Answer on Question #66803–Math–Linear Algebra
Question
Apply the Gram-Schmidt orthogonalization process to find an orthonormal basis for the subspace of R 4 \mathbb{R}^4 R 4 generated by the vectors { ( − 1 , 1 , 0 , 1 ) , ( 1 , 0 , − 1 , 0 ) , ( 1 , 0 , 2 , − 1 ) } \{(-1,1,0,1),(1,0,-1,0),(1,0,2,-1)\} {( − 1 , 1 , 0 , 1 ) , ( 1 , 0 , − 1 , 0 ) , ( 1 , 0 , 2 , − 1 )} .
Solution
Let u 1 = ( − 1 , 1 , 0 , 1 ) u_{1} = (-1,1,0,1) u 1 = ( − 1 , 1 , 0 , 1 ) , u 2 = ( 1 , 0 , − 1 , 0 ) u_{2} = (1,0, -1,0) u 2 = ( 1 , 0 , − 1 , 0 ) , u 3 = ( 1 , 0 , 2 , − 1 ) u_{3} = (1,0,2, -1) u 3 = ( 1 , 0 , 2 , − 1 ) .
By the Gram-Schmidt orthogonalization process { { 1 } , { 2 , pp 544 , 558 } } \{\{1\}, \{2, \text{pp } 544, 558\}\} {{ 1 } , { 2 , pp 544 , 558 }} consider v 1 = ( − 1 , 1 , 0 , 1 ) v_{1} = (-1,1,0,1) v 1 = ( − 1 , 1 , 0 , 1 ) and v 2 = u 2 − u 2 ⋅ v 1 v 1 ⋅ v 1 v 1 v_{2} = u_{2} - \frac{u_{2} \cdot v_{1}}{v_{1} \cdot v_{1}} v_{1} v 2 = u 2 − v 1 ⋅ v 1 u 2 ⋅ v 1 v 1 ;
Note that
u 2 ⋅ v 1 = 1 ⋅ ( − 1 ) + 0 ⋅ 1 + ( − 1 ) ⋅ 0 + 0 ⋅ 1 = − 1 ; v 1 ⋅ v 1 = ∥ v 1 ∥ = ( − 1 ) ⋅ ( − 1 ) + 1 ⋅ 1 + 0 ⋅ 0 + 1 ⋅ 1 = 3. v 2 = u 2 − u 2 ⋅ v 1 v 1 ⋅ v 1 v 1 = ( 1 , 0 , − 1 , 0 ) − ( − 1 ) 3 ( − 1 , 1 , 0 , 1 ) = ( 1 , 0 , − 1 , 0 ) + 1 3 ( − 1 , 1 , 0 , 1 ) = 1 3 ( 2 , 1 , − 3 , 1 ) , \begin{array}{l}
u_{2} \cdot v_{1} = 1 \cdot (-1) + 0 \cdot 1 + (-1) \cdot 0 + 0 \cdot 1 = -1; \\
v_{1} \cdot v_{1} = \|v_{1}\| = (-1) \cdot (-1) + 1 \cdot 1 + 0 \cdot 0 + 1 \cdot 1 = 3. \\
v_{2} = u_{2} - \frac{u_{2} \cdot v_{1}}{v_{1} \cdot v_{1}} v_{1} = (1, 0, -1, 0) - \frac{(-1)}{3} (-1, 1, 0, 1) = (1, 0, -1, 0) + \frac{1}{3} (-1, 1, 0, 1) = \frac{1}{3} (2, 1, -3, 1),
\end{array} u 2 ⋅ v 1 = 1 ⋅ ( − 1 ) + 0 ⋅ 1 + ( − 1 ) ⋅ 0 + 0 ⋅ 1 = − 1 ; v 1 ⋅ v 1 = ∥ v 1 ∥ = ( − 1 ) ⋅ ( − 1 ) + 1 ⋅ 1 + 0 ⋅ 0 + 1 ⋅ 1 = 3. v 2 = u 2 − v 1 ⋅ v 1 u 2 ⋅ v 1 v 1 = ( 1 , 0 , − 1 , 0 ) − 3 ( − 1 ) ( − 1 , 1 , 0 , 1 ) = ( 1 , 0 , − 1 , 0 ) + 3 1 ( − 1 , 1 , 0 , 1 ) = 3 1 ( 2 , 1 , − 3 , 1 ) ,
we can to consider v 2 = ( 2 , 1 , − 3 , 1 ) v_{2} = (2,1, -3,1) v 2 = ( 2 , 1 , − 3 , 1 ) .
