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113 台綜大微積分(B) 第 5 題

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113學年度 · 113微積分B · 第 5 題

題目

Problem

5. Evaluate the improper integral

3e3xdx.(10%)\int_3^\infty e^{-\sqrt{3x}} \,\mathrm{d}x \,. \quad (10\%)

解答

解法一:變數代換與伽瑪函數(最速法)

思路

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  1. 本題為廣義積分 3e3xdx\int_3^\infty e^{-\sqrt{3x}} \,\mathrm{d}x
  2. 指數包含根式 3x\sqrt{3x},我們首先進行變數代換以消去根式。
  3. 第一步:選取代換變數: 令 u=3x    u2=3x    2udu=3dx    dx=23uduu = \sqrt{3x} \implies u^2 = 3x \implies 2u\,\mathrm{d}u = 3\,\mathrm{d}x \implies \mathrm{d}x = \frac{2}{3}u\,\mathrm{d}u
  4. 第二步:更換積分上下限
    • x=3    u=9=3x = 3 \implies u = \sqrt{9} = 3
    • x    ux \to \infty \implies u \to \infty
    • 積分式化為: I=233ueuduI = \frac{2}{3} \int_3^\infty u e^{-u} \,\mathrm{d}u
  5. 第三步:利用平移變數將下限化為 0 並引入 Gamma 函數
    • t=u3    u=t+3,du=dtt = u - 3 \implies u = t + 3, \mathrm{d}u = \mathrm{d}t
    • u=3    t=0u = 3 \implies t = 0
    • 積分變為: I=230(t+3)e(t+3)dt=23e30(t+3)etdtI = \frac{2}{3} \int_0^\infty (t+3) e^{-(t+3)} \,\mathrm{d}t = \frac{2}{3}e^{-3} \int_0^\infty (t+3) e^{-t} \,\mathrm{d}t =23e3(0tetdt+30etdt)= \frac{2}{3}e^{-3} \left( \int_0^\infty t e^{-t} \,\mathrm{d}t + 3 \int_0^\infty e^{-t} \,\mathrm{d}t \right)
    • 利用 0tetdt=Γ(2)=1\int_0^\infty t e^{-t} \,\mathrm{d}t = \Gamma(2) = 10etdt=Γ(1)=1\int_0^\infty e^{-t} \,\mathrm{d}t = \Gamma(1) = 1
    • 代入求得答案。

答題過程

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我們首先引入代換法,令:

u=3x    u2=3x    dx=23uduu = \sqrt{3x} \implies u^2 = 3x \implies \mathrm{d}x = \frac{2}{3} u \,\mathrm{d}u

更換積分限:

  • x=3x = 3 時, u=3(3)=3u = \sqrt{3(3)} = 3
  • xx \to \infty 時, uu \to \infty

將其代回廣義積分中:

3e3xdx=3eu(23udu)=233ueudu\int_3^\infty e^{-\sqrt{3x}} \,\mathrm{d}x = \int_3^\infty e^{-u} \cdot \left( \frac{2}{3} u \,\mathrm{d}u \right) = \frac{2}{3} \int_3^\infty u e^{-u} \,\mathrm{d}u

為了將下限化為 00 以便使用伽瑪函數(Gamma Function)或分部積分,我們令:

t=u3    u=t+3,du=dtt = u - 3 \implies u = t + 3, \quad \mathrm{d}u = \mathrm{d}t

此時當 u=3    t=0u = 3 \implies t = 0。代入得:

233ueudu=230(t+3)e(t+3)dt=23e30(t+3)etdt=23e3(0tetdt+30etdt)\begin{align*} \frac{2}{3} \int_3^\infty u e^{-u} \,\mathrm{d}u =&\, \frac{2}{3} \int_0^\infty (t + 3) e^{-(t+3)} \,\mathrm{d}t \\[4mm] =&\, \frac{2}{3} e^{-3} \int_0^\infty (t + 3) e^{-t} \,\mathrm{d}t \\[4mm] =&\, \frac{2}{3} e^{-3} \left( \int_0^\infty t e^{-t} \,\mathrm{d}t + 3 \int_0^\infty e^{-t} \,\mathrm{d}t \right) \end{align*}

利用伽瑪函數的性質:

  • 0tetdt=Γ(2)=1!=1\displaystyle \int_0^\infty t e^{-t} \,\mathrm{d}t = \Gamma(2) = 1! = 1
  • 0etdt=Γ(1)=0!=1\displaystyle \int_0^\infty e^{-t} \,\mathrm{d}t = \Gamma(1) = 0! = 1

代入數值:

I=23e3(1+3(1))=23e3(4)=83e3=83e3I = \frac{2}{3} e^{-3} \left( 1 + 3(1) \right) = \frac{2}{3} e^{-3} (4) = \frac{8}{3} e^{-3} = \frac{8}{3e^3}

解法二:分部積分法(傳統做法)

思路

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  1. 經過與解法一相同的初次換元,得到 233ueudu\frac{2}{3} \int_3^\infty u e^{-u} \,\mathrm{d}u
  2. 使用分部積分法求解此反常積分:
    • w=u    dw=duw = u \implies \mathrm{d}w = \mathrm{d}u;令 dv=eudu    v=eu\mathrm{d}v = e^{-u}\,\mathrm{d}u \implies v = -e^{-u}
    • 展開: ueu3+3eudu\left. -u e^{-u} \right|_3^\infty + \int_3^\infty e^{-u} \,\mathrm{d}u

答題過程

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經過初次換元 u=3xu = \sqrt{3x},原積分轉化為:

I=233ueuduI = \frac{2}{3} \int_3^\infty u e^{-u} \,\mathrm{d}u

對不定積分使用分部積分法,令:

w=u    dw=duw = u \implies \mathrm{d}w = \mathrm{d}u dv=eudu    v=eu\mathrm{d}v = e^{-u}\,\mathrm{d}u \implies v = -e^{-u}

則有:

ueudu=ueu(eu)du=ueueu=eu(u+1)\int u e^{-u} \,\mathrm{d}u = -u e^{-u} - \int (-e^{-u}) \,\mathrm{d}u = -u e^{-u} - e^{-u} = -e^{-u}(u + 1)

我們將此原函數代回廣義積分,並求極限:

233ueudu=23limb[eu(u+1)]3b=23(limb(eb(b+1))(e3(3+1)))\begin{align*} \frac{2}{3} \int_3^\infty u e^{-u} \,\mathrm{d}u =&\, \frac{2}{3} \lim_{b\to\infty} \left[ -e^{-u}(u + 1) \right]_3^b \\[4mm] =&\, \frac{2}{3} \left( \lim_{b\to\infty} \left( -e^{-b}(b+1) \right) - \left( -e^{-3}(3+1) \right) \right) \end{align*}

由於 limbb+1eb=0\lim_{b\to\infty} \frac{b+1}{e^b} = 0(由羅必達法則知):

I=23(0+4e3)=83e3I = \frac{2}{3} \left( 0 + 4 e^{-3} \right) = \frac{8}{3}e^{-3}

結論: 反常積分值為 83e3\displaystyle \frac{8}{3}e^{-3}