 = 1 4 ( y 2 + 2 + 1 y 2 ) = 1 4 ( y + 1 y ) 2 x^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 x 2 + 1 = 4 1 ( y 2 − 2 + y 2 1 ) + 1 = 4 1 ( y 2 + 2 + y 2 1 ) = 4 1 ( y + y 1 ) 2 .
So, x 2 + 1 = 1 2 ( y + 1 y ) \sqrt{x^2 + 1} = \frac{1}{2}(y + \frac{1}{y}) x 2 + 1 = 2 1 ( y + y 1 ) .
Then, 1 x 2 + 1 = 2 y + 1 y = 2 y y 2 + 1 \frac{1}{\sqrt{x^2 + 1}} = \frac{2}{y + \frac{1}{y}} = \frac{2y}{y^2 + 1} x 2 + 1 1 = y + y 1 2 = y 2 + 1 2 y .
So, 1 x 2 + 1 d x = 2 y y 2 + 1 ⋅ 1 2 y 2 + 1 y 2 d y = 1 y d y \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 x 2 + 1 1 d x = y 2 + 1 2 y ⋅ 2 1 y 2 y 2 + 1 d y = y 1 d y .
Now, when x = 0 x=0 x = 0 , 1 2 ( y − 1 y ) = 0 \frac{1}{2}(y - \frac{1}{y}) = 0 2 1 ( y − y 1 ) = 0 , which implies y − 1 y = 0 y - \frac{1}{y} = 0 y − y 1 = 0 , so y 2 = 1 y^2 = 1 y 2 = 1 . Since y > 0 y > 0 y > 0 , y = 1 y=1 y = 1 .
When x = 2 x=2 x = 2 , 1 2 ( y − 1 y ) = 2 \frac{1}{2}(y - \frac{1}{y}) = 2 2 1 ( y − y 1 ) = 2 , which implies y − 1 y = 4 y - \frac{1}{y} = 4 y − y 1 = 4 , so y 2 − 4 y − 1 = 0 y^2 - 4y - 1 = 0 y 2 − 4 y − 1 = 0 . Then y = 4 ± 16 + 4 2 = 4 ± 20 2 = 4 ± 2 5 2 = 2 ± 5 y = \frac{4 \pm \sqrt{16 + 4}}{2} = \frac{4 \pm \sqrt{20}}{2} = \frac{4 \pm 2\sqrt{5}}{2} = 2 \pm \sqrt{5} y = 2 4 ± 16 + 4 = 2 4 ± 20 = 2 4 ± 2 5 = 2 ± 5 . Since y > 0 y > 0 y > 0 , y = 2 + 5 y = 2 + \sqrt{5} y = 2 + 5 .
Therefore, the integral becomes:
∫ 1 2 + 5 1 y d y = [ ln y ] 1 2 + 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}) ∫ 1 2 + 5 y 1 d y = [ ln y ] 1 2 + 5 = ln ( 2 + 5 ) − ln ( 1 ) = ln ( 2 + 5 )
So, the answer is ln ( 2 + 5 ) \ln(2+\sqrt{5}) ln ( 2 + 5 ) .
小問B3
Let u = x + y u = x + y u = x + y and v = x − y v = x - y v = x − y . Then x = u + v 2 x = \frac{u+v}{2} x = 2 u + v and y = u − v 2 y = \frac{u-v}{2} y = 2 u − v .
The Jacobian is given by
∂ ( x , y ) ∂ ( u , v ) = ∣ ∂ x ∂ u ∂ x ∂ v ∂ y ∂ u ∂ y ∂ v ∣ = ∣ 1 2 1 2 1 2 − 1 2 ∣ = − 1 4 − 1 4 = − 1 2 \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} ∂ ( u , v ) ∂ ( x , y ) = ∂ u ∂ x ∂ u ∂ y ∂ v ∂ x ∂ v ∂ y = 2 1 2 1 2 1 − 2 1 = − 4 1 − 4 1 = − 2 1
Therefore, ∣ ∂ ( x , y ) ∂ ( u , v ) ∣ = 1 2 \left| \frac{\partial(x, y)}{\partial(u, v)} \right| = \frac{1}{2} ∂ ( u , v ) ∂ ( x , y ) = 2 1 .
The region D is transformed into the region R such that − 1 ≤ u ≤ 1 -1 \leq u \leq 1 − 1 ≤ u ≤ 1 and − 1 ≤ v ≤ 1 -1 \leq v \leq 1 − 1 ≤ v ≤ 1 .
Then, the double integral becomes
∬ D 1 − ( x + y ) 2 d x d y = ∬ R 1 − u 2 ∣ ∂ ( x , y ) ∂ ( u , v ) ∣ d u d v = ∫ − 1 1 ∫ − 1 1 1 − u 2 ⋅ 1 2 d u d v \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 ∬ D 1 − ( x + y ) 2 d x d y = ∬ R 1 − u 2 ∂ ( u , v ) ∂ ( x , y ) d u d v = ∫ − 1 1 ∫ − 1 1 1 − u 2 ⋅ 2 1 d u d v
= 1 2 ∫ − 1 1 1 − u 2 d u ∫ − 1 1 d v = 1 2 ⋅ ( 2 ) ∫ − 1 1 1 − u 2 d u = ∫ − 1 1 1 − u 2 d u = \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 = 2 1 ∫ − 1 1 1 − u 2 d u ∫ − 1 1 d v = 2 1 ⋅ ( 2 ) ∫ − 1 1 1 − u 2 d u = ∫ − 1 1 1 − u 2 d u
Let u = sin θ u = \sin\theta u = sin θ . Then d u = cos θ d θ du = \cos\theta d\theta d u = cos θ d θ .
When u = − 1 u = -1 u = − 1 , θ = − π 2 \theta = -\frac{\pi}{2} θ = − 2 π . When u = 1 u = 1 u = 1 , θ = π 2 \theta = \frac{\pi}{2} θ = 2 π .
∫ − 1 1 1 − u 2 d u = ∫ − π 2 π 2 1 − sin 2 θ cos θ d θ = ∫ − π 2 π 2 cos 2 θ d θ = ∫ − π 2 π 2 1 + cos ( 2 θ ) 2 d θ \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 ∫ − 1 1 1 − u 2 d u = ∫ − 2 π 2 π 1 − sin 2 θ cos θ d θ = ∫ − 2 π 2 π cos 2 θ d θ = ∫ − 2 π 2 π 2 1 + cos ( 2 θ ) d θ
= 1 2 [ θ + sin ( 2 θ ) 2 ] − π 2 π 2 = 1 2 [ ( π 2 + 0 ) − ( − π 2 + 0 ) ] = 1 2 ( π ) = π 2 = \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} = 2 1 [ θ + 2 sin ( 2 θ ) ] − 2 π 2 π = 2 1 [ ( 2 π + 0 ) − ( − 2 π + 0 ) ] = 2 1 ( π ) = 2 π
Therefore, the double integral is π 2 \frac{\pi}{2} 2 π .