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find a fundamental matrix for the given system of equations. In each case also find the fundamental matrix \(\mathbf{\Phi}(t)\) satisfying \(\Phi(0)=\mathbf{1}\) $$ \mathbf{x}^{\prime}=\left(\begin{array}{rr}{-1} & {-4} \\ {1} & {-1}\end{array}\right) \mathbf{x} $$

Short Answer

Expert verified
Short Answer: The fundamental matrix for the given system of differential equations is: $$ \mathbf{\Phi}(t) = \frac{1}{4} e^{-3t} \begin{pmatrix} 4 & 2 \\ 2 & 1 \end{pmatrix} +\frac{3}{4} e^{t} \begin{pmatrix} 4 & -2 \\ -2 & 1 \end{pmatrix}. $$

Step by step solution

01

Find eigenvalues and eigenvectors of the matrix

To find the eigenvalues, we need to solve the following equation for \(\lambda\): \( \text{det}(A - \lambda I) = 0 \) where \(A = \begin{pmatrix} -1 & -4\\ 1& -1 \end{pmatrix}\) and \(I\) is the identity matrix. So, $$ \text{det}\begin{pmatrix} (-1-\lambda) & -4 \\ 1 & (-1-\lambda) \end{pmatrix} = ( -1 -\lambda)( -1 -\lambda) - (-4)(1)= \lambda^2 +2\lambda -3 = (\lambda+3)(\lambda-1) = 0 $$ Here, we find two eigenvalues: \(\lambda_1 = -3\) and \(\lambda_2 = 1\). Now, let's find the eigenvectors corresponding to each eigenvalue. For \(\lambda_1 = -3\), we have \((A-\lambda_1 I) \mathbf{v}_1 = 0\): $$ \begin{pmatrix} 2 & -4 \\ 1 & 2 \end{pmatrix} \mathbf{v}_1 = 0 $$ As row-2 of the matrix is a multiple of row-1, we can consider only the first row. From the first row, \(2v_{1,1}-4v_{1,2}=0 \Rightarrow v_{1,2}= \frac{1}{2}v_{1,1}\). Taking \(v_{1,1}=2,\) we have \(v_{1,2} = 1\), so \(\mathbf{v}_1 =\begin{pmatrix} 2 \\1 \end{pmatrix}\) For \(\lambda_2 = 1\), we have \((A-\lambda_2 I) \mathbf{v}_2 = 0\): $$ \begin{pmatrix} -2 & -4 \\ 1 & -2 \end{pmatrix} \mathbf{v}_2 = 0 $$ Again, the row-2 of the matrix is a multiple of row-1, so we can consider only the first row. From the first row, \(-2v_{2,1}-4v_{2,2}=0 \Rightarrow v_{2,1}=-2v_{2,2}\). Taking \(v_{2,2}=1,\) we have \(v_{2,1} = -2\), so \(\mathbf{v}_2 =\begin{pmatrix} -2 \\1 \end{pmatrix}\)
02

Form the matrix exponential

Now, we will form the matrix exponential using the eigenvalues and eigenvectors we found. We can express the matrix exponential as: $$ \mathbf{\Phi}(t) = c_1 e^{\lambda_1 t} \mathbf{v}_1 \mathbf{v}_1^T + c_2 e^{\lambda_2 t} \mathbf{v}_2 \mathbf{v}_2^T, $$ where \(c_1\) and \(c_2\) are constants. Now, we have to find the values of \(c_1\) and \(c_2\) such that \(\Phi(0)=\mathbf{1}\), where \(\mathbf{1}\) is the identity matrix.
03

Find \(c_1\) and \(c_2\)

By substituting \(t=0\) in the matrix exponential, we get: $$ \mathbf{1} = c_1 e^{0} \mathbf{v}_1 \mathbf{v}_1^T + c_2 e^{0} \mathbf{v}_2 \mathbf{v}_2^T =c_1 \begin{pmatrix} 2 \\1 \end{pmatrix}\begin{pmatrix} 2&1 \end{pmatrix} + c_2 \begin{pmatrix} -2 \\1 \end{pmatrix}\begin{pmatrix} -2&1 \end{pmatrix} $$ This gives us: $$ \mathbf{1} = c_1 \begin{pmatrix} 4 & 2 \\ 2 & 1 \end{pmatrix} + c_2 \begin{pmatrix} 4 & -2 \\ -2 & 1 \end{pmatrix}. $$ By equating the matrices, we obtain the following system of linear equations: $$ \begin{cases} 4c_1+4c_2=1 \\ 2c_1-2c_2=0 \\ 2c_1-2c_2=0 \\ c_1+c_2=1 \end{cases} $$ Solving this system, we find \(c_1=\frac{1}{4}\) and \(c_2=\frac{3}{4}\).
04

