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Solve the initial value problem. $$ \mathbf{y}^{\prime}=\left[\begin{array}{lll} -2 & 2 & 1 \\ -2 & 2 & 1 \\ -3 & 3 & 2 \end{array}\right] \mathbf{y}, \quad \mathbf{y}(0)=\left[\begin{array}{r} -6 \\ -2 \\ 0 \end{array}\right] $$

Short Answer

Expert verified
Based on the given matrix and initial value, the solution to the initial value problem for the system of first-order linear differential equations is: $$\mathbf{y}(t) = 7e^{7t}\begin{bmatrix} 0 \\ 1 \end{bmatrix} -e^{-7t}\begin{bmatrix} 1 \\ 0 \end{bmatrix}$$

Step by step solution

01

Find the eigenvalues of the given matrix

To find the eigenvalues, we need to solve the characteristic equation, which is obtained by setting the determinant of the matrix minus the eigenvalue times the identity matrix to zero: $$\begin{vmatrix} -7 - \lambda & 4 \\ -6 & 7 - \lambda \end{vmatrix} = 0$$ Expanding the determinant, we get: \((-7 - \lambda)(7-\lambda) - (-6)4 = \lambda^2 - 49\) Solving for the eigenvalues, we have: \(\lambda_1 = 7\) \(\lambda_2 = -7\)
02

Find the eigenvectors corresponding to the eigenvalues

We start by finding the eigenvector corresponding to \(\lambda_1 = 7\). Substitute the eigenvalue into the matrix equation \((A - \lambda I)\mathbf{v} = 0\): $$ \begin{bmatrix} -7 - 7 & 4 \\ -6 & 7 - 7 \end{bmatrix} \begin{bmatrix} v_1 \\ v_2 \end{bmatrix} = 0 $$ This simplifies to the system of linear equations: $$-14v_1 + 4v_2 =0$$ $$-6v_1 =0$$ Solving for \(v_1\) and \(v_2\) gives \(v_{11} = 0\) and \(v_{12} = 1\). This means, the eigenvector corresponding to \(\lambda_1\) is \(\mathbf{v}_1=\begin{bmatrix} 0 \\ 1 \end{bmatrix}\). Next, find the eigenvector corresponding to \(\lambda_2 = -7\): $$ \begin{bmatrix} -7 - (-7) & 4 \\ -6 & 7 - (-7) \end{bmatrix} \begin{bmatrix} v_1 \\ v_2 \end{bmatrix} = 0 $$ This simplifies to the system of linear equations: $$4v_2 =0$$ $$-6v_1 + 14v_2 =0$$ Solving for \(v_1\) and \(v_2\) gives \(v_{21} = 1\) and \(v_{22} = 0\). This means, the eigenvector corresponding to \(\lambda_2\) is \(\mathbf{v}_2=\begin{bmatrix} 1 \\ 0 \end{bmatrix}\).
03

Set up and solve the general solution of the system

Based on the eigenvalues and eigenvectors found in steps 1 and 2, the general solution of the given system is: $$\mathbf{y}(t) = c_1e^{7t}\begin{bmatrix} 0 \\ 1 \end{bmatrix} + c_2e^{-7t}\begin{bmatrix} 1 \\ 0 \end{bmatrix}$$ Now, we apply the initial condition \(\mathbf{y}(0)=\left[\begin{array}{l}-1\\\ 7\end{array}\right]\) to determine the constants \(c_1\) and \(c_2\): $$\begin{bmatrix} -1 \\ 7 \end{bmatrix} = c_1\begin{bmatrix} 0 \\ 1 \end{bmatrix} + c_2\begin{bmatrix} 1 \\ 0 \end{bmatrix}$$ This gives us the equations \(c_2 = -1\) and \(c_1 = 7\). Substituting the constants back into the general solution gives the particular solution: $$\mathbf{y}(t) = 7e^{7t}\begin{bmatrix} 0 \\ 1 \end{bmatrix} -e^{-7t}\begin{bmatrix} 1 \\ 0 \end{bmatrix}$$ This is the solution to the initial value problem.

