注意到
$a>0$ $\implies$ ${-a}<{0}$
解构
对区间 $[0,a]$ 应用带Lagrange余项的Taylor公式可知存在 $\eta_{1}\in(\min\{0,a\},\max\{0,a\})$ 使得 $$f(a)=f(0)+f'(0)(a-0)+\frac{f''(\eta_{1})}{2}(a-0)^{2}$$
解构
对区间 $[-a,0]$ 应用带Lagrange余项的Taylor公式可知存在 $\eta_{2}\in(\min\{0,-a\},\max\{0,-a\})$ 使得 $$f(-a)=f(0)+f'(0)(-a-0)+\frac{f''(\eta_{2})}{2}(-a-0)^{2}$$
解构
由于 $f''$ 连续, 应用介值定理可知存在 $\xi\in(\min\{\eta_{1},\eta_{2}\},\max\{\eta_{1},\eta_{2}\})$ 使得 $$f''(\xi)=\frac{f''(\eta_{1})+f''(\eta_{2})}{2}$$
构造
我们断言 $\xi$ 就是所要找的对象, 下面我们证明 $$\xi\in(-a,a)\quad\text{且}\quad f''(\xi)=\frac{f(a)+f(-a)}{a^{2}}$$
目标分解
子目标
$\xi\in(-a,a)$
变形
条件 $\eta_{1}\in(\min\{0,a\},\max\{0,a\})$ 可化简为 $\eta_{1}\in(0,a)$
变形
条件 $\eta_{2}\in(\min\{0,-a\},\max\{0,-a\})$ 可化简为 $\eta_{2}\in(-a,0)$
注意到
$\eta_{2}<{0}$ 且 $\eta_{1}>0$ $\implies$ $\eta_{2}<\eta_{1}$
变形
条件 $\xi\in(\min\{\eta_{1},\eta_{2}\},\max\{\eta_{1},\eta_{2}\})$ 可化简为 $\xi\in(\eta_{2},\eta_{1})$
传递性
由 $\eta_{2}>-a$ , $\xi>\eta_{2}$ , $\xi<\eta_{1}$ , $\eta_{1}<{a}$ 可推出所需结论
$\to$ 证毕
子目标
$f''(\xi)=\frac{f(a)+f(-a)}{a^{2}}$
我们有
$f(a)=f'(0)a+\frac{f''(\eta_{1})}{2}a^{2}$
| $f(a)$ |
$=$ |
$f(0)+f'(0)(a-0)+\frac{f''(\eta_{1})}{2}(a-0)^{2}$ |
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$=$ |
$0+f'(0)(a-0)+\frac{f''(\eta_{1})}{2}(a-0)^{2}$ |
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$=$ |
$f'(0)a+\frac{f''(\eta_{1})}{2}a^{2}$ |
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ring 多项式化简 |
我们有
$f(-a)=f'(0)(-a)+\frac{f''(\eta_{2})}{2}a^{2}$
| $f(-a)$ |
$=$ |
$f(0)+f'(0)(-a-0)+\frac{f''(\eta_{2})}{2}(-a-0)^{2}$ |
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$=$ |
$0+f'(0)(-a-0)+\frac{f''(\eta_{2})}{2}(-a-0)^{2}$ |
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$=$ |
$f'(0)(-a)+\frac{f''(\eta_{2})}{2}a^{2}$ |
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ring 多项式化简 |
计算
$\frac{f(a)+f(-a)}{a^{2}}=f''(\xi)$
$\to$ 证毕
| $\displaystyle\frac{f(a)+f(-a)}{a^{2}}$ |
$=$ |
$\displaystyle\frac{\left(f'(0)a+\frac{f''(\eta_{1})}{2}a^{2}\right)+\left(f'(0)(-a)+\frac{f''(\eta_{2})}{2}a^2\right)}{a^2}$ |
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$=$ |
$\displaystyle\frac{\frac{f''(\eta_{1})+f''(\eta_{2})}{2}a^{2}}{a^{2}}$ |
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ring 多项式化简 |
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$=$ |
$\displaystyle\frac{f''(\eta_{1})+f''(\eta_{2})}{2}$ |
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$a\cdot b/b=a$ 对一切 $b\ne 0$ 成立 |
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$=$ |
$f''(\xi)$ |
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