Determine the fundamental matrix \(\mathbf{\Phi}(t)\)

Finally, substitute the values of \(c_1\) and \(c_2\) into the matrix exponential to obtain the fundamental matrix \(\mathbf{\Phi}(t)\): $$ \mathbf{\Phi}(t) = \frac{1}{4} e^{-3t} \begin{pmatrix} 2 \\1 \end{pmatrix}\begin{pmatrix} 2&1 \end{pmatrix} + \frac{3}{4} e^{t} \begin{pmatrix} -2 \\1 \end{pmatrix}\begin{pmatrix} -2&1 \end{pmatrix} $$ Therefore, the fundamental matrix \(\mathbf{\Phi}(t)\) is: $$ \mathbf{\Phi}(t) = \frac{1}{4} e^{-3t} \begin{pmatrix} 4 & 2 \\ 2 & 1 \end{pmatrix} +\frac{3}{4} e^{t} \begin{pmatrix} 4 & -2 \\ -2 & 1 \end{pmatrix}. $$

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Key Concepts

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

Eigenvalues and Eigenvectors
The concepts of eigenvalues and eigenvectors are fundamental in understanding how matrices operate, especially within systems of differential equations.

An **eigenvalue** is a scalar that indicates how much the direction of an eigenvector is scaled during a matrix transformation. To find eigenvalues, solve the characteristic equation \( \text{det}(A - \lambda I) = 0 \), where \( A \) is your matrix and \( I \) is the identity matrix.

For example, given \( A = \begin{pmatrix} -1 & -4 \ 1 & -1 \end{pmatrix} \), solving the determinant equation helps locate two eigenvalues: \( \lambda_1 = -3 \) and \( \lambda_2 = 1 \).

An **eigenvector** is a non-zero vector that changes only in scale, not direction, when the matrix is applied. To find an eigenvector, insert each eigenvalue back into \( (A - \lambda I) \mathbf{v} = 0 \). For \( \lambda_1 = -3 \), an eigenvector is \( \mathbf{v}_1 = \begin{pmatrix} 2 \ 1 \end{pmatrix} \), and for \( \lambda_2 = 1 \), it's \( \mathbf{v}_2 = \begin{pmatrix} -2 \ 1 \end{pmatrix} \).

These vectors are key in forming the fundamental matrix that solves differential systems.
System of Differential Equations
A system of differential equations involves multiple equations that relate functions and their derivatives. These are widely used to model real-world problems like population growth or electrical circuits.

Consider the given system \( \mathbf{x}' = A\mathbf{x} \), where \( A = \begin{pmatrix} -1 & -4 \ 1 & -1 \end{pmatrix} \). Our goal is to find the solution matrix \( \mathbf{x}(t) \).

The solution begins with finding the eigenvalues and eigenvectors of matrix \( A \). These help construct the fundamental matrix, which in turn makes it possible to express the general solution of the system.

The fundamental matrix \( \mathbf{\Phi}(t) \) offers a way to convert a complex system into manageable computations. It describes the effect of the matrix on the state vector as it evolves over time.
  • First, calculate eigenvalues and eigenvectors of the matrix \( A \).
  • Use these to solve the homogeneous system and find \( \mathbf{\Phi}(t) \).
Solving such systems involves combining linear algebra concepts within the framework of calculus.
Matrix Exponential
The matrix exponential provides a powerful method to solve systems of linear differential equations. It is analogous to the exponential function for scalars.

To construct the matrix exponential \( \mathbf{\Phi}(t) \) for a matrix \( A \), employ the formula using eigenvalues and eigenvectors: \[ \mathbf{\Phi}(t) = c_1 e^{\lambda_1 t} \mathbf{v}_1 \mathbf{v}_1^T + c_2 e^{\lambda_2 t} \mathbf{v}_2 \mathbf{v}_2^T \] where \( c_1 \) and \( c_2 \) are constants determined by initial conditions.