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Key Concepts

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

Eigenvalues
Eigenvalues are fundamental in understanding the behavior of linear transformations. They are scalars associated with a square matrix that, when multiplied by an eigenvector, don't alter its direction. In simple terms, finding the eigenvalues of a matrix involves solving the characteristic polynomial equation derived by subtracting a scalar \(\lambda\) from the diagonal entries of the matrix.
  • Mathematically, this is expressed as: \det(A - \lambda I) = 0\.
  • Where \(A\) is the matrix, \(I\) is the identity matrix, and \(\lambda\) represents the eigenvalues.
Determining eigenvalues is critical for systems of differential equations because they help analyze the stability and dynamics of solutions.
Eigenvectors
Eigenvectors work hand-in-hand with eigenvalues to provide deep insights into matrix transformations. An eigenvector corresponding to an eigenvalue \(\lambda\) is a non-zero vector that, when multiplied by the matrix \(A\), results in a scaled version of itself, specifically \(Av = \lambda v\).
  • Once the eigenvalues are found, we solve \( (A - \lambda I)\mathbf{v} = 0 \) for non-trivial vectors \(\mathbf{v}\).
  • The solutions to this equation indicate how the initial movement described by the vector \(\mathbf{v}\) scales under the transformation.
In real-world applications, eigenvectors often represent directions of action, major modes of oscillation, or principal components in systems analysis.
Linear Differential Equations
Linear differential equations are equations involving unknown functions and their derivatives. These equations highlight relationships where the unknown function's exponent is one, maintaining a linear relationship.
  • In the context of matrices, they are expressed as \(\mathbf{y}' = A\mathbf{y}\), where \(\mathbf{y}\) is the vector of unknown functions.
  • The linearity ensures the principle of superposition applies, meaning the sum of solutions is also a solution.
Linear differential equations simplify solving systems because their solutions can be constructed using basic techniques, such as finding eigenvalues and eigenvectors. They also often model real-world phenomena where effects are proportional to causes, such as in mechanical vibrations or electrical circuits.
System of Differential Equations
A system of differential equations comprises multiple equations involving derivatives of several functions. Such systems effectively model complex interactions between different variables.
  • In matrix form, this can be expressed as a vector equation \(\mathbf{y}' = A\mathbf{y}\), where \(\mathbf{y}\) is a vector of unknown functions differentiated and \(A\) is a matrix of coefficients.
  • These systems frequently use initial conditions to find unique solutions, which in turn identify how a system evolves over time.
Analyzing these systems with matrices makes it easy to apply concepts of linear algebra, like eigenvalues and eigenvectors, to find solutions. Interpretation of these solutions then offers insights into the dynamics of the system, allowing predictions of future behavior under given conditions.

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Most popular questions from this chapter

Let \(A\) be an \(n \times n\) constant matrix. Then Theorem 10.2 .1 implies that the solutions of $$\mathbf{y}^{\prime}=A \mathbf{y}$$ are all defined on \((-\infty, \infty)\). (a) Use Theorem 10.2 .1 to show that the only solution of ( A) that can ever equal the zero vector is \(\mathbf{y} \equiv \mathbf{0}\). (b) Suppose \(\mathbf{y}_{1}\) is a solution of \((\mathrm{A})\) and \(\mathbf{y}_{2}\) is defined by \(\mathbf{y}_{2}(t)=\mathbf{y}_{1}(t-\tau),\) where \(\tau\) is an arbitrary real number. Show that \(y_{2}\) is also a solution of (A). (c) Suppose \(\mathbf{y}_{1}\) and \(\mathbf{y}_{2}\) are solutions of \((\mathrm{A})\) and there are real numbers \(t_{1}\) and \(t_{2}\) such that \(\mathbf{y}_{1}\left(t_{1}\right)=\mathbf{y}_{2}\left(t_{2}\right) .\) Show that \(\mathbf{y}_{2}(t)=\mathbf{y}_{1}(t-\tau)\) for all \(t,\) where \(\tau=t_{2}-t_{1} .\) HINT: Show that \(\mathbf{y}_{1}(t-\tau)\) and \(\mathbf{y}_{2}(t)\) are solutions of the same initial value problem for \((\mathrm{A}),\) and apply the uniqueness assertion of Theorem \(10.2 .1 .\)

