早稲田大学 創造理工学研究科 経営システム工学専攻 2024年7月実施 数理基礎 問題1
Author
思齐塾 , 祭音Myyura
Description
日本語
小問1
y = f ( x ) , x = s 2 + t 2 + u 2 y = f(x), x = \sqrt{s^2 + t^2 + u^2} y = f ( x ) , x = s 2 + t 2 + u 2 とするとき、二階偏微分の和 ∂ 2 y ∂ s 2 + ∂ 2 y ∂ t 2 + ∂ 2 y ∂ u 2 \frac{\partial^2 y}{\partial s^2} + \frac{\partial^2 y}{\partial t^2} + \frac{\partial^2 y}{\partial u^2} ∂ s 2 ∂ 2 y + ∂ t 2 ∂ 2 y + ∂ u 2 ∂ 2 y を x , f ′ ( x ) , f ′ ′ ( x ) x, f'(x), f''(x) x , f ′ ( x ) , f ′′ ( x ) を用いて表せ。
小問2
関数 z = f ( x , y ) = x 4 + y 4 − 9 ( x + y ) 2 z = f(x, y) = x^4 + y^4 - 9(x+y)^2 z = f ( x , y ) = x 4 + y 4 − 9 ( x + y ) 2 に対し、関数の停留点と極値を全て求めよ。
小問3
領域Dを
D = { ( x , y ) ∣ x 2 + y 2 ≤ 2 } D = \{(x, y)| x^2 + y^2 \leq 2\} D = {( x , y ) ∣ x 2 + y 2 ≤ 2 }
のように定義するとき、次の二重積分を求めよ。
∬ D 2 − x 2 − y 2 2 + x 2 + y 2 d x d y \iint_{D} \sqrt{\frac{2-x^2-y^2}{2+x^2+y^2}}dxdy ∬ D 2 + x 2 + y 2 2 − x 2 − y 2 d x d y
题目描述
小问1
设
y = f ( x ) , x = s 2 + t 2 + u 2 . y=f(x),\qquad x=\sqrt{s^2+t^2+u^2}. y = f ( x ) , x = s 2 + t 2 + u 2 .
用 x , f ′ ( x ) , f ′ ′ ( x ) x,f'(x),f''(x) x , f ′ ( x ) , f ′′ ( x ) 表示
∂ 2 y ∂ s 2 + ∂ 2 y ∂ t 2 + ∂ 2 y ∂ u 2 . \frac{\partial^2y}{\partial s^2}
+\frac{\partial^2y}{\partial t^2}
+\frac{\partial^2y}{\partial u^2}. ∂ s 2 ∂ 2 y + ∂ t 2 ∂ 2 y + ∂ u 2 ∂ 2 y .
原题没有说明原点处的光滑性;因此一般公式应在 x > 0 x>0 x > 0 上给出。若还讨论 x = 0 x=0 x = 0 ,须另行说明使径向函数在原点二次可微所需的条件及原点处的取值。
小问2
对函数
z = f ( x , y ) = x 4 + y 4 − 9 ( x + y ) 2 , z=f(x,y)=x^4+y^4-9(x+y)^2, z = f ( x , y ) = x 4 + y 4 − 9 ( x + y ) 2 ,
求出全部驻点,并确定所有极值。
小问3
定义区域
D = { ( x , y ) ∣ x 2 + y 2 ≤ 2 } . D=\{(x,y)\mid x^2+y^2\leq2\}. D = {( x , y ) ∣ x 2 + y 2 ≤ 2 } .
求二重积分
∬ D 2 − x 2 − y 2 2 + x 2 + y 2 d x d y . \iint_D
\sqrt{\frac{2-x^2-y^2}{2+x^2+y^2}}\,dx\,dy. ∬ D 2 + x 2 + y 2 2 − x 2 − y 2 d x d y .