Next calculate v 3 = u 3 − u 3 ⋅ v 1 v 1 ⋅ v 1 v 1 − u 3 ⋅ v 2 v 2 ⋅ v 2 v 2 v_{3} = u_{3} - \frac{u_{3} \cdot v_{1}}{v_{1} \cdot v_{1}} v_{1} - \frac{u_{3} \cdot v_{2}}{v_{2} \cdot v_{2}} v_{2} v 3 = u 3 − v 1 ⋅ v 1 u 3 ⋅ v 1 v 1 − v 2 ⋅ v 2 u 3 ⋅ v 2 v 2 ;
u 3 ⋅ v 1 = 1 ⋅ ( − 1 ) + 0 ⋅ 1 + 2 ⋅ 0 + ( − 1 ) ⋅ 1 = − 2 ; u 3 ⋅ v 2 = 1 ⋅ 2 + 0 ⋅ 1 + 2 ⋅ ( − 3 ) + ( − 1 ) ⋅ 1 = − 5 ; v 2 ⋅ v 2 = 2 ⋅ 2 + 1 ⋅ 1 + ( − 3 ) ⋅ ( − 3 ) + 1 ⋅ 1 = 15. \begin{array}{l}
u_{3} \cdot v_{1} = 1 \cdot (-1) + 0 \cdot 1 + 2 \cdot 0 + (-1) \cdot 1 = -2; \\
u_{3} \cdot v_{2} = 1 \cdot 2 + 0 \cdot 1 + 2 \cdot (-3) + (-1) \cdot 1 = -5; \\
v_{2} \cdot v_{2} = 2 \cdot 2 + 1 \cdot 1 + (-3) \cdot (-3) + 1 \cdot 1 = 15.
\end{array} u 3 ⋅ v 1 = 1 ⋅ ( − 1 ) + 0 ⋅ 1 + 2 ⋅ 0 + ( − 1 ) ⋅ 1 = − 2 ; u 3 ⋅ v 2 = 1 ⋅ 2 + 0 ⋅ 1 + 2 ⋅ ( − 3 ) + ( − 1 ) ⋅ 1 = − 5 ; v 2 ⋅ v 2 = 2 ⋅ 2 + 1 ⋅ 1 + ( − 3 ) ⋅ ( − 3 ) + 1 ⋅ 1 = 15.
We get v 3 = u 3 − u 3 ⋅ v 1 v 1 ⋅ v 1 v 1 − u 3 ⋅ v 2 v 2 ⋅ v 2 v 2 = ( 1 , 0 , 2 , − 1 ) − ( − 2 ) 3 ( − 1 , 1 , 0 , 1 ) − ( − 5 ) 15 ( 2 , 1 , − 3 , 1 ) = v_{3} = u_{3} - \frac{u_{3} \cdot v_{1}}{v_{1} \cdot v_{1}} v_{1} - \frac{u_{3} \cdot v_{2}}{v_{2} \cdot v_{2}} v_{2} = (1, 0, 2, -1) - \frac{(-2)}{3} (-1, 1, 0, 1) - \frac{(-5)}{15} (2, 1, -3, 1) = v 3 = u 3 − v 1 ⋅ v 1 u 3 ⋅ v 1 v 1 − v 2 ⋅ v 2 u 3 ⋅ v 2 v 2 = ( 1 , 0 , 2 , − 1 ) − 3 ( − 2 ) ( − 1 , 1 , 0 , 1 ) − 15 ( − 5 ) ( 2 , 1 , − 3 , 1 ) =
= ( 1 , 0 , 2 , − 1 ) + 2 3 ( − 1 , 1 , 0 , 1 ) + 1 3 ( 2 , 1 , − 3 , 1 ) = ( 1 , 1 , 1 , 0 ) , hence, v 3 = ( 1 , 1 , 1 , 0 ) . = (1, 0, 2, -1) + \frac{2}{3} (-1, 1, 0, 1) + \frac{1}{3} (2, 1, -3, 1) = (1, 1, 1, 0), \text{ hence, } v_{3} = (1, 1, 1, 0). = ( 1 , 0 , 2 , − 1 ) + 3 2 ( − 1 , 1 , 0 , 1 ) + 3 1 ( 2 , 1 , − 3 , 1 ) = ( 1 , 1 , 1 , 0 ) , hence, v 3 = ( 1 , 1 , 1 , 0 ) .
