通过两次分部积分证明:∫e2xsin⁡x dx=15e2x(2sin⁡x−cos⁡x)+c.\int e^{2x}\sin x\,dx=\tfrac{1}{5}e^{2x}(2\sin x-\cos x)+c. 下图显示了阴影区域 RR,该区域由曲线 y=ex−π/2sin⁡xy= e^{x-\pi/2}\sqrt{\sin x} 的一部分、直线 4x=π(y+1)4x=\pi(y+1) 和 xx 轴围成。直线 4x=π(y+1)4x=\pi(y+1) 分别在 (π2,1)\left(\dfrac{\pi}{2},1\right) 和 (π4,0)\left(\dfrac{\pi}{4},0\right) 处与曲线和 xx 轴相交。 证明当区域 RR 绕 xx 轴旋转 2π2\pi 弧度时,所产生的体积由 Aπ(B+e−π)+Cπr2A\pi(B+e^{-\pi})+C\pi r^2 给出,其中 AA、BB 和 CC 是待确定的常数。

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完整解法

3(a)

1. Set up and apply the first integration by parts.

Let I=∫e2xsin⁡x dxI = \int e^{2x}\sin x\,dx.
Using the integration by parts formula ∫udvdx dx=uv−∫vdudx dx\int u \frac{dv}{dx} \, dx = uv - \int v \frac{du}{dx} \, dx, we choose u=e2xu = e^{2x} and dvdx=sin⁡x\frac{dv}{dx} = \sin x.
Then dudx=2e2x\frac{du}{dx} = 2e^{2x} and v=−cos⁡xv = -\cos x.
I=−e2xcos⁡x−∫(−cos⁡x)(2e2x) dxI = -e^{2x}\cos x - \int (-\cos x)(2e^{2x})\,dx
I=−e2xcos⁡x+2∫e2xcos⁡x dxI = -e^{2x}\cos x + 2\int e^{2x}\cos x\,dx

2. Apply integration by parts a second time on the new integral.

For the remaining integral ∫e2xcos⁡x dx\int e^{2x}\cos x\,dx, we apply integration by parts again, choosing u=e2xu = e^{2x} and dvdx=cos⁡x\frac{dv}{dx} = \cos x.
Then dudx=2e2x\frac{du}{dx} = 2e^{2x} and v=sin⁡xv = \sin x.
∫e2xcos⁡x dx=e2xsin⁡x−∫(sin⁡x)(2e2x) dx\int e^{2x}\cos x\,dx = e^{2x}\sin x - \int (\sin x)(2e^{2x})\,dx
∫e2xcos⁡x dx=e2xsin⁡x−2∫e2xsin⁡x dx\int e^{2x}\cos x\,dx = e^{2x}\sin x - 2\int e^{2x}\sin x\,dx

3. Substitute the result of the second integration back to form an equation in terms of the original integral.

Substitute this result back into the expression for II:
I=−e2xcos⁡x+2(e2xsin⁡x−2∫e2xsin⁡x dx)I = -e^{2x}\cos x + 2\left(e^{2x}\sin x - 2\int e^{2x}\sin x\,dx\right)
Recognising that the original integral has reappeared on the right-hand side, we replace ∫e2xsin⁡x dx\int e^{2x}\sin x\,dx with II:
I=−e2xcos⁡x+2e2xsin⁡x−4II = -e^{2x}\cos x + 2e^{2x}\sin x - 4I

4. Solve algebraically for the original integral to obtain the final expression.

Bring all terms involving II to the left-hand side:
I+4I=2e2xsin⁡x−e2xcos⁡xI + 4I = 2e^{2x}\sin x - e^{2x}\cos x
5I=e2x(2sin⁡x−cos⁡x)5I = e^{2x}(2\sin x - \cos x)
Divide by 5 and add an arbitrary constant of integration cc:
I=15e2x(2sin⁡x−cos⁡x)+cI = \frac{1}{5}e^{2x}(2\sin x - \cos x) + c
∫e2xsin⁡x dx=15e2x(2sin⁡x−cos⁡x)+c\int e^{2x}\sin x\,dx = \tfrac{1}{5}e^{2x}(2\sin x - \cos x) + c (shown)

