Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Find the eigenvalues and eigenvectors of the following matrices.\(\left(\begin{array}{ll}1 & 3 \\ 2 & 2\end{array}\right)\)

Short Answer

Expert verified
Eigenvalues: \(4, -1\). Eigenvectors: \[ \begin{pmatrix} 1 \ 1 \end{pmatrix} \] for \(\lambda = 4\) and \[ \begin{pmatrix} -3 \ 2 \end{pmatrix} \] for \(\lambda = -1\).

Step by step solution

01

- Write the characteristic equation

To find the eigenvalues, set up the characteristic equation by finding the determinant of the matrix \(A - \lambda I\), where \(A\) is your matrix and \(I\) is the identity matrix:\[ A = \left(\begin{array}{ll}1 & 3 \ 2 & 2\end{array}\right) \] Subtract \(\lambda\) times the identity matrix \(I\) from \(A\) and set the determinant to zero:\[ \left| \begin{array}{cc} 1 - \lambda & 3 \ 2 & 2 - \lambda \end{array} \right| = 0 \]
02

- Solve the determinant

Calculate the determinant of the matrix \[ \left(\begin{array}{cc} 1 - \lambda & 3 \ 2 & 2 - \lambda \end{array}\right) \]: Using the formula for the determinant of a 2x2 matrix, \(det(A) = a*d - b*c\):\[ (1-\lambda)(2-\lambda) - (3)(2) = 0 \] Simplify the above equation:\[ (1-\lambda)(2-\lambda) - 6 = 0 \] \[ \lambda^2 - 3\lambda - 4 = 0 \]
03

- Find the eigenvalues

Solve the quadratic equation to find the eigenvalues \(\lambda\):\[ \lambda^2 - 3\lambda - 4 = 0 \] Factoring the quadratic equation:\[ (\lambda - 4)(\lambda + 1) = 0 \] The solutions to the equation are:\[ \lambda = 4, \lambda = -1 \]
04

- Find the eigenvectors for \( \lambda = 4 \)

Substitute \(\lambda = 4\) back into the equation \(A - \lambda I = 0\) to find the eigenvector. Set up the matrix:\[ \left(\begin{array}{cc} 1-4 & 3 \ 2 & 2-4 \end{array}\right) = \left(\begin{array}{cc} -3 & 3 \ 2 & -2 \end{array}\right) \] Find the vector \(v\) that satisfies the equation \[ \left(\begin{array}{cc} -3 & 3 \ 2 & -2 \end{array}\right) \left( \begin{array}{c} x \ y \end{array} \right) = \left(\begin{array}{c} 0 \ 0 \end{array} \right) \] Simplifying the system, we get \-3x + 3y = 0\ and \2x - 2y = 0\, which simplifies to \x = y\. So, an eigenvector corresponding to \(\lambda = 4\) is \[ \begin{pmatrix} 1 \ 1 \end{pmatrix} \] (or any scalar multiple).
05

- Find the eigenvectors for \( \lambda = -1 \)

Substitute \(\lambda = -1\) back into the equation \(A - \lambda I = 0\) to find the eigenvector. Set up the matrix:\[ \left(\begin{array}{cc} 1-(-1) & 3 \ 2 & 2-(-1) \end{array}\right) = \left(\begin{array}{cc} 2 & 3 \ 2 & 3 \end{array}\right) \] Find the vector \(v\) that satisfies the equation \[ \left(\begin{array}{cc} 2 & 3 \ 2 & 3 \end{array}\right) \left( \begin{array}{c} x \ y \end{array} \right) = \left(\begin{array}{c} 0 \ 0 \end{array} \right) \] Simplifying the system, we get \2x + 3y = 0\ and \2x + 3y = 0\, which simplifies to \x = -\frac{3}{2}y\. So, an eigenvector corresponding to \(\lambda = -1\) is \[ \begin{pmatrix} -3 \ 2 \end{pmatrix} \] (or any scalar multiple).

