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微分中值定理:还原法构造函数

  • 微分中值定理:还原法构造函数

(2022·上海大学·8) 设 f(x)f(x) 在 R\mathbb{R} 上二阶可导, 且 f(0)=0f(0)=0, 证明: 存在 ξ∈(−π2,π2)\xi \in\left(-\frac{\pi}{2}, \frac{\pi}{2}\right), 使得

f′′(ξ)=3f′(ξ)tan⁡ξ+2f(ξ)f^{\prime \prime}(\xi)=3 f^{\prime}(\xi) \tan \xi+2 f(\xi)

证 设 g(x)=f(x)cos⁡2xg(x)=f(x) \cos ^{2} x(如何构造?往下看)
⇒g′(x)=cos⁡x(f′(x)cos⁡x−2f(x)sin⁡x)\Rightarrow g^{\prime}(x)=\cos x\left(f^{\prime}(x) \cos x-2 f(x) \sin x\right). 由于 f(0)=0f(0)=0,故 g(0)=0g(0)=0 且 g(π2)=0,g(−π2)=0g\left(\frac{\pi}{2}\right)=0, g\left(-\frac{\pi}{2}\right)=0. 利用罗尔中值定理,有

∃ξ1∈(−π2,0),ξ2∈(0,π2)\exists \xi_{1} \in\left(-\frac{\pi}{2}, 0\right), \xi_{2} \in\left(0, \frac{\pi}{2}\right)

使得 g′(ξ1)=g′(ξ2)=0g^{\prime}\left(\xi_{1}\right)=g^{\prime}\left(\xi_{2}\right)=0.

由于cos⁡ξ1≠0\cos \xi_{1} \neq 0 且 cos⁡ξ2≠0\cos \xi_{2} \neq 0, 故令h(x)=f′(x)cos⁡x−2f(x)sin⁡x\left.h(x)=f^{\prime}(x) \cos x-2 f(x) \sin x\right.

有 h(ξ1)=0h\left(\xi_{1}\right)=0 且 h(ξ2)=0h\left(\xi_{2}\right)=0. 而

h′(x)=f′′(x)cos⁡x−3f′(x)sin⁡x−2f(x)cos⁡x.h^{\prime}(x)=f^{\prime \prime}(x) \cos x-3 f^{\prime}(x) \sin x-2 f(x)\cos x.

利用罗尔定理,存在 ξ∈(ξ1,ξ2)\xi \in\left(\xi_{1}, \xi_{2}\right), 使得 f′′(ξ)=3f′(ξ)tan⁡3+2f(ξ)f^{\prime \prime}(\xi)=3 f^{\prime}(\xi) \tan 3+2 f(\xi) .

还原法构造函数
step1: 先将ξ\xi换成xx

f′′(x)=3f′(x)tan⁡x+2f(x)f^{\prime \prime}(x)=3 f^{\prime}(x) \tan x+2 f(x)

step2: 整理如下:

f′′(x)cos⁡x=3f′(x)sin⁡x+2f(x)cos⁡x(f′(x)cos⁡x−f′(x)sin⁡x)−2(f′(x)sin⁡x−f(x)cos⁡x)=0(f′(x)cos⁡x)′−2(f(x)sin⁡x)′=0⇒(f′(x)cos⁡x−2f(x)sin⁡x)′=0\begin{aligned} &f^{\prime \prime}(x) \cos x=3 f^{\prime}(x) \sin x+2 f(x) \cos x\\ &\left(f^{\prime}(x) \cos x-f^{\prime}(x) \sin x\right)-2\left(f^{\prime}(x) \sin x-f(x) \cos x\right)=0\\ &\left(f^{\prime}(x) \cos x\right)^{\prime}-2(f(x) \sin x)^{\prime}=0\\ &\Rightarrow\left(f^{\prime}(x) \cos x-2 f(x) \sin x\right)^{\prime}=0 \end{aligned}

step3: 根据 f′(x)cos⁡x−2f(x)sin⁡x=0f^{\prime}(x) \cos x-2 f(x) \sin x=0用还原法构造:整理为 (ln⁡f(x))′−(ln⁡g(x))′=0(\ln f(x))^{\prime}-\left(\ln g(x)\right)^{\prime}=0 形式.

f′(x)f(x)−2tan⁡x=0⇒(ln⁡f(x))′−2(ln⁡∣cos⁡x∣)′=0(ln⁡f(x))′−(ln⁡cos⁡2x)′=0⇒g(x)=f(x)cos⁡2x.\begin{aligned} &\dfrac{f^{\prime}(x) }{f(x)}-2 \tan x=0\\ &\Rightarrow(\ln f(x))^{\prime}-2(\ln |\cos x|)^{\prime}=0\\ &(\ln f(x))^{\prime}-\left(\ln \cos ^{2} x\right)^{\prime}=0\\ &\Rightarrow g(x)=f(x) \cos ^{2} x. \end{aligned}