9.2: Ortogonalización Gram-Schmidt
- Page ID
- 113131
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)Supongamos que\(M\) es un subespacio\(m\) -dimensional con base
\[\{x_{1}, \cdots, x_{m}\} \nonumber\]
Transformamos esto en una base ortonormal
\[\{q_{1}, \cdots, q_{m}\} \nonumber\]
para\(M\) vía
1. Set\(y_{1} = x_{1}\) y\(q_{1} = \frac{y_{1}}{||y_{1}||}\)
2. \(y_{2} = x_{2}\)menos la proyección de\(x_{2}\) sobre la línea abarcada por\(q_{1}\).
Es decir,\[y_{2} = x_{2}-q_{1}(q_{1}^{T}q_{1})^{-1}q_{1}^{T}x_{2} = x_{2}-q_{1}q_{1}^{T}x_{2} \nonumber\]
Set\(q_{2} = \frac{y_{2}}{||y_{2}||}\) y\(Q_{2} = \{q_{1}, q_{2}\}\)
3. \(y_{3} = x_{3}\)menos la proyección de\(x_{3}\) sobre el plano abarcado por\(q_{1}\) y\(q_{2}\). Es decir,
\[y_{3} = x_{3}-Q_{2}(Q_{2}^{T}Q_{2})^{-1}Q_{2}^{T} x_{3} = x_{3}-q_{1}q_{1}^{T}x_{3} \nonumber\]
Establecer\(q_{3} = \frac{y_{3}}{||y_{3}||}\) y\(Q_{3} = \{q_{1}, q_{2}, q_{3}\}\). Continuar de esta manera a través del paso (m)
- (m)\(y_{m} = x_{m}\) menos su proyección sobre el subespacio abarcado por las columnas de\(Q_{m-1}\)
\[y_{m} = x_{m}-Q_{m-1}(Q_{m-1}^{T}Q_{m-1})^{-1}Q_{m-1}^{T} x_{m}x_{m}- \sum_{j=1}^{m-1} q_{j}q_{j}^{T} x_{m} \nonumber\]
Set\(q_{m} = \frac{y_{m}}{||y_{m}||}\). Para tomar un ejemplo sencillo, ortogonalicemos las siguientes bases para\(\mathbb{R}^3\)
\[\begin{array}{ccc} {x_{1} = \begin{pmatrix} {1}\\{0}\\{0} \end{pmatrix}}&{x_{2} = \begin{pmatrix} {1}\\{1}\\{0} \end{pmatrix}}&{x_{3} = \begin{pmatrix} {1}\\{1}\\{1} \end{pmatrix}} \end{array} \nonumber\]
- \(q_{1} = y_{1} = x_{1}\)
- \(y_{2} = x_{2}-q_{1}q_{1}^{T}x_{2} = \begin{pmatrix} {0}&{1}&{0} \end{pmatrix}^T\)y así,\(q_{2} = y_{2}\)
- \(y_{3} = x_{3}-q_{2}q_{2}^{T}x_{3} = \begin{pmatrix} {0}&{0}&{1} \end{pmatrix}^T\)y así,\(q_{3} = y_{3}\)
Hemos llegado a
\[\begin{array}{ccc} {q_{1} = \begin{pmatrix} {1}\\{0}\\{0} \end{pmatrix}}&{q_{2} = \begin{pmatrix} {0}\\{1}\\{0} \end{pmatrix}}&{q_{3} = \begin{pmatrix} {0}\\{0}\\{1} \end{pmatrix}} \end{array} \nonumber\]
Una vez que se capta la idea, es mejor dejar los cálculos reales en manos de una máquina. Matlab logra esto a través del comando orth. Su implementación es un poco más sofisticada que una carrera a ciegas a través de nuestros pasos (1) a (m). En consecuencia, no hay garantía de que devolverá la misma base. Por ejemplo
>>X=[1 1 1;0 1 1 ;0 0 1]; >>Q=orth(X) Q= 0.7370 -0.5910 0.3280 0.5910 0.3280 -0.7370 0.3280 0.7370 0.5910
Esta ambigüedad no nos molesta, pues una base ortogonal es tan buena como otra. Pongamos esto en práctica, vía (10.8).