Kai
小問1
Let x = s 2 + t 2 + u 2 x = \sqrt{s^2 + t^2 + u^2} x = s 2 + t 2 + u 2 . Then x 2 = s 2 + t 2 + u 2 x^2 = s^2 + t^2 + u^2 x 2 = s 2 + t 2 + u 2 . We have
∂ x ∂ s = s s 2 + t 2 + u 2 = s x \frac{\partial x}{\partial s} = \frac{s}{\sqrt{s^2 + t^2 + u^2}} = \frac{s}{x} ∂ s ∂ x = s 2 + t 2 + u 2 s = x s
∂ x ∂ t = t s 2 + t 2 + u 2 = t x \frac{\partial x}{\partial t} = \frac{t}{\sqrt{s^2 + t^2 + u^2}} = \frac{t}{x} ∂ t ∂ x = s 2 + t 2 + u 2 t = x t
∂ x ∂ u = u s 2 + t 2 + u 2 = u x \frac{\partial x}{\partial u} = \frac{u}{\sqrt{s^2 + t^2 + u^2}} = \frac{u}{x} ∂ u ∂ x = s 2 + t 2 + u 2 u = x u
Now, we compute the second derivatives:
∂ 2 y ∂ s 2 = ∂ ∂ s ( ∂ y ∂ s ) = ∂ ∂ s ( f ′ ( x ) ∂ x ∂ s ) = ∂ ∂ s ( f ′ ( x ) s x ) \frac{\partial^2 y}{\partial s^2} = \frac{\partial}{\partial s} \left( \frac{\partial y}{\partial s} \right) = \frac{\partial}{\partial s} \left( f'(x) \frac{\partial x}{\partial s} \right) = \frac{\partial}{\partial s} \left( f'(x) \frac{s}{x} \right) ∂ s 2 ∂ 2 y = ∂ s ∂ ( ∂ s ∂ y ) = ∂ s ∂ ( f ′ ( x ) ∂ s ∂ x ) = ∂ s ∂ ( f ′ ( x ) x s )
∂ 2 y ∂ s 2 = f ′ ′ ( x ) ∂ x ∂ s s x + f ′ ( x ) x − s ∂ x ∂ s x 2 = f ′ ′ ( x ) s 2 x 2 + f ′ ( x ) x − s 2 x x 2 = f ′ ′ ( x ) s 2 x 2 + f ′ ( x ) x 2 − s 2 x 3 \frac{\partial^2 y}{\partial s^2} = f''(x) \frac{\partial x}{\partial s} \frac{s}{x} + f'(x) \frac{x - s \frac{\partial x}{\partial s}}{x^2} = f''(x) \frac{s^2}{x^2} + f'(x) \frac{x - \frac{s^2}{x}}{x^2} = f''(x) \frac{s^2}{x^2} + f'(x) \frac{x^2 - s^2}{x^3} ∂ s 2 ∂ 2 y = f ′′ ( x ) ∂ s ∂ x x s + f ′ ( x ) x 2 x − s ∂ s ∂ x = f ′′ ( x ) x 2 s 2 + f ′ ( x ) x 2 x − x s 2 = f ′′ ( x ) x 2 s 2 + f ′ ( x ) x 3 x 2 − s 2
Similarly,
∂ 2 y ∂ t 2 = f ′ ′ ( x ) t 2 x 2 + f ′ ( x ) x 2 − t 2 x 3 \frac{\partial^2 y}{\partial t^2} = f''(x) \frac{t^2}{x^2} + f'(x) \frac{x^2 - t^2}{x^3} ∂ t 2 ∂ 2 y = f ′′ ( x ) x 2 t 2 + f ′ ( x ) x 3 x 2 − t 2
