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In each exercise, \(\lambda\) is an eigenvalue of the given matrix \(A\). Determine an eigenvector corresponding to \(\lambda\). $$ A=\left[\begin{array}{rrr} 1 & -7 & 3 \\ -1 & -1 & 1 \\ 4 & -4 & 0 \end{array}\right], \quad \lambda=-4 $$

Short Answer

Expert verified
Question: Find the eigenvector associated with the eigenvalue λ = -4 for the matrix A = \(\begin{bmatrix} 1 & -7 & 3 \\ -1 & -1 & 1 \\ 4 & -4 & 0 \end{bmatrix}\). Answer: The eigenvector corresponding to the eigenvalue λ = -4 is \(v = \begin{bmatrix} -7 \\ -5 \\ 15 \end{bmatrix}\).

Step by step solution

01

Find the matrix (A - λI)

To find the matrix \((A - \lambda I)\), we subtract the eigenvalue \(\lambda\) multiplied by the identity matrix \(I\) from the given matrix \(A\): $$ (A - \lambda I) = \left[\begin{array}{rrr} 1 & -7 & 3 \\\ -1 & -1 & 1 \\\ 4 & -4 & 0 \end{array}\right] - (-4) \left[\begin{array}{rrr} 1 & 0 & 0 \\\ 0 & 1 & 0 \\\ 0 & 0 & 1 \end{array}\right] = \left[\begin{array}{rrr} 1+4 & -7 & 3 \\\ -1 & -1+4 & 1 \\\ 4 & -4 & 0+4 \end{array}\right] $$ $$ (A - \lambda I) = \left[\begin{array}{rrr} 5 & -7 & 3 \\\ -1 & 3 & 1 \\\ 4 & -4 & 4 \end{array}\right] $$
02

Solve the linear system

Now, we need to solve the linear system \((A - \lambda I)v = 0\) for the vector \(v\). We can represent the system in the augmented matrix form and reduce it to row echelon form: $$ \left[\begin{array}{rrr|r} 5 & -7 & 3 & 0 \\\ -1 & 3 & 1 & 0 \\\ 4 & -4 & 4 & 0 \end{array}\right] \rightarrow \left[\begin{array}{rrr|r} 1 & -7/5 & 3/5 & 0 \\\ 0 & 1 & 1/3 & 0 \\\ 0 & 0 & 0 & 0 \end{array}\right] $$ The system of equations represented by the row echelon form is: $$ x_1 - \frac{7}{5}x_2 + \frac{3}{5}x_3 = 0 \\ x_2 + \frac{1}{3}x_3 = 0 $$ Now, let \(x_3 = t\), where t is a free parameter. The second equation gives us: $$ x_2 = -\frac{1}{3}t $$ Substituting this into the first equation, we get: $$ x_1 - \frac{7}{5}(-\frac{1}{3}t) + \frac{3}{5}t = 0 \\ x_1 + \frac{7}{15}t = 0 $$ So, \(x_1 = -\frac{7}{15}t\). This gives us the eigenvector \(v\) in the form: $$ v = \left[\begin{array}{r} -\frac{7}{15}t \\\ -\frac{1}{3}t\\\ t \end{array}\right] = t \left[\begin{array}{r} -\frac{7}{15}\\\ -\frac{1}{3}\\\ 1 \end{array}\right] $$ Since eigenvectors can be multiplied by a constant without changing their significance, we can choose any non-zero value of \(t\). Here, we choose \(t = 15\) to avoid fractions: $$ v = 15 \left[\begin{array}{r} -\frac{7}{15}\\\ -\frac{1}{3}\\\ 1 \end{array}\right] = \left[\begin{array}{r} -7\\\ -5\\\ 15 \end{array}\right] $$ So, the eigenvector corresponding to the eigenvalue \(\lambda = -4\) is: $$ v = \left[\begin{array}{r} -7 \\\ -5 \\\ 15 \end{array}\right] $$

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Key Concepts

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

Eigenvalues
Eigenvalues are special numbers associated with a square matrix. They tell us about the scaling factor of eigenvectors when a matrix acts on them. In mathematical terms, if a matrix \( A \) has an eigenvalue \( \lambda \), it means there exists a non-zero vector \( v \) such that
  • \( Av = \lambda v \)
This equation shows that the action of \( A \) on \( v \) results in scaling the vector by \( \lambda \).
Finding eigenvalues typically involves solving the characteristic equation, which is derived from the determinant:
  • \( \det(A - \lambda I) = 0 \)
Here, \( I \) is the identity matrix of the same size as \( A \). Eigenvalues play a crucial role in many applications, such as stability analysis and quantum mechanics.
Matrix Algebra
Matrix algebra involves operations with matrices, including addition, multiplication, and finding inverses. When dealing with eigenvalues and eigenvectors, we often manipulate matrices to simplify calculations.
Some key concepts include:
  • Matrix Addition: Add corresponding elements of matrices.
  • Matrix Multiplication: Multiply rows by columns (the number of columns in the first matrix must match the number of rows in the second).
  • Identity Matrix: A matrix with ones on the diagonal and zeroes elsewhere, often denoted by \( I \).
In the exercise, we used matrix subtraction to find \( A - \lambda I \), an essential part of determining eigenvectors.
Understanding these basics is crucial for solving linear systems and exploring deeper mathematical theories.
Linear Systems
Solving linear systems involves finding solutions for variables within a set of linear equations. In the context of eigenvalues and eigenvectors, we express the problem \( (A - \lambda I)v = 0 \). This linear system represents a homogeneous equation since it equals zero.
To find eigenvectors, we solve this system, often involving:
  • Formulating the system as an augmented matrix
  • Applying row operations to simplify the system
A solution exists when variables align in a way that satisfies all the system's equations. For eigenvectors, we often find a free parameter, resulting in infinitely many solutions, or scaling factors.
Row Echelon Form
Row Echelon Form (REF) is a simplified version of a matrix that makes solving linear systems straightforward. It involves arranging the matrix so that each leading (non-zero) entry is to the right of the leading entry in the previous row, and zero rows are at the bottom.
Here's how we achieve REF:
  • Pivoting: Use leading entries (or pivots) to eliminate elements in lower rows.
  • Row Swap: Adjust row order for optimal zero placement.
  • Row Multiplication: Multiply or divide rows by non-zero scalars.
In the exercise, we transformed the matrix into REF to make the relationship between variables clearer. This helped isolate free variables and solve for the eigenvector. Understanding REF is foundational for deep insights into matrix solutions and linear algebra techniques.

