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@ -22,26 +22,42 @@
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**解析**
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$$H^TH
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\begin{align*}
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H^T &= (E - l\alpha\alpha^T)^T = E - l\alpha\alpha^T \\
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H^TH &= (E - l\alpha\alpha^T)(E - l\alpha\alpha^T) \\
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解题思路
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正交矩阵的定义是:若矩阵 H 满足 $H^T H = E$(其中 E 为单位矩阵),则 H 为正交矩阵。我们从这个定义出发推导条件。
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步骤1:写出 $H^T$
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已知 $H = E - l\alpha\alpha^T$,转置得
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$$H^T = (E - l\alpha\alpha^T)^T = E^T - l(\alpha\alpha^T)^T = E - l\alpha\alpha^T$$
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(因为 $E^T=E$,且 $(\alpha\alpha^T)^T = \alpha\alpha^T$)
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步骤2:计算 $H^T H$
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$$\begin{align*}
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H^T H &= (E - l\alpha\alpha^T)(E - l\alpha\alpha^T) \\
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&= E \cdot E - E \cdot l\alpha\alpha^T - l\alpha\alpha^T \cdot E + l^2\alpha\alpha^T \cdot \alpha\alpha^T \\
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&= E - 2l\alpha\alpha^T + l^2\alpha(\alpha^T\alpha)\alpha^T \\
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&= E - 2l\alpha\alpha^T + l^2k^2\alpha\alpha^T \\
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&= E + \left(-2l + l^2k^2\right)\alpha\alpha^T
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&= E - 2l\alpha\alpha^T + l^2\alpha(\alpha^T\alpha)\alpha^T
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\end{align*}$$
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令 $H^TH = E$
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要使 $H^TH = E$,必须满足:
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$$\left(-2l + l^2k^2\right)\alpha\alpha^T = O$$
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若 $\alpha \neq \boldsymbol{0}$(即 $k \neq 0$),则 $\alpha\alpha^T \neq O$,故
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$$-2l + l^2k^2 = 0 \implies l(lk^2 - 2) = 0$$
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解得 $l = 0$或 $l = \dfrac{2}{k^2}$。
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故
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若 $\alpha = \boldsymbol{0}$(即 k = 0),则 $H = E$,显然 H 是正交矩阵,此时 $l$ 可取任意实数。
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当 k = 0(即$\alpha = \boldsymbol{0}$)时,H = E 恒为正交矩阵,$l$ 为任意实数。
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当 $k \neq 0$(即 $\alpha \neq \boldsymbol{0}$)时,H 为正交矩阵当且仅当 $l = 0 或 l = \dfrac{2}{k^2}$。
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步骤3:代入$\alpha^T\alpha = \|\alpha\|^2 = k^2$
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$$H^T H = E - 2l\alpha\alpha^T + l^2 k^2 \alpha\alpha^T$$
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合并同类项:
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$$H^T H = E + \left(-2l + l^2 k^2\right)\alpha\alpha^T$$
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步骤4:令 $H^T H = E$
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要使上式等于单位矩阵 E,必须满足:
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$$\left(-2l + l^2 k^2\right)\alpha\alpha^T = O$$
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(O 为零矩阵)
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若 $\alpha \neq 0(即 k \neq 0)$,则$\alpha\alpha^T \neq O$,因此系数必须为0:
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$$-2l + l^2 k^2 = 0 \implies l(l k^2 - 2) = 0$$
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解得$l = 0$ 或 $l = \dfrac{2}{k^2}$。
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若 $\alpha = 0(即 k = 0$),则 H = E,显然 E 是正交矩阵,此时对任意$l \in \mathbb{R}$ 均成立。
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最终结论
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$$\boxed{
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\begin{aligned}
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&1.\ \text{当}\ k = 0\ \text{时,对任意实数}\ l,\ H\ \text{为正交矩阵;} \\
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&2.\ \text{当}\ k \neq 0\ \text{时,}l = 0\ \text{或}\ l = \dfrac{2}{k^2}\ \text{时,}H\ \text{为正交矩阵。}
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\end{aligned}
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}
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$$
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@ -52,15 +68,15 @@ $$-2l + l^2k^2 = 0 \implies l(lk^2 - 2) = 0$$
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**解析**
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证明
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设 A为 n阶正交矩阵(n≥2),则
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$$\boldsymbol{A}^\top\boldsymbol{A}=\boldsymbol{E}$$
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$$\boldsymbol{A}^T\boldsymbol{A}=\boldsymbol{E}$$
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又由伴随矩阵与逆矩阵的关系:
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$$A^{-1} = \frac{1}{|A|} \text{adj}(A)$$
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$$\boldsymbol A^{-1} = \frac{1}{|A|}\boldsymbol{A}^*$$
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联立得
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$$\boldsymbol{A}\top\boldsymbol= \frac{1}{|A|} \text{adj}(A)$$
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$$\boldsymbol{A}^T= \frac{1}{|A|}\boldsymbol A^*$$
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正交矩阵的行列式满足 $\frac{1}{|A|} =±1$,故
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$adj(A)=(detA)AT=±AT$
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由伴随矩阵的定义,其第 (j,i)元为 aij的代数余子式 Aij,而 ±AT的第 (j,i)元为 ±aij。比较对应元素得
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$$Aij=±aij,i,j=1,2,…,n.$$
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$A^*={|A|}A^T=±A^T$
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由伴随矩阵的定义,其第 (j,i)元为 $a_{ij}$的代数余子式 $A_{ij}$,而 $±A^T$的第 (j,i)元为 $±a_{ij}$。比较对应元素得
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$$A_{ij}=±a_{ij},i,j=1,2,…,n.$$
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证毕
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@ -77,21 +93,20 @@ $$\begin{align*}
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\boldsymbol{u}_k &= \boldsymbol{\alpha}_k - \sum_{i=1}^{k-1}\frac{\langle\boldsymbol{\alpha}_k,\boldsymbol{u}_i\rangle}{\langle\boldsymbol{u}_i,\boldsymbol{u}_i\rangle}\boldsymbol{u}_i,\quad k=2,3,\dots,p.