∂ 2 y ∂ u 2 = f ′ ′ ( x ) u 2 x 2 + f ′ ( x ) x 2 − u 2 x 3 \frac{\partial^2 y}{\partial u^2} = f''(x) \frac{u^2}{x^2} + f'(x) \frac{x^2 - u^2}{x^3} ∂ u 2 ∂ 2 y = f ′′ ( x ) x 2 u 2 + f ′ ( x ) x 3 x 2 − u 2
Thus,
∂ 2 y ∂ s 2 + ∂ 2 y ∂ t 2 + ∂ 2 y ∂ u 2 = f ′ ′ ( x ) s 2 + t 2 + u 2 x 2 + f ′ ( x ) 3 x 2 − ( s 2 + t 2 + u 2 ) x 3 = f ′ ′ ( x ) x 2 x 2 + f ′ ( x ) 3 x 2 − x 2 x 3 = f ′ ′ ( x ) + f ′ ( x ) 2 x 2 x 3 = f ′ ′ ( x ) + 2 x f ′ ( x ) \frac{\partial^2 y}{\partial s^2} + \frac{\partial^2 y}{\partial t^2} + \frac{\partial^2 y}{\partial u^2} = f''(x) \frac{s^2 + t^2 + u^2}{x^2} + f'(x) \frac{3x^2 - (s^2 + t^2 + u^2)}{x^3} = f''(x) \frac{x^2}{x^2} + f'(x) \frac{3x^2 - x^2}{x^3} = f''(x) + f'(x) \frac{2x^2}{x^3} = f''(x) + \frac{2}{x} f'(x) ∂ s 2 ∂ 2 y + ∂ t 2 ∂ 2 y + ∂ u 2 ∂ 2 y = f ′′ ( x ) x 2 s 2 + t 2 + u 2 + f ′ ( x ) x 3 3 x 2 − ( s 2 + t 2 + u 2 ) = f ′′ ( x ) x 2 x 2 + f ′ ( x ) x 3 3 x 2 − x 2 = f ′′ ( x ) + f ′ ( x ) x 3 2 x 2 = f ′′ ( x ) + x 2 f ′ ( x )
Therefore,
For x > 0 x>0 x > 0 ,
∂ 2 y ∂ s 2 + ∂ 2 y ∂ t 2 + ∂ 2 y ∂ u 2 = f ′ ′ ( x ) + 2 x f ′ ( x ) . \boxed{
\frac{\partial^2 y}{\partial s^2}
+\frac{\partial^2 y}{\partial t^2}
+\frac{\partial^2 y}{\partial u^2}
=f''(x)+\frac{2}{x}f'(x)
}. ∂ s 2 ∂ 2 y + ∂ t 2 ∂ 2 y + ∂ u 2 ∂ 2 y = f ′′ ( x ) + x 2 f ′ ( x ) .
At x = 0 x=0 x = 0 , the divisions by x x x used above are not valid. If the radial function f ( s 2 + t 2 + u 2 ) f(\sqrt{s^2+t^2+u^2}) f ( s 2 + t 2 + u 2 ) is twice differentiable at the origin, then necessarily f ′ ( 0 ) = 0 f'(0)=0 f ′ ( 0 ) = 0 , and direct differentiation along the three coordinate axes gives
( ∂ 2 y ∂ s 2 + ∂ 2 y ∂ t 2 + ∂ 2 y ∂ u 2 ) ∣ ( 0 , 0 , 0 ) = 3 f ′ ′ ( 0 ) . \left.
\left(
\frac{\partial^2 y}{\partial s^2}
+\frac{\partial^2 y}{\partial t^2}
+\frac{\partial^2 y}{\partial u^2}
\right)\right|_{(0,0,0)}
=3f''(0). ( ∂ s 2 ∂ 2 y + ∂ t 2 ∂ 2 y + ∂ u 2 ∂ 2 y ) ( 0 , 0 , 0 ) = 3 f ′′ ( 0 ) .
Without these regularity conditions, the second partial derivatives at the origin need not exist.