The calculation starts with transforming the system by finding \( \lambda_1 \), \( \lambda_2 \), \( \mathbf{v}_1 \), and \( \mathbf{v}_2 \). The goal is to make \( \mathbf{\Phi}(t) \) satisfy \( \Phi(0) = \mathbf{1} \).
  • Identify eigenvalues and corresponding eigenvectors.
  • Insert these into the exponential format.
  • Apply the initial conditions to determine constants.
This results in the solution for the system's dynamic behavior over time, offering insights into its stability and responses.

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Most popular questions from this chapter

Find the solution of the given initial value problem. Draw the corresponding trajectory in \(x_{1} x_{2} x_{3}\) - space and also draw the graph of \(x_{1}\) versus \(t .\) $$ \mathbf{x}^{\prime}=\left(\begin{array}{rrr}{1} & {0} & {0} \\ {-4} & {1} & {0} \\ {3} & {6} & {2}\end{array}\right) \mathbf{x}, \quad \mathbf{x}(0)=\left(\begin{array}{r}{-1} \\ {2} \\ {-30}\end{array}\right) $$

Find all eigenvalues and eigenvectors of the given matrix. $$ \left(\begin{array}{cc}{1} & {i} \\ {-i} & {1}\end{array}\right) $$

The coefficient matrix contains a parameter \(\alpha\). In each of these problems: (a) Determine the eigervalues in terms of \(\alpha\). (b) Find the critical value or values of \(\alpha\) where the qualitative nature of the phase portrait for the system changes. (c) Draw a phase portrait for a value of \(\alpha\) slightly below, and for another value slightly above, each crititical value. $$ x^{\prime}=\left(\begin{array}{cc}{4} & {\alpha} \\ {8} & {-6}\end{array}\right) \mathbf{x} $$

Find all eigenvalues and eigenvectors of the given matrix. $$ \left(\begin{array}{rrr}{3} & {2} & {2} \\ {1} & {4} & {1} \\ {-2} & {-4} & {-1}\end{array}\right) $$

In this problem we indicate how to show that \(\mathbf{u}(t)\) and \(\mathbf{v}(t)\), as given by Eqs. (9), are linearly independent. Let \(r_{1}=\lambda+i \mu\) and \(\bar{r}_{1}=\lambda-i \mu\) be a pair of conjugate eigenvalues of the coefficient matrix \(\mathbf{A}\) of \(\mathrm{Fq}(1)\); let \(\xi^{(1)}=\mathbf{a}+i \mathbf{b}\) and \(\bar{\xi}^{(1)}=\mathbf{a}-i \mathbf{b}\) be the corresponding eigenvectors. Recall that it was stated in Section 7.3 that if \(r_{1} \neq \bar{r}_{1},\) then \(\boldsymbol{\xi}^{(1)}\) and \(\bar{\xi}^{(1)}\) are linearly independent. (a) First we show that a and b are linearly independent. Consider the equation \(c_{1} \mathrm{a}+\) \(c_{2} \mathrm{b}=0 .\) Express a and \(\mathrm{b}\) in terms of \(\xi^{(1)}\) and \(\bar{\xi}^{(1)},\) and then show that \(\left(c_{1}-i c_{2}\right) \xi^{(1)}+\) \(\left(c_{1}+i c_{2}\right) \bar{\xi}^{(1)}=0\) (b) Show that \(c_{1}-i c_{2}=0\) and \(c_{1}+i c_{2}=0\) and then that \(c_{1}=0\) and \(c_{2}=0 .\) Consequently, a and b are linearly independent. (c) To show that \(\mathbf{u}(t)\) and \(\mathbf{v}(t)\) are linearly independent consider the equation \(c_{1} \mathbf{u}\left(t_{0}\right)+\) \(c_{2} \mathbf{v}\left(t_{0}\right)=\mathbf{0}\), where \(t_{0}\) is an arbitrary point. Rewrite this equation in terms of a and \(\mathbf{b}\), and then proceed as in part (b) to show that \(c_{1}=0\) and \(c_{2}=0 .\) Hence \(\mathbf{u}(t)\) and \(\mathbf{v}(t)\) are linearly independent at the arbitrary point \(t_{0}\). Therefore they are linearly independent at every point and on every interval.

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