So we get an orthogonal basis v 1 = ( − 1 , 1 , 0 , 1 ) v_{1} = (-1,1,0,1) v 1 = ( − 1 , 1 , 0 , 1 ) , v 2 = ( 2 , 1 , − 3 , 1 ) v_{2} = (2,1, -3,1) v 2 = ( 2 , 1 , − 3 , 1 ) , v 3 = ( 1 , 1 , 1 , 0 ) v_{3} = (1,1,1,0) v 3 = ( 1 , 1 , 1 , 0 ) .
Normalizing the vectors:
∥ v 1 ∥ = v 1 ⋅ v 1 = 3 ; e 1 = v 1 ∥ v 1 ∥ = 1 3 ( − 1 , 1 , 0 , 1 ) . ∥ v 2 ∥ = v 2 ⋅ v 2 = 15 ; e 2 = v 2 ∥ v 2 ∥ = 1 15 ( 2 , 1 , − 3 , 1 ) . ∥ v 3 ∥ = v 3 ⋅ v 3 = 1 ⋅ 1 + 1 ⋅ 1 + 1 ⋅ 1 + 0 ⋅ 0 = 3 ; e 3 = v 3 ∥ v 3 ∥ = 1 3 ( 1 , 1 , 1 , 0 ) . \begin{array}{l}
\|v_{1}\| = \sqrt{v_{1} \cdot v_{1}} = \sqrt{3}; \quad e_{1} = \frac{v_{1}}{\|v_{1}\|} = \frac{1}{\sqrt{3}} (-1, 1, 0, 1). \\
\|v_{2}\| = \sqrt{v_{2} \cdot v_{2}} = \sqrt{15}; \quad e_{2} = \frac{v_{2}}{\|v_{2}\|} = \frac{1}{\sqrt{15}} (2, 1, -3, 1). \\
\|v_{3}\| = \sqrt{v_{3} \cdot v_{3}} = \sqrt{1 \cdot 1 + 1 \cdot 1 + 1 \cdot 1 + 0 \cdot 0} = \sqrt{3}; \quad e_{3} = \frac{v_{3}}{\|v_{3}\|} = \frac{1}{\sqrt{3}} (1, 1, 1, 0).
\end{array} ∥ v 1 ∥ = v 1 ⋅ v 1 = 3 ; e 1 = ∥ v 1 ∥ v 1 = 3 1 ( − 1 , 1 , 0 , 1 ) . ∥ v 2 ∥ = v 2 ⋅ v 2 = 15 ; e 2 = ∥ v 2 ∥ v 2 = 15 1 ( 2 , 1 , − 3 , 1 ) . ∥ v 3 ∥ = v 3 ⋅ v 3 = 1 ⋅ 1 + 1 ⋅ 1 + 1 ⋅ 1 + 0 ⋅ 0 = 3 ; e 3 = ∥ v 3 ∥ v 3 = 3 1 ( 1 , 1 , 1 , 0 ) .
Answer: 1 3 ( − 1 , 1 , 0 , 1 ) ; 1 15 ( 2 , 1 , − 3 , 1 ) ⋅ 1 3 ( 1 , 1 , 1 , 0 ) \frac{1}{\sqrt{3}} (-1, 1, 0, 1); \frac{1}{\sqrt{15}} (2, 1, -3, 1) \cdot \frac{1}{\sqrt{3}} (1, 1, 1, 0) 3 1 ( − 1 , 1 , 0 , 1 ) ; 15 1 ( 2 , 1 , − 3 , 1 ) ⋅ 3 1 ( 1 , 1 , 1 , 0 ) .
References:
1. Hazewinkel, Michel (2001) Orthogonalization. Encyclopedia of Mathematics, Springer ISBN 978-1-55608-010-4
https://www.encyclopediaofmath.org/index.php/Orthogonalization
2. E W. Cheney, D. Ronald (2009) Linear Algebra: Theory and Applications, Sudbury Massachusetts, 740 p. ISBN 978-0-7637-5020-6.
https://books.google.com/books?id=Gg3Uj1GkHK8C&pg=PA544&redir_esc=y#v=onepage&q&f=false
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