小問2
首先,求偏导数:
∂ f ∂ x = 4 x 3 − 18 ( x + y ) \frac{\partial f}{\partial x} = 4x^3 - 18(x+y) ∂ x ∂ f = 4 x 3 − 18 ( x + y )
∂ f ∂ y = 4 y 3 − 18 ( x + y ) \frac{\partial f}{\partial y} = 4y^3 - 18(x+y) ∂ y ∂ f = 4 y 3 − 18 ( x + y )
令偏导数为0,得到方程组:
4 x 3 − 18 ( x + y ) = 0 4x^3 - 18(x+y) = 0 4 x 3 − 18 ( x + y ) = 0
4 y 3 − 18 ( x + y ) = 0 4y^3 - 18(x+y) = 0 4 y 3 − 18 ( x + y ) = 0
因此, 4 x 3 = 4 y 3 4x^3 = 4y^3 4 x 3 = 4 y 3 ,得到 x = y x = y x = y 。
将 x = y x = y x = y 代入第一个方程:
4 x 3 − 18 ( x + x ) = 0 4x^3 - 18(x+x) = 0 4 x 3 − 18 ( x + x ) = 0
4 x 3 − 36 x = 0 4x^3 - 36x = 0 4 x 3 − 36 x = 0
4 x ( x 2 − 9 ) = 0 4x(x^2 - 9) = 0 4 x ( x 2 − 9 ) = 0
4 x ( x − 3 ) ( x + 3 ) = 0 4x(x-3)(x+3) = 0 4 x ( x − 3 ) ( x + 3 ) = 0
所以,x = 0, x = 3, x = -3
对应的 y 值也相等,所以得到三个驻点:(0, 0), (3, 3), (-3, -3)
接下来,求二阶偏导数:
∂ 2 f ∂ x 2 = 12 x 2 − 18 \frac{\partial^2 f}{\partial x^2} = 12x^2 - 18 ∂ x 2 ∂ 2 f = 12 x 2 − 18
∂ 2 f ∂ y 2 = 12 y 2 − 18 \frac{\partial^2 f}{\partial y^2} = 12y^2 - 18 ∂ y 2 ∂ 2 f = 12 y 2 − 18
∂ 2 f ∂ x ∂ y = − 18 \frac{\partial^2 f}{\partial x \partial y} = -18 ∂ x ∂ y ∂ 2 f = − 18
令 A = ∂ 2 f ∂ x 2 , B = ∂ 2 f ∂ x ∂ y , C = ∂ 2 f ∂ y 2 A = \frac{\partial^2 f}{\partial x^2}, B = \frac{\partial^2 f}{\partial x \partial y}, C = \frac{\partial^2 f}{\partial y^2} A = ∂ x 2 ∂ 2 f , B = ∂ x ∂ y ∂ 2 f , C = ∂ y 2 ∂ 2 f ,计算 A C − B 2 AC - B^2 A C − B 2
对于 ( 0 , 0 ) (0, 0) ( 0 , 0 ) : A = − 18 A = -18 A = − 18 , B = − 18 B = -18 B = − 18 , C = − 18 C = -18 C = − 18 , A C − B 2 = ( − 18 ) ( − 18 ) − ( − 18 ) 2 = 0 AC - B^2 = (-18)(-18) - (-18)^2 = 0 A C − B 2 = ( − 18 ) ( − 18 ) − ( − 18 ) 2 = 0 , 无法确定极值。
对于 ( 3 , 3 ) (3, 3) ( 3 , 3 ) : A = 12 ( 3 2 ) − 18 = 108 − 18 = 90 A = 12(3^2) - 18 = 108 - 18 = 90 A = 12 ( 3 2 ) − 18 = 108 − 18 = 90 , B = − 18 B = -18 B = − 18 , C = 90 C = 90 C = 90 , A C − B 2 = ( 90 ) ( 90 ) − ( − 18 ) 2 = 8100 − 324 = 7776 > 0 AC - B^2 = (90)(90) - (-18)^2 = 8100 - 324 = 7776 > 0 A C − B 2 = ( 90 ) ( 90 ) − ( − 18 ) 2 = 8100 − 324 = 7776 > 0 , A > 0 A > 0 A > 0 , 所以 ( 3 , 3 ) (3, 3) ( 3 , 3 ) 是极小值点, 极小值为 f ( 3 , 3 ) = 3 4 + 3 4 − 9 ( 3 + 3 ) 2 = 81 + 81 − 9 ( 36 ) = 162 − 324 = − 162 f(3,3) = 3^4 + 3^4 - 9(3+3)^2 = 81 + 81 - 9(36) = 162 - 324 = -162 f ( 3 , 3 ) = 3 4 + 3 4 − 9 ( 3 + 3 ) 2 = 81 + 81 − 9 ( 36 ) = 162 − 324 = − 162 。
对于 ( − 3 , − 3 ) (-3, -3) ( − 3 , − 3 ) : A = 12 ( − 3 ) 2 − 18 = 108 − 18 = 90 A = 12(-3)^2 - 18 = 108 - 18 = 90 A = 12 ( − 3 ) 2 − 18 = 108 − 18 = 90 , B = − 18 B = -18 B = − 18 , C = 90 C = 90 C = 90 , A C − B 2 = ( 90 ) ( 90 ) − ( − 18 ) 2 = 8100 − 324 = 7776 > 0 AC - B^2 = (90)(90) - (-18)^2 = 8100 - 324 = 7776 > 0 A C − B 2 = ( 90 ) ( 90 ) − ( − 18 ) 2 = 8100 − 324 = 7776 > 0 , A > 0 A > 0 A > 0 , 所以 ( − 3 , − 3 ) (-3, -3) ( − 3 , − 3 ) 是极小值点, 极小值为 f ( − 3 , − 3 ) = ( − 3 ) 4 + ( − 3 ) 4 − 9 ( − 3 − 3 ) 2 = 81 + 81 − 9 ( 36 ) = 162 − 324 = − 162 f(-3,-3) = (-3)^4 + (-3)^4 - 9(-3-3)^2 = 81 + 81 - 9(36) = 162 - 324 = -162 f ( − 3 , − 3 ) = ( − 3 ) 4 + ( − 3 ) 4 − 9 ( − 3 − 3 ) 2 = 81 + 81 − 9 ( 36 ) = 162 − 324 = − 162 。
对于 ( 0 , 0 ) (0,0) ( 0 , 0 ) ,需要进一步分析。沿 y = 0 y=0 y = 0 ,
f ( x , 0 ) = x 4 − 9 x 2 < 0 ( 0 < ∣ x ∣ < 3 ) , f(x,0)=x^4-9x^2<0\qquad(0<|x|<3), f ( x , 0 ) = x 4 − 9 x 2 < 0 ( 0 < ∣ x ∣ < 3 ) ,
而沿 y = − x y=-x y = − x ,
f ( x , − x ) = 2 x 4 > 0 ( x ≠ 0 ) . f(x,-x)=2x^4>0\qquad(x\ne0). f ( x , − x ) = 2 x 4 > 0 ( x = 0 ) .
因此任意小的原点邻域内都有正值和负值,故 ( 0 , 0 ) (0,0) ( 0 , 0 ) 是鞍点。
此外,
x 4 + y 4 − 9 ( x + y ) 2 ≥ 1 2 ( x 2 + y 2 ) 2 − 18 ( x 2 + y 2 ) ⟶ + ∞ x^4+y^4-9(x+y)^2
\geq\frac12(x^2+y^2)^2-18(x^2+y^2)\longrightarrow+\infty x 4 + y 4 − 9 ( x + y ) 2 ≥ 2 1 ( x 2 + y 2 ) 2 − 18 ( x 2 + y 2 ) ⟶ + ∞
当 x 2 + y 2 → ∞ x^2+y^2\to\infty x 2 + y 2 → ∞ 。所以两个极小值点 ( 3 , 3 ) (3,3) ( 3 , 3 ) 和 ( − 3 , − 3 ) (-3,-3) ( − 3 , − 3 ) 也是全局最小值点,全局最小值为 − 162 \boxed{-162} − 162 ;不存在极大值。
小問3
首先,将直角坐标转换为极坐标: x = r cos θ , y = r sin θ x = r\cos\theta, y = r\sin\theta x = r cos θ , y = r sin θ , 并且 x 2 + y 2 = r 2 x^2+y^2=r^2 x 2 + y 2 = r 2 , d x d y = r d r d θ dxdy = rdrd\theta d x d y = r d r d θ 。
