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If \(b \neq 0,\) orthogonally diagonalize \(A=\left[\begin{array}{ll}a & b \\ b & a\end{array}\right]\)

Short Answer

Expert verified
The matrix is orthogonally diagonalized by matrix \( P \) and diagonal matrix \( D \).

Step by step solution

01

Find Eigenvalues

To diagonalize the matrix, start by finding its eigenvalues. The characteristic equation is given by \( \det(A - \lambda I) = 0 \), where \( I \) is the identity matrix. Calculating, we have:\[\det \left( \begin{array}{cc} a - \lambda & b \ b & a - \lambda \end{array} \right) = (a - \lambda)^2 - b^2 = 0\]This simplifies to \( (a - \lambda)^2 = b^2 \), leading to \( a - \lambda = \pm b \). Thus, the eigenvalues are \( \lambda_1 = a + b \) and \( \lambda_2 = a - b \).
02

Find Eigenvectors

For each eigenvalue, find the corresponding eigenvector by solving \( (A - \lambda I)\mathbf{v} = 0 \).**For \( \lambda_1 = a + b \):**\[(A - (a + b)I) = \begin{bmatrix} -b & b \ b & -b \end{bmatrix}\]A possible eigenvector is \( \mathbf{v_1} = \begin{bmatrix} 1 \ 1 \end{bmatrix} \).**For \( \lambda_2 = a - b \):**\[(A - (a - b)I) = \begin{bmatrix} b & b \ b & b \end{bmatrix}\]A possible eigenvector is \( \mathbf{v_2} = \begin{bmatrix} 1 \ -1 \end{bmatrix} \).
03

Normalize Eigenvectors

Orthogonalize the eigenvectors by normalizing them:- For \( \mathbf{v_1} = \begin{bmatrix} 1 \ 1 \end{bmatrix} \), normalize as follows: \[ \mathbf{u_1} = \frac{1}{\sqrt{2}} \begin{bmatrix} 1 \ 1 \end{bmatrix} \]- For \( \mathbf{v_2} = \begin{bmatrix} 1 \ -1 \end{bmatrix} \), normalize as follows: \[ \mathbf{u_2} = \frac{1}{\sqrt{2}} \begin{bmatrix} 1 \ -1 \end{bmatrix} \]
04

Construct Orthogonal Matrix P and Diagonal Matrix D

Using the normalized eigenvectors, construct matrix \( P \) and diagonal matrix \( D \). \[ P = \begin{bmatrix} \mathbf{u_1} & \mathbf{u_2} \end{bmatrix} = \begin{bmatrix} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \ \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \end{bmatrix} \]\( D \) will then be:\[ D = \begin{bmatrix} \lambda_1 & 0 \ 0 & \lambda_2 \end{bmatrix} = \begin{bmatrix} a+b & 0 \ 0 & a-b \end{bmatrix} \]
05

Verify Orthogonal Diagonalization

Ensure \( A = PDP^T \):- Compute \( P^T = \begin{bmatrix} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \ \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \end{bmatrix} \)- Verify that applying \( PDP^T \) gives back matrix \( A \): \[ PDP^T = \begin{bmatrix} a & b \ b & a \end{bmatrix} \]The matrix is thus orthogonally diagonalized correctly.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Eigenvalues and Eigenvectors
In the matrix diagonalization process, a key step is finding eigenvalues and their corresponding eigenvectors. These elements are essential in transforming a matrix into its simpler form, allowing easier analysis and computations. To start, eigenvalues are found by solving the characteristic equation, usually taking the form of \( \det(A - \lambda I) = 0 \). Here, \( A \) is the given matrix, \( \lambda \) represents the unknown eigenvalues, and \( I \) is the identity matrix. For the matrix in question:
  • The characteristic equation simplifies to \( (a - \lambda)^2 = b^2 \), resulting from the determinant of the matrix \( A - \lambda I \).
  • This leads to the discovery of two eigenvalues: \( \lambda_1 = a + b \) and \( \lambda_2 = a - b \).
Eigenvectors are vectors that indicate the direction of "stretching" without changing direction, when a linear transformation is applied. Once eigenvalues are found, eigenvectors can be calculated by solving \( (A - \lambda I) \mathbf{v} = 0 \), yielding vectors for each eigenvalue:
  • For \( \lambda_1 = a + b \), a valid eigenvector is \( \mathbf{v_1} = \begin{bmatrix} 1 \ 1 \end{bmatrix} \).
  • For \( \lambda_2 = a - b \), a valid eigenvector is \( \mathbf{v_2} = \begin{bmatrix} 1 \ -1 \end{bmatrix} \).
Orthogonalization
Orthogonalization is the process of converting a set of vectors into mutually orthogonal vectors, meaning they are perpendicular to each other in space. This is a critical step in orthogonal diagonalization, ensuring the resulting matrix \( P \) is an orthogonal matrix.