答案

∫e2xsin⁡x dx=15e2x(2sin⁡x−cos⁡x)+c\int e^{2x}\sin x\,dx = \tfrac{1}{5}e^{2x}(2\sin x - \cos x) + c

3(b)

1. Set up the volume as (solid under curve) − (cone under line)

The curve y=ex−π/2sin⁡xy=e^{x-\pi/2}\sqrt{\sin x} meets the xx-axis at the origin (where sin⁡x=0\sin x=0) and reaches (π2,1)(\tfrac{\pi}{2},1). The region RR is bounded below by the xx-axis from x=0x=0 to x=π4x=\tfrac{\pi}{4}, on the right by the line from (π4,0)(\tfrac{\pi}{4},0) to (π2,1)(\tfrac{\pi}{2},1), and above by the curve. Rotating about the xx-axis:
V=π∫0π/2ycurve2 dx−(cone from the line between x=π4 and x=π2).V=\pi\int_{0}^{\pi/2}y_{\text{curve}}^{2}\,dx-\Big(\text{cone from the line between }x=\tfrac{\pi}{4}\text{ and }x=\tfrac{\pi}{2}\Big).
Here ycurve2=e2(x−π/2)sin⁡x=e2x−πsin⁡xy_{\text{curve}}^{2}=e^{2(x-\pi/2)}\sin x=e^{2x-\pi}\sin x.

2. Evaluate the curve volume using part (a)

π∫0π/2e2x−πsin⁡x dx=πe−π∫0π/2e2xsin⁡x dx.\pi\int_{0}^{\pi/2}e^{2x-\pi}\sin x\,dx=\pi e^{-\pi}\int_{0}^{\pi/2}e^{2x}\sin x\,dx.
Using part (a), ∫e2xsin⁡x dx=15e2x(2sin⁡x−cos⁡x)\int e^{2x}\sin x\,dx=\tfrac{1}{5}e^{2x}(2\sin x-\cos x):
[15e2x(2sin⁡x−cos⁡x)]0π/2=15eπ(2)−15e0(−1)=15(2eπ+1).\Big[\tfrac{1}{5}e^{2x}(2\sin x-\cos x)\Big]_{0}^{\pi/2}=\tfrac{1}{5}e^{\pi}(2)-\tfrac{1}{5}e^{0}(-1)=\tfrac{1}{5}(2e^{\pi}+1).

3. Simplify the curve volume to the required form

πe−π⋅15(2eπ+1)=15π(2+e−π).\pi e^{-\pi}\cdot\tfrac{1}{5}(2e^{\pi}+1)=\tfrac{1}{5}\pi\left(2+e^{-\pi}\right).
This is the Aπ(B+e−π)A\pi(B+e^{-\pi}) term with A=15A=\tfrac{1}{5}, B=2B=2.

4. Compute the cone volume and combine

The line from (π4,0)(\tfrac{\pi}{4},0) to (π2,1)(\tfrac{\pi}{2},1) generates a cone of radius r=1r=1 and height h=π2−π4=π4h=\tfrac{\pi}{2}-\tfrac{\pi}{4}=\tfrac{\pi}{4}:
Vcone=13πr2h=13π(1)2⋅π4=π212.V_{\text{cone}}=\tfrac{1}{3}\pi r^{2}h=\tfrac{1}{3}\pi(1)^{2}\cdot\tfrac{\pi}{4}=\tfrac{\pi^{2}}{12}.
Therefore
V=15π(2+e−π)−13πr2h=15π(2+e−π)−π212,V=\tfrac{1}{5}\pi\left(2+e^{-\pi}\right)-\tfrac{1}{3}\pi r^{2}h=\tfrac{1}{5}\pi\left(2+e^{-\pi}\right)-\tfrac{\pi^{2}}{12},
so A=15A=\tfrac{1}{5}, B=2B=2, C=−13C=-\tfrac{1}{3}.

答案

V=15π(2+e−π)−13πr2h=15π(2+e−π)−π212V=\tfrac{1}{5}\pi\left(2+e^{-\pi}\right)-\tfrac{1}{3}\pi r^2h=\tfrac{1}{5}\pi\left(2+e^{-\pi}\right)-\tfrac{\pi^2}{12} so A=15A=\tfrac{1}{5}, B=2B=2, C=−13C=-\tfrac{1}{3} (cone with r=1r=1, h=π4h=\tfrac{\pi}{4}).

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