积分区域D变为 0 ≤ r ≤ 2 , 0 ≤ θ ≤ 2 π 0 \leq r \leq \sqrt{2}, 0 \leq \theta \leq 2\pi 0 ≤ r ≤ 2 , 0 ≤ θ ≤ 2 π 。
原积分变为:
∬ D 2 − x 2 − y 2 2 + x 2 + y 2 d x d y = ∫ 0 2 π ∫ 0 2 2 − r 2 2 + r 2 r d r d θ \iint_{D} \sqrt{\frac{2-x^2-y^2}{2+x^2+y^2}}dxdy = \int_0^{2\pi} \int_0^{\sqrt{2}} \sqrt{\frac{2-r^2}{2+r^2}}rdrd\theta ∬ D 2 + x 2 + y 2 2 − x 2 − y 2 d x d y = ∫ 0 2 π ∫ 0 2 2 + r 2 2 − r 2 r d r d θ
令 u = r 2 u = r^2 u = r 2 , 则 d u = 2 r d r du = 2rdr d u = 2 r d r , 所以 r d r = 1 2 d u rdr = \frac{1}{2}du r d r = 2 1 d u 。
当 r = 0 r=0 r = 0 时, u = 0 u=0 u = 0 。当 r = 2 r=\sqrt{2} r = 2 时, u = 2 u=2 u = 2 。
积分变为:
∫ 0 2 π ∫ 0 2 2 − u 2 + u 1 2 d u d θ = 1 2 ∫ 0 2 π ∫ 0 2 2 − u 2 + u d u d θ \int_0^{2\pi} \int_0^{2} \sqrt{\frac{2-u}{2+u}}\frac{1}{2}dud\theta = \frac{1}{2} \int_0^{2\pi} \int_0^{2} \sqrt{\frac{2-u}{2+u}}dud\theta ∫ 0 2 π ∫ 0 2 2 + u 2 − u 2 1 d u d θ = 2 1 ∫ 0 2 π ∫ 0 2 2 + u 2 − u d u d θ
考虑积分 ∫ 0 2 2 − u 2 + u d u \int_0^{2} \sqrt{\frac{2-u}{2+u}}du ∫ 0 2 2 + u 2 − u d u 。
令 u = 2 cos ( 2 v ) u = 2\cos(2v) u = 2 cos ( 2 v ) , 则 d u = − 4 sin ( 2 v ) d v du = -4\sin(2v)dv d u = − 4 sin ( 2 v ) d v 。
当 u = 0 u=0 u = 0 时, 2 cos ( 2 v ) = 0 2\cos(2v) = 0 2 cos ( 2 v ) = 0 , 则 2 v = π 2 2v = \frac{\pi}{2} 2 v = 2 π , v = π 4 v = \frac{\pi}{4} v = 4 π 。
当 u = 2 u=2 u = 2 时, 2 cos ( 2 v ) = 2 2\cos(2v) = 2 2 cos ( 2 v ) = 2 , 则 cos ( 2 v ) = 1 \cos(2v) = 1 cos ( 2 v ) = 1 , 2 v = 0 2v = 0 2 v = 0 , v = 0 v = 0 v = 0 。
因此,
2 − u 2 + u = 2 − 2 cos ( 2 v ) 2 + 2 cos ( 2 v ) = 1 − cos ( 2 v ) 1 + cos ( 2 v ) = 2 sin 2 ( v ) 2 cos 2 ( v ) = tan 2 ( v ) = tan ( v ) \sqrt{\frac{2-u}{2+u}} = \sqrt{\frac{2-2\cos(2v)}{2+2\cos(2v)}} = \sqrt{\frac{1-\cos(2v)}{1+\cos(2v)}} = \sqrt{\frac{2\sin^2(v)}{2\cos^2(v)}} = \sqrt{\tan^2(v)} = \tan(v) 2 + u 2 − u = 2 + 2 cos ( 2 v ) 2 − 2 cos ( 2 v ) = 1 + cos ( 2 v ) 1 − cos ( 2 v ) = 2 cos 2 ( v ) 2 sin 2 ( v ) = tan 2 ( v ) = tan ( v )