For each eigenvector obtained, normalizing is performed to achieve this:
  • Normalization involves adjusting the length of a vector to 1 to facilitate orthogonality. This is done by dividing each component of the vector by its length.
  • For example, for \( \mathbf{v_1} = \begin{bmatrix} 1 \ 1 \end{bmatrix} \), the normalized orthogonal eigenvector is \( \mathbf{u_1} = \frac{1}{\sqrt{2}} \begin{bmatrix} 1 \ 1 \end{bmatrix} \).
  • Similarly, \( \mathbf{v_2} = \begin{bmatrix} 1 \ -1 \end{bmatrix} \) normalizes to \( \mathbf{u_2} = \frac{1}{\sqrt{2}} \begin{bmatrix} 1 \ -1 \end{bmatrix} \).
Upon obtaining the orthogonal eigenvectors, these help in forming matrix \( P \), a pillar in the orthogonalization process.
Characteristic Equation
The characteristic equation is foundational to matrix diagonalization. It is employed to determine eigenvalues of a matrix. The equation is derived by setting the determinant of \( A - \lambda I \) to zero, where \( \lambda \) represents the eigenvalue.

The given problem provides:
  • Matrix \( A = \begin{bmatrix} a & b \ b & a \end{bmatrix} \), which is an example of a 2x2 symmetric matrix.
  • Setting its determinant \( \det(A - \lambda I) = (a - \lambda)^2 - b^2 = 0 \) leads to solving \( (a - \lambda)^2 = b^2 \).
  • This equation simplifies into the direct eigenvalues \( \lambda_1 = a + b \) and \( \lambda_2 = a - b \), crucial for the subsequent steps.
Understanding this step solidifies the basis for finding both eigenvalues and the resulting eigenvectors, opening the door to matrix transformations and other linear algebra applications.

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Most popular questions from this chapter

Find the orthogonal projection of v onto the subspace \(W\) spanned by the vectors \(\mathbf{u}_{\mathbf{r}}\) (You may assume that the vectors \(\mathbf{u}_{i}\) are orthogonal. ) $$\mathbf{v}=\left[\begin{array}{r} 7 \\ -4 \end{array}\right], \mathbf{u}_{1}=\left[\begin{array}{l} 1 \\ 1 \end{array}\right]$$

Let \(A\) be a real \(2 \times 2\) matrix with complex eigenvalues \(\lambda=a \pm b i\) such that \(b \neq 0\) and \(|\lambda|=1 .\) Prove that every trajectory of the dynamical system \(\mathbf{x}_{k+1}=A \mathbf{x}_{k}\) lies on an ellipse. [Hint: Theorem 4.43 shows that if \(\mathbf{v}\) is an eigenvector corresponding to \(\lambda=a-b i\), then the matrix \(P=[\operatorname{Re} \mathbf{v} \quad \operatorname{Im} \mathbf{v}]\) is invertible and \(A=P\left[\begin{array}{cc}a & -b \\ b & a\end{array}\right] P^{-1} .\) Set \(B=\left(P P^{T}\right)^{-1} .\) Show that the quadratic \(\mathbf{x}^{T} B \mathbf{x}=k\) defines an ellipse for all \(k>0\) and prove that if \(x \text { lies on this ellipse, so does } A x .]\)

Diagonalize the quadratic forms by finding an orthogonal matrix \(Q\) such that the change of variable \(\mathbf{x}=\) Qy transforms the given form into one with no cross-product terms. Give Q and the new quadratic form. $$2 x_{1}^{2}+5 x_{2}^{2}-4 x_{1} x_{2}$$

Sometimes the graph of a quadratic equation is a straight line, a pair of straight lines, or a single point. We refer to such a graph as a degenerate conic. It is also possible that the equation is not satisfied for any values of the variables, in which case there is no graph at all and we refer to the conic as an imaginary conic. Identify the conic with the given equation as either degenerate or imaginary and, where possible, sketch the graph. $$3 x^{2}+y^{2}=0$$

Let \(B\) be an invertible matrix. Show that \(A=B^{T} B\) is positive definite.

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