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\end{align*}$$
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单位化过程
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$$\boldsymbol{\varepsilon}_1 = \frac{\boldsymbol{\alpha}_1}{\|\boldsymbol{\alpha}_1\|}$$
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$$\boldsymbol{\varepsilon}_k = \frac{\boldsymbol{u}_k}{\|\boldsymbol{u}_k\|},\quad
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k=2,3,\dots,p$$
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k=1,2,3,\dots,p$$
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### **例子**
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>[!example] **例1**
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已知 为欧氏空间 V 的一组标准正交基,令$\boldsymbol{\alpha}_1,\boldsymbol{\alpha}_2,\dots,\boldsymbol{\alpha}_5$ $$\boldsymbol{\beta}_1 = \boldsymbol{\alpha}_1+\boldsymbol{\alpha}_3,\quad
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已知 $\boldsymbol{\alpha}_1,\boldsymbol{\alpha}_2,\dots,\boldsymbol{\alpha}_5$ 为欧氏空间 V 的一组标准正交基,令$$\boldsymbol{\beta}_1 = \boldsymbol{\alpha}_1+\boldsymbol{\alpha}_3,\quad
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\boldsymbol{\beta}_2 = \boldsymbol{\alpha}_1-\boldsymbol{\alpha}_2+\boldsymbol{\alpha}_4,\quad
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\boldsymbol{\beta}_3 = 2\boldsymbol{\alpha}_1+\boldsymbol{\alpha}_2+\boldsymbol{\alpha}_3,$$
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$U = \text{span}\{\boldsymbol{\beta}_1,\boldsymbol{\beta}_2,\boldsymbol{\beta}_3\}$求 U 的一个标准正交基。
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**解析**。
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**解析**:
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施密特正交化
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步骤1:正交化
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取$$ \boldsymbol{\gamma}_1=\boldsymbol{\beta}_1=\boldsymbol{\alpha}_1+\boldsymbol{\alpha}_3
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取$$ \boldsymbol{\gamma}_1=\boldsymbol{\beta}_1=\boldsymbol{\alpha}_1+\boldsymbol{\alpha}_3,\ \
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\boldsymbol{\gamma}_2=\boldsymbol{\beta}_2-\dfrac{\langle\boldsymbol{\beta}_2,\boldsymbol{\gamma}_1\rangle}{\langle\boldsymbol{\gamma}_1,\boldsymbol{\gamma}_1\rangle}\boldsymbol{\gamma}_1$$$$\langle\boldsymbol{\beta}_2,\boldsymbol{\gamma}_1\rangle=1,\quad
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\langle\boldsymbol{\gamma}_1,\boldsymbol{\gamma}_1\rangle=2$$
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$$\boldsymbol{\gamma}_2=\frac{1}{2}\boldsymbol{\alpha}_1-\boldsymbol{\alpha}_2-\frac{1}{2}\boldsymbol{\alpha}_3+\boldsymbol{\alpha}_4$$
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@ -126,7 +141,7 @@ $$\begin{cases}
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\langle\boldsymbol{x},\boldsymbol{\alpha}_3\rangle = x_1 - 2x_2 + 2x_4 = 0\\
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\langle\boldsymbol{x},\boldsymbol{\alpha}_4\rangle = 2\sqrt{6}x_1 - \sqrt{6}x_3 - \sqrt{6}x_4 = 0 \implies 2x_1 - x_3 - x_4 = 0
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\end{cases}$$
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解上述齐次方程组,基础解系,得到两个线性无关的解:
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解上述齐次方程组,得到两个线性无关的解:
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$$\boldsymbol{\xi}_1=(2,1,4,0)^T,\quad
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\boldsymbol{\xi}_2=(0,1,0,1)^T$$
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正交化
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