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Characteristic Equation
The characteristic equation is crucial when finding eigenvalues and eigenvectors of a matrix. It involves setting up an equation derived from the matrix, which helps identify the unique values associated with the matrix.
To start, you need the given matrix, let's call it \(A\). For example, if \(A = \begin{pmatrix}1 & 3 \ 2 & 2\thumb\right)\), we aim to find eigenvalues by solving the characteristic equation. First, we subtract \(λ\) times the identity matrix \(I\) from our matrix \(A\). This becomes \(A - λI\). The identity matrix \(I\) for a 2x2 matrix looks like this: \(\begin{pmatrix}1 & 0 \ 0 & 1\face_with_monocle \right)\).
Now, subtracting \(λI\) from \(A\) gives us \(\begin{pmatrix}1-λ & 3 \ 2 & 2-λ\right)\). The characteristic equation is then formed by setting the determinant of \(A - λI\) to zero: \(det(A - λI) = 0\). This forms the quadratic equation we solve to find eigenvalues.
Determinant
The determinant is a scalar value that can be computed from the elements of a square matrix. It provides important properties regarding the matrix, including whether it is invertible.
For a 2x2 matrix \(\begin{pmatrix}a & b \ c & d\right)\), the determinant is calculated as \(det(A) = ad - bc\). This helps in finding the characteristic equation by setting \(det(A - λI) = 0\).
Let's take our example, \(A = \begin{pmatrix}1 & 3 \ 2 & 2\right)\). After subtracting \(λI\), we have \(A - λI = \begin{pmatrix}1-λ & 3 \ 2 & 2-λ\right)\). The determinant is \((1-λ)(2-λ) - (3)(2) = λ^2 - 3λ - 4 = 0\). This algebraic expression, when solved, gives us the eigenvalues.
Eigenvalues
Eigenvalues are found from the characteristic equation and are key to understanding a matrix's properties. They are the values of \(λ\) for which \(Av = λv\), where \(v\) is an eigenvector.
From our quadratic equation \(λ^2 - 3λ - 4 = 0\), solving this gives the eigenvalues. Factoring the equation, we get \((λ - 4)(λ + 1) = 0\). Therefore, the eigenvalues are \(λ = 4\) and \(λ = -1\).
These values are critical as they indicate particular scaling factors in the transformation described by the matrix.
Eigenvectors
Eigenvectors are non-zero vectors that change at most by a scalar factor when that linear transformation is applied. They correspond to eigenvalues and provide insights into the transformation represented by the matrix.
For \(λ = 4\), substitute back into \(A - λI = 0\): \(\begin{pmatrix}1-4 & 3 \ 2 & 2-4\right) = \begin{pmatrix}-3 & 3 \ 2 & -2\right)\). Solving \((-3x + 3y = 0\) and \(2x - 2y = 0)\), we find \(x = y\). Thus, an eigenvector is \(v = \begin{pmatrix}1 \ 1\right)\).
For \(λ = -1\), substitute back: \(\begin{pmatrix}1-(-1) & 3 \ 2 & 2-(-1)\right) = \begin{pmatrix}2 & 3 \ 2 & 3\right)\). Solving \((2x + 3y = 0\)), we get \(x = -3/2y\). Hence, an eigenvector is \(v = \begin{pmatrix}-3 \ 2\right)\). Eigenvectors offer direction and scale to the transformation, making them vital in data analysis, computer graphics, and more.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