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Most popular questions from this chapter

The flow system shown in the figure is activated at time \(t=0 .\) Let \(Q_{i}(t)\) denote the amount of solute present in the \(i\) th tank at time \(t\). For simplicity, we assume all the flow rates are a constant \(10 \mathrm{gal} / \mathrm{min}\). It follows that volume of solution in each tank remains constant; we assume the volume to be \(1000 \mathrm{gal}\).The flow system shown in the figure is activated at time \(t=0 .\) Let \(Q_{i}(t)\) denote the amount of solute present in the \(i\) th tank at time \(t\). For simplicity, we assume all the flow rates are a constant \(10 \mathrm{gal} / \mathrm{min}\). It follows that volume of solution in each tank remains constant; we assume the volume to be \(1000 \mathrm{gal}\).(b) Solve the initial value problem defined by the given inflow concentrations and initial conditions. Also, determine \(\lim _{t \rightarrow \infty} \mathbf{Q}(t)\). (c) In Exercises 33 and 34 , the inflow concentrations are constant. Compute the equilibrium solution of the system in part (a). What is the physical significance of this equilibrium solution? (d) In Exercise 35 , the system in part (a) is not autonomous. Graph \(Q_{1}(t)\) and \(Q_{2}(t)\). Determine the maximum amounts of solute in each tank.\(c_{1}=0.5 \mathrm{lb} / \mathrm{gal}, \quad c_{2}=0, \quad Q_{1}(0)=Q_{2}(0)=0\)

In each exercise, assume that a numerical solution is desired on the interval \(t_{0} \leq t \leq t_{0}+T\), using a uniform step size \(h\). (a) As in equation (8), write the Euler's method algorithm in explicit form for the given initial value problem. Specify the starting values \(t_{0}\) and \(\mathbf{y}_{0}\). (b) Give a formula for the \(k\) th \(t\)-value, \(t_{k}\). What is the range of the index \(k\) if we choose \(h=0.01\) ? (c) Use a calculator to carry out two steps of Euler's method, finding \(\mathbf{y}_{1}\) and \(\mathbf{y}_{2}\). Use a step size of \(h=0.01\) for the given initial value problem. Hand calculations such as these are used to check the coding of a numerical algorithm.\(\mathbf{y}^{\prime}=\left[\begin{array}{cc}1 & t \\ 2+t & 2\end{array}\right] \mathbf{y}+\left[\begin{array}{l}1 \\\ t\end{array}\right], \quad \mathbf{y}(1)=\left[\begin{array}{l}2 \\\ 1\end{array}\right], \quad 1 \leq t \leq 1.5\)

Consider the \(R L\) network shown in the figure. Assume that the loop currents \(I_{1}\) and \(I_{2}\) are zero until a voltage source \(V_{S}(t)\), having the polarity shown, is turned on at time \(t=0 .\) Applying Kirchhoff's voltage law to each loop, we obtain the equations $$ \begin{aligned} -V_{S}(t)+L_{1} \frac{d I_{1}}{d t}+R_{1} I_{1}+R_{3}\left(I_{1}-I_{2}\right) &=0 \\ R_{3}\left(I_{2}-I_{1}\right)+R_{2} I_{2}+L_{2} \frac{d I_{2}}{d t} &=0 \end{aligned} $$ (a) Formulate the initial value problem for the loop currents, \(\left[\begin{array}{l}I_{1}(t) \\ I_{2}(t)\end{array}\right]\), assuming that $$ L_{1}=L_{2}=0.5 H, \quad R_{1}=R_{2}=1 k \Omega, \quad \text { and } \quad R_{3}=2 k \Omega . $$ (b) Determine a fundamental matrix for the associated linear homogeneous system. (c) Use the method of variation of parameters to solve the initial value problem for the case where \(V_{S}(t)=1\) for \(t>0\).

Determine all values \(t\) such that \(A(t)\) is invertible and, for those \(t\)-values, find \(A^{-1}(t)\) $$ \text { 3. } A(t)=\left[\begin{array}{lr} \sin t & -\cos t \\ \sin t & \cos t \end{array}\right] $$

Verify, for any values \(c_{1}\) and \(c_{2}\), that the functions \(y_{1}(t)\) and \(y_{2}(t)\) satisfy the given system of linear differential equations. $$ \begin{array}{ll} y_{1}^{\prime}=4 y_{1}+y_{2}, & y_{1}(t)=c_{1} e^{5 t}+c_{2} e^{3 t} \\ y_{2}^{\prime}=y_{1}+4 y_{2}, & y_{2}(t)=c_{1} e^{5 t}-c_{2} e^{3 t} \end{array} $$

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