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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

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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: $$ \mathbf{\Phi}(t) = \frac{1}{4} e^{-3t} \begin{pmatrix} 4 & 2 \\ 2 & 1 \end{pmatrix} +\frac{3}{4} e^{t} \begin{pmatrix} 4 & -2 \\ -2 & 1 \end{pmatrix}. $$

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

Express the general solution of the given system of equations in terms of real-valued functions. In each of Problems 1 through 6 also draw a direction field, sketch a few of the trajectories, and describe the behavior of the solutions as \(t \rightarrow \infty\). $$ \mathbf{x}^{\prime}=\left(\begin{array}{rr}{-1} & {-4} \\ {1} & {-1}\end{array}\right) \mathbf{x} $$

In each of Problems 9 and 10 find the solution of the given initial value problem. Describe the behavior of the solution as \(t \rightarrow \infty\). $$ \mathbf{x}^{\prime}=\left(\begin{array}{ll}{1} & {-5} \\ {1} & {-3}\end{array}\right) \mathbf{x}, \quad \mathbf{x}(0)=\left(\begin{array}{l}{1} \\ {1}\end{array}\right) $$

Let $$ \mathbf{J}=\left(\begin{array}{ccc}{\lambda} & {1} & {0} \\ {0} & {\lambda} & {1} \\ {0} & {0} & {\lambda}\end{array}\right) $$ where \(\lambda\) is an arbitrary real number. (a) Find \(\mathbf{J}^{2}, \mathbf{J}^{3},\) and \(\mathbf{J}^{4}\). (b) Use an inductive argument to show that $$ \mathbf{J}^{n}=\left(\begin{array}{ccc}{\lambda^{n}} & {n \lambda^{n-1}} & {[n(n-1) / 2] \lambda^{n-2}} \\ {0} & {\lambda^{n}} & {n \lambda^{n-1}} \\\ {0} & {0} & {\lambda^{n}}\end{array}\right) $$ (c) Determine exp(Jt). (d) Observe that if you choose \(\lambda=2\), then the matrix \(\mathbf{J}\) in this problem is the same as the matrix \(\mathbf{J}\) in Problem \(17(f)\). Using the matrix T from Problem \(17(f),\) form the product Texp(Jt) with \(\lambda=2\). Observe that the resulting matrix is the same as the fundamental matrix \(\Psi(t)\) in Problem \(17(e) .\)

Prove that if \(\mathbf{A}\) is Hermitian, then \((\mathbf{A} \mathbf{x}, \mathbf{y})=(\mathbf{x}, \mathbf{A} \mathbf{y}),\) where \(\mathbf{x}\) and \(\mathbf{y}\) are any vectors.

Let \(x^{(1)}, \ldots, x^{(n)}\) be linearly independent solutions of \(x^{\prime}=P(t) x,\) where \(P\) is continuous on \(\alpha

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