(a) If a body is rotating about a fixed axis, then its angular momentum \(L\) and its angular velocity \(\boldsymbol{o}\) are parallel vectors and \(\mathrm{L}=\mathrm{le} \mathrm{s}\), where \(I\) is the (scalar) moment of inertia of the body about the axis. However, in general, \(L\) and \(\omega\) are not parallel and \(I\) in the equation must be a second-order tensor; let us call it I. Find I in dyadic form in the following way: For simplicity, first consider a point mass \(m\) at the point \(r\). The angular momentum of \(m\) about the origin is by definition \(m r \times v\), where \(v\) is the linear velocity.From Chapter \(6, v=\omega \times r .\) Write out the triple vector product for \(L\) and from it write each component of \(\mathrm{L}\) in terms of the three components of 6 . Write your results in matrix form and in dyadic form $$ \mathbf{L}=\mathbf{I} \cdot \mathbf{\omega}=\left(\mathrm{ii} l_{x x}+\mathrm{ij} l_{x y}+\cdots\right)+\omega $$ You should have $$ I_{x z}=m\left(y^{2}+z^{2}\right), \quad I_{x y}=-m x y, \quad \text { etc. } $$ For a set of masses \(m_{i}\) or an extended body, replace the cxpressions for \(I_{z x+}, \operatorname{ctc}_{4}\), by the corresponding sums or integrals: $$ \begin{aligned} &I_{x x}=\sum m_{i}\left(y_{i}^{2}+z_{i}^{2}\right) \quad \text { or } \quad \int\left(y^{2}+z^{2}\right) d m_{4} \\ &I_{x y}=-\sum m_{j} x_{i} y_{i} \quad \text { or }-\int x y d m_{4} \quad \text { etc. } \end{aligned} $$ (b) Show that 1 is a second-order (Cartesian) tensor by expressing its components relative to a rotated system \(\left[I_{s^{\prime} x^{\prime}}=m\left(y^{2}+z^{\prime 2}\right)\right.\), etc. \(]\) in terms of \(x, y, z\) using \((11.7)\) or \((11.11)\), and hence in terms of \(I_{x \pi}\), etc., to show that I obeys the transformation equations \((11,13)\). (c) Show that if \(\mathrm{n}\) is a unit vector, the expression \(\mathbf{n}+\mathbf{1} \cdot \mathbf{n}\) gives the moment of inertia about an axis through the origin parallel to n. Hint: Consider I rotated to a system in which one of the axes is along \(n\). (d) Observe that the I matrix is symmetric and recall that a symmetric matrix may be diagonalized by a rotation of axes. The eigenvalues of the I matrix are called the principal moments of inertia. Show by part (c) that they are moments of inertia abour the new axes \(\left(x^{\prime}, y^{\prime}, z^{\prime}\right)\) relative to which \(\mathbf{I}\) is diagonal. These new axes are called the principal axes of incrtia. For the mass distribution consisting of point masses \(m\) at \((1,1,1)\) and \((1,1,-1)\), find the nine components of 1, and find the principal moments of inertia and the principal axes.

Find the inverse of the transformation $$ \begin{aligned} &x^{\prime}=2 x-3 y \\ &y^{\prime}=x+y \end{aligned} $$ that is, find \(x, y\) in terms of \(x^{\prime}, y^{\prime}\). (Hint : Use matrices.) Is the transformation orthogonal?

Let each of the following matrices \(M\) describe a deformation of the \((x, y)\) plane. For each given \(M\) find: the eigenvalues and eigenvectors of the transformation, the matrix \(C\) which diagonalizes \(M\) and specifies the rotation to new axes \(\left(x^{\prime}, y^{\prime}\right)\) along the eigenvectors, and the matrix \(D\) which gives the deformation relative to the new axes. Describe the deformation relative to the new axes.\(\left(\begin{array}{rr}6 & -2 \\ -2 & 3\end{array}\right)\)

(a) Show that the product of two symmetric matrices is symmetric if and only if they commute. (b) When is the product of two Hermitian matrices a Hermitian matrix?

The trace of a matrix is the sum of the elements on the main diagonal. Show that the trace is not changed by cyclic permutation of the matrices, that is, \(\operatorname{Tr}(A B C)=\operatorname{Tr}(C A B)=\) Tr \((B C A)\). [Caution: \(\operatorname{Tr}(A B C) \neq \operatorname{Tr}(A C B)\) in general. ]

See all solutions

Recommended explanations on Combined Science Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free