Suppose \(\mathbf{u}=\left[\begin{array}{l}u_{1} \\ u_{2}\end{array}\right]\) and \(\mathbf{v}=\left[\begin{array}{l}v_{1} \\ v_{2}\end{array}\right]\) are not orthogonal; that is, \((\mathbf{u}, \mathbf{v}) \neq 0\) (a) Show that the quadratic equation $$ (\mathbf{u}, \mathbf{v}) k^{2}+\left(\|\mathbf{v}\|^{2}-\|\mathbf{u}\|^{2}\right) k-(\mathbf{u}, \mathbf{v})=0 $$ has a positive root \(k_{1}\) and a negative root \(k_{2}=-1 / k_{1}\). (b) Let \(\mathbf{u}_{1}^{(1)}=\mathbf{u}-k_{1} \mathbf{v}, \mathbf{v}_{1}^{(1)}=\mathbf{v}+k_{1} \mathbf{u}, \mathbf{u}_{1}^{(2)}=\mathbf{u}-k_{2} \mathbf{v},\) and \(\mathbf{v}_{1}^{(2)}=\mathbf{v}+k_{2} \mathbf{u},\) so that \(\left(\mathbf{u}_{1}^{(1)}, \mathbf{v}_{1}^{(1)}\right)=\left(\mathbf{u}_{1}^{(2)}, \mathbf{v}_{1}^{(2)}\right)=0,\) from the discussion given above. Show that $$ \mathbf{u}_{1}^{(2)}=\frac{\mathbf{v}_{1}^{(1)}}{k_{1}} \quad \text { and } \quad \mathbf{v}_{1}^{(2)}=-\frac{\mathbf{u}_{1}^{(1)}}{k_{1}} $$ (c) Let \(\mathbf{U}_{1}, \mathbf{V}_{1}, \mathbf{U}_{2},\) and \(\mathbf{V}_{2}\) be unit vectors in the directions of \(\mathbf{u}_{1}^{(1)}, \mathbf{v}_{1}^{(1)}, \mathbf{u}_{1}^{(2)},\) and \(\mathbf{v}_{1}^{(2)}\), respectively. Conclude from (a) that \(\mathbf{U}_{2}=\mathbf{V}_{1}\) and \(\mathbf{V}_{2}=-\mathbf{U}_{1},\) and that therefore the counterclockwise angles from \(\mathbf{U}_{1}\) to \(\mathbf{V}_{1}\) and from \(\mathbf{U}_{2}\) to \(\mathbf{V}_{2}\) are both \(\pi / 2\) or both \(-\pi / 2\).

Let $$ \begin{aligned} A &=\left[\begin{array}{rrr} 3 & -1 & -1 \\ -2 & 3 & 2 \\ 4 & -1 & -2 \end{array}\right] \\ \mathbf{y}_{1}=\left[\begin{array}{c} e^{2 t} \\ 0 \\ e^{2 t} \end{array}\right], & \mathbf{y}_{2}=\left[\begin{array}{c} e^{3 t} \\ -e^{3 t} \\ e^{3 t} \end{array}\right], \quad \mathbf{y}_{3}=\left[\begin{array}{c} e^{-t} \\ -3 e^{-t} \\ 7 e^{-t} \end{array}\right], \quad \mathbf{k}=\left[\begin{array}{r} 2 \\ -7 \\ 20 \end{array}\right] \end{aligned} $$ (a) Verify that \(\left\\{\mathbf{y}_{1}, \mathbf{y}_{2}, \mathbf{y}_{3}\right\\}\) is a fundamental set of solutions for \(\mathbf{y}^{\prime}=A \mathbf{y}\). (b) Solve the initial value problem $$ \mathbf{y}^{\prime}=A \mathbf{y}, \quad \mathbf{y}(0)=\mathbf{k} $$ (c) Use the result of Exercise \(6(\mathbf{b})\) to find a formula for the solution of \((\mathrm{A})\) for an arbitrary initial vector \(\mathbf{k}\).

In Exercises \(11-20\) find a particular solution, given that \(Y\) is a fundamental matrix for the complementary system. $$ \mathbf{y}^{\prime}=-\frac{1}{t}\left[\begin{array}{rrr} e^{-t} & -t & 1-e^{-t} \\ e^{-t} & 1 & -t-e^{-t} \\ e^{-t} & -t & 1-e^{-t} \end{array}\right] \mathbf{y}+\frac{1}{t}\left[\begin{array}{c} e^{t} \\ 0 \\ e^{t} \end{array}\right] ; \quad Y=\frac{1}{t}\left[\begin{array}{ccc} e^{t} & e^{-t} & t \\ e^{t} & -e^{-t} & e^{-t} \\ e^{t} & e^{-t} & 0 \end{array}\right] $$

Verify that $$ \mathbf{y}_{1}=e^{\alpha t}(\mathbf{u} \cos \beta t-\mathbf{v} \sin \beta t) \quad \text { and } \quad \mathbf{y}_{2}=e^{\alpha t}(\mathbf{u} \sin \beta t+\mathbf{v} \cos \beta t) $$ are the real and imaginary parts of $$ e^{\alpha t}(\cos \beta t+i \sin \beta t)(\mathbf{u}+i \mathbf{v}) $$

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