/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 11 If a system has two distinct neg... [FREE SOLUTION] | 91Ó°ÊÓ

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If a system has two distinct negative eigenvalues, then both straight line solutions will decay to the origin with the passage of time. Consequently, all solutions will decay to the origin. Enter the system, \(x^{\prime}=-4 x+y, y^{\prime}=-2 x-y\), in pplane6 and plot the straight line solutions. Plot several more solutions and note that they also decay to the origin. Select Solutions \(\rightarrow\) Find an equilibrium point, find the equilibrium point at the origin, then read its classification from the PPLANE6 Equilibrium point data window.

Short Answer

Expert verified
The origin is a stable node, and all solutions decay to the origin.

Step by step solution

01

Write the System in Matrix Form

The given system is \[ x' = -4x + y \] and \[ y' = -2x - y \]. We can represent it in matrix form as \[ \begin{pmatrix} x' \ y' \end{pmatrix} = \begin{pmatrix} -4 & 1 \ -2 & -1 \end{pmatrix} \begin{pmatrix} x \ y \end{pmatrix}. \]
02

Determine the Eigenvalues of the Matrix

To find the eigenvalues, calculate the determinant of \( A - \lambda I \) where \( A = \begin{pmatrix} -4 & 1 \ -2 & -1 \end{pmatrix} \) and \( I \) is the identity matrix. This yields the characteristic equation: \[ \det(\begin{pmatrix} -4 - \lambda & 1 \ -2 & -1 - \lambda \end{pmatrix}) = 0. \] Solving the determinant gives \[ (-4 - \lambda)(-1 - \lambda) - (1)(-2) = \lambda^2 + 5\lambda + 6 = 0. \] This factors to \( (\lambda + 2)(\lambda + 3) = 0 \) with eigenvalues \( \lambda_1 = -2 \) and \( \lambda_2 = -3 \).
03

Analyze the Eigenvalues

The eigenvalues of the system are \( \lambda_1 = -2 \) and \( \lambda_2 = -3 \). Both are negative, indicating that the solutions will decay toward the origin over time.
04

Understand the Nature of the Solutions

Since both eigenvalues are distinct and negative, the straight line solutions corresponding to each eigenvalue will approach the origin as time progresses. This is confirmed by the system matrix and implies stability at the origin.
05

Pplane6 Analysis

Enter the system into Pplane6 and find the equilibrium point by selecting Solutions \( \rightarrow \) Find an equilibrium point. The equilibrium point is at the origin \((0,0)\). From the Pplane6 Equilibrium point data window, note that the classification is a "stable node" due to the negative eigenvalues.
06

Plot Solutions in Pplane6

Plot the straight line solutions and several additional trajectories in Pplane6. As expected, they all decay to the origin, affirming the analysis that the origin is a stable equilibrium point.

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Key Concepts

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

Eigenvalues
Eigenvalues are crucial in understanding the behavior of linear systems. In the context of this exercise, they help determine the fate of solutions over time. Solving for eigenvalues involves finding the roots of the characteristic equation derived from the matrix form of a given system. In our problem, the eigenvalues are
  • \( \lambda_1 = -2 \)
  • \( \lambda_2 = -3 \)
Both are negative, which is significant for understanding system dynamics. When eigenvalues are negative, they indicate that solutions to the system tend to decay to the equilibrium point, specifically the origin in our system. Negative eigenvalues imply that the system is stable, meaning any perturbation will fade away, and the solutions will return to equilibrium. This is why finding eigenvalues is a primary step in stability analysis.
Matrix Form
Expressing a system in matrix form is essential for using mathematical techniques like eigenvalue computation. The given system of equations can be compactly represented in matrix form as follows:\[\begin{pmatrix} x' \ y' \end{pmatrix} = \begin{pmatrix} -4 & 1 \ -2 & -1 \end{pmatrix} \begin{pmatrix} x \ y \end{pmatrix}\]This representation is notably efficient, as it consolidates the equations into a single mathematical expression. In matrix form, systems are easier to analyze and solve using linear algebra techniques. This form allows us to utilize matrix operations, calculate determinants, and derive the characteristic equation necessary for finding eigenvalues. Matrix form serves as the gateway to understanding and modeling system behaviors succinctly.
Equilibrium Point
An equilibrium point in a dynamical system is where the system does not change, i.e., the derivatives become zero. For our system, we establish equilibrium by setting the derivatives to zero:\[ x' = -4x + y = 0 \]\[ y' = -2x - y = 0 \]Through either substitution or elimination methods, solving these equations leads us to the origin \( (0,0) \). This point is often the center of analysis for stability. If a system is perturbed, how it returns to or deviates from this point determines its stability traits. In our exercise, analyzing this point using Pplane6 confirms its stability due