则积分变为:
∫ π / 4 0 tan ( v ) ( − 4 sin ( 2 v ) ) d v = 4 ∫ 0 π / 4 tan ( v ) ( 2 sin ( v ) cos ( v ) ) d v = 8 ∫ 0 π / 4 sin ( v ) cos ( v ) sin ( v ) cos ( v ) d v = 8 ∫ 0 π / 4 sin 2 ( v ) d v \int_{\pi/4}^{0} \tan(v)(-4\sin(2v))dv = 4\int_0^{\pi/4} \tan(v)(2\sin(v)\cos(v))dv = 8 \int_0^{\pi/4} \frac{\sin(v)}{\cos(v)} \sin(v)\cos(v)dv = 8\int_0^{\pi/4} \sin^2(v)dv ∫ π /4 0 tan ( v ) ( − 4 sin ( 2 v )) d v = 4 ∫ 0 π /4 tan ( v ) ( 2 sin ( v ) cos ( v )) d v = 8 ∫ 0 π /4 cos ( v ) sin ( v ) sin ( v ) cos ( v ) d v = 8 ∫ 0 π /4 sin 2 ( v ) d v
∫ 0 π / 4 sin 2 ( v ) d v = ∫ 0 π / 4 1 − cos ( 2 v ) 2 d v = 1 2 [ v − sin ( 2 v ) 2 ] 0 π / 4 = 1 2 [ π 4 − sin ( π / 2 ) 2 ] = 1 2 ( π 4 − 1 2 ) = π 8 − 1 4 \int_0^{\pi/4} \sin^2(v)dv = \int_0^{\pi/4} \frac{1 - \cos(2v)}{2}dv = \frac{1}{2} \left[v - \frac{\sin(2v)}{2}\right]_0^{\pi/4} = \frac{1}{2} \left[\frac{\pi}{4} - \frac{\sin(\pi/2)}{2}\right] = \frac{1}{2} \left(\frac{\pi}{4} - \frac{1}{2}\right) = \frac{\pi}{8} - \frac{1}{4} ∫ 0 π /4 sin 2 ( v ) d v = ∫ 0 π /4 2 1 − cos ( 2 v ) d v = 2 1 [ v − 2 sin ( 2 v ) ] 0 π /4 = 2 1 [ 4 π − 2 sin ( π /2 ) ] = 2 1 ( 4 π − 2 1 ) = 8 π − 4 1
因此,
∫ 0 2 2 − u 2 + u d u = 8 ( π 8 − 1 4 ) = π − 2 \int_0^{2} \sqrt{\frac{2-u}{2+u}}du = 8\left(\frac{\pi}{8} - \frac{1}{4}\right) = \pi - 2 ∫ 0 2 2 + u 2 − u d u = 8 ( 8 π − 4 1 ) = π − 2
原积分变为:
1 2 ∫ 0 2 π ( π − 2 ) d θ = 1 2 ( π − 2 ) ∫ 0 2 π d θ = 1 2 ( π − 2 ) [ θ ] 0 2 π = 1 2 ( π − 2 ) ( 2 π ) = π ( π − 2 ) = π 2 − 2 π \frac{1}{2} \int_0^{2\pi} (\pi - 2) d\theta = \frac{1}{2} (\pi - 2) \int_0^{2\pi} d\theta = \frac{1}{2} (\pi - 2) [\theta]_0^{2\pi} = \frac{1}{2} (\pi - 2) (2\pi) = \pi(\pi - 2) = \pi^2 - 2\pi 2 1 ∫ 0 2 π ( π − 2 ) d θ = 2 1 ( π − 2 ) ∫ 0 2 π d θ = 2 1 ( π − 2 ) [ θ ] 0 2 π = 2 1 ( π − 2 ) ( 2 π ) = π ( π − 2 ) = π 2 − 2 π
因此,
∬ D 2 − x 2 − y 2 2 + x 2 + y 2 d x d y = π 2 − 2 π \iint_{D} \sqrt{\frac{2-x^2-y^2}{2+x^2+y^2}}dxdy = \pi^2 - 2\pi ∬ D 2 + x 2 + y 2 2 − x 2 − y 2 d x d y = π 2 − 2 π