91Ó°ÊÓ

With abasis\(\left\{ {{{\bf{x}}_1}, \ldots ,{{\bf{x}}_p}} \right\}\)for a nonzero subspace \(W\) of \({\mathbb{R}^n}\), the expressionis shown below:

\(\begin{aligned}{}{{\bf{v}}_1} &= {{\bf{x}}_1}\\{{\bf{v}}_2}& = {{\bf{x}}_2} - \frac{{{{\bf{x}}_2} \cdot {{\bf{v}}_1}}}{{{{\bf{v}}_1} \cdot {{\bf{v}}_1}}}{{\bf{v}}_2}\\ \vdots \\{{\bf{v}}_p} &= \frac{{{{\bf{x}}_p} \cdot {{\bf{v}}_1}}}{{{{\bf{v}}_1} \cdot {{\bf{v}}_1}}}{{\bf{v}}_p} - \frac{{{{\bf{x}}_p} \cdot {{\bf{v}}_2}}}{{{{\bf{v}}_2} \cdot {{\bf{v}}_2}}}{{\bf{v}}_p} - \ldots - \frac{{{{\bf{x}}_{p - 1}} \cdot {{\bf{v}}_{p - 1}}}}{{{{\bf{v}}_{p - 1}} \cdot {{\bf{v}}_{p - 1}}}}{{\bf{v}}_{p - 1}}\end{aligned}\)

Therefore, theorthogonal basisfor \(W\) is \(\left\{ {{{\bf{v}}_1}, \ldots ,{{\bf{v}}_p}} \right\}\). Furthermore,

\({\mathop{\rm Span}\nolimits} \left\{ {{{\bf{v}}_1}, \ldots ,{{\bf{v}}_k}} \right\} = {\mathop{\rm Span}\nolimits} \left\{ {{{\bf{x}}_1}, \ldots ,{{\bf{x}}_k}} \right\}\) for \(1 \le k \le p\).

Let \({{\bf{x}}_1} = \left( {\begin{aligned}{{}{}}3\\0\\{ - 1}\end{aligned}} \right),{{\bf{x}}_2} = \left( {\begin{aligned}{{}{}}8\\5\\{ - 6}\end{aligned}} \right)\).

Use a Gram-Schmidt process and let\({{\bf{x}}_1} = {{\bf{v}}_1}\) to calculate \({{\bf{v}}_2}\) as shown below:

\(\begin{aligned}{}{{\bf{v}}_2} &= {{\bf{x}}_2} - \frac{{{{\bf{x}}_2} \cdot {{\bf{v}}_1}}}{{{{\bf{v}}_1} \cdot {{\bf{v}}_1}}}{{\bf{v}}_2}\\ &= {{\bf{x}}_2} - \frac{{30}}{{10}}{{\bf{v}}_1}\\ &= {{\bf{x}}_2} - 3{{\bf{v}}_1}\\ &= \left( {\begin{aligned}{{}{}}8\\5\\{ - 6}\end{aligned}} \right) - 3\left( {\begin{aligned}{*{20}{}}3\\0\\{ - 1}\end{aligned}} \right)\\ &= \left( {\begin{aligned}{{}{}}{8 - 9}\\{5 - 0}\\{ - 6 + 3}\end{aligned}} \right)\\ &= \left( {\begin{aligned}{{}{}}{ - 1}\\5\\{ - 3}\end{aligned}} \right)\end{aligned}\)

Thus, \(\left\{ {\left( {\begin{aligned}{{}{}}3\\0\\{ - 1}\end{aligned}} \right),\left( {\begin{aligned}{{}{}}{ - 1}\\5\\{ - 3}\end{aligned}} \right)} \right\}\) is an orthogonal basis for \(W\).