求 ∫x2e−2x dx\displaystyle\int x^{2}e^{-2x}\,\mathrm{d}x。 方程为 y=xe−xy = xe^{-x} 的曲线与方程为 y=1exy=\tfrac{1}{e}x 的直线相交于原点 OO 和 xx 坐标为 1 的点 PP。区域 RR 由该曲线和直线所围成(见图)。 求区域 RR 绕 xx 轴旋转 360∘360^\circ 形成的旋转体的确切体积。

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完整解法

6(i)

1. Set up the first integration by parts

Let u=x2  ⟹  dudx=2xu = x^2 \implies \frac{\mathrm{d}u}{\mathrm{d}x} = 2x
Let dvdx=e−2x  ⟹  v=−12e−2x\frac{\mathrm{d}v}{\mathrm{d}x} = e^{-2x} \implies v = -\frac{1}{2}e^{-2x}

2. Apply the integration by parts formula

∫x2e−2x dx=x2(−12e−2x)−∫(−12e−2x)(2x) dx\int x^2 e^{-2x} \,\mathrm{d}x = x^2 \left(-\frac{1}{2}e^{-2x}\right) - \int \left(-\frac{1}{2}e^{-2x}\right)(2x) \,\mathrm{d}x
=−12x2e−2x+∫xe−2x dx= -\frac{1}{2}x^2 e^{-2x} + \int x e^{-2x} \,\mathrm{d}x

3. Apply integration by parts a second time to the new integral

For ∫xe−2x dx\int x e^{-2x} \,\mathrm{d}x, let u=x  ⟹  dudx=1u = x \implies \frac{\mathrm{d}u}{\mathrm{d}x} = 1
and dvdx=e−2x  ⟹  v=−12e−2x\frac{\mathrm{d}v}{\mathrm{d}x} = e^{-2x} \implies v = -\frac{1}{2}e^{-2x}.
∫xe−2x dx=x(−12e−2x)−∫(−12e−2x)(1) dx\int x e^{-2x} \,\mathrm{d}x = x \left(-\frac{1}{2}e^{-2x}\right) - \int \left(-\frac{1}{2}e^{-2x}\right)(1) \,\mathrm{d}x
=−12xe−2x+12∫e−2x dx= -\frac{1}{2}x e^{-2x} + \frac{1}{2}\int e^{-2x} \,\mathrm{d}x

4. Evaluate the final integral and state the complete result with the constant of integration

12∫e−2x dx=12(−12e−2x)=−14e−2x\frac{1}{2}\int e^{-2x} \,\mathrm{d}x = \frac{1}{2} \left(-\frac{1}{2}e^{-2x}\right) = -\frac{1}{4}e^{-2x}
Substituting this back into the original expression gives:
∫x2e−2x dx=−12x2e−2x−12xe−2x−14e−2x+C\int x^2 e^{-2x} \,\mathrm{d}x = -\frac{1}{2}x^2 e^{-2x} - \frac{1}{2}x e^{-2x} - \frac{1}{4}e^{-2x} + C

答案

−12x2e−2x−12xe−2x−14e−2x+C-\frac{1}{2}x^2 e^{-2x} - \frac{1}{2}x e^{-2x} - \frac{1}{4}e^{-2x} + C

6(ii)

1. Calculate the indefinite integral from part (i), which is required for this part, using integration by parts.

Let I=∫x2e−2x dxI = \displaystyle\int x^{2}e^{-2x}\,\mathrm{d}x. Using integration by parts with u=x2u = x^2 and dvdx=e−2x\frac{\mathrm{d}v}{\mathrm{d}x} = e^{-2x}:
I=−12x2e−2x−∫(−12e−2x)(2x) dx=−12x2e−2x+∫xe−2x dxI = -\frac{1}{2}x^2e^{-2x} - \int \left(-\frac{1}{2}e^{-2x}\right)(2x)\,\mathrm{d}x = -\frac{1}{2}x^2e^{-2x} + \int xe^{-2x}\,\mathrm{d}x
Using integration by parts again for ∫xe−2x dx\displaystyle\int xe^{-2x}\,\mathrm{d}x with u=xu = x and dvdx=e−2x\frac{\mathrm{d}v}{\mathrm{d}x} = e^{-2x}:
∫xe−2x dx=−12xe−2x−∫(−12e−2x)(1) dx=−12xe−2x−14e−2x\int xe^{-2x}\,\mathrm{d}x = -\frac{1}{2}xe^{-2x} - \int \left(-\frac{1}{2}e^{-2x}\right)(1)\,\mathrm{d}x = -\frac{1}{2}xe^{-2x} - \frac{1}{4}e^{-2x}
∴∫x2e−2x dx=−12x2e−2x−12xe−2x−14e−2x+C\therefore \int x^{2}e^{-2x}\,\mathrm{d}x = -\frac{1}{2}x^2e^{-2x} - \frac{1}{2}xe^{-2x} - \frac{1}{4}e^{-2x} + C

2. Set up the integral for the volume of revolution for the region bounded between the curve and the line.

The volume of revolution VV about the x-axis is given by:
V=π∫01(ycurve2−yline2)dxV = \pi \int_{0}^{1} \left( y_{\text{curve}}^2 - y_{\text{line}}^2 \right) \mathrm{d}x
V=π∫01((xe−x)2−(1ex)2)dxV = \pi \int_{0}^{1} \left( (xe^{-x})^2 - \left(\frac{1}{e}x\right)^2 \right) \mathrm{d}x
V=π∫01x2e−2x dx−π∫01x2e2 dxV = \pi \int_{0}^{1} x^2e^{-2x} \,\mathrm{d}x - \pi \int_{0}^{1} \frac{x^2}{e^2} \,\mathrm{d}x

3. Evaluate the exact volume generated by rotating the region under the curve.

Using the integral found in part (i):
Vcurve=π[−12x2e−2x−12xe−2x−14e−2x]01V_{\text{curve}} = \pi \left[ -\frac{1}{2}x^2e^{-2x} - \frac{1}{2}xe^{-2x} - \frac{1}{4}e^{-2x} \right]_0^1
=π((−12e−2−12e−2−14e−2)−(0−0−14))= \pi \left( \left(-\frac{1}{2}e^{-2} - \frac{1}{2}e^{-2} - \frac{1}{4}e^{-2}\right) - \left(0 - 0 - \frac{1}{4}\right) \right)
=π(14−54e−2)= \pi \left( \frac{1}{4} - \frac{5}{4}e^{-2} \right)

4. Evaluate the exact volume generated by rotating the region under the line.

Vline=π∫01x2e2 dxV_{\text{line}} = \pi \int_{0}^{1} \frac{x^2}{e^2} \,\mathrm{d}x
=πe2[x33]01=π3e2= \frac{\pi}{e^2} \left[ \frac{x^3}{3} \right]_0^1 = \frac{\pi}{3e^2}

5. Subtract the two volumes to find the final exact volume.

V=Vcurve−Vline=π(14−54e2)−π3e2V = V_{\text{curve}} - V_{\text{line}} = \pi \left( \frac{1}{4} - \frac{5}{4e^2} \right) - \frac{\pi}{3e^2}
V=π(14−1512e2−412e2)V = \pi \left( \frac{1}{4} - \frac{15}{12e^2} - \frac{4}{12e^2} \right)
V=π(14−1912e2)V = \pi \left( \frac{1}{4} - \frac{19}{12e^2} \right)

答案

π(14−1912e2)\pi \left( \frac{1}{4} - \frac{19}{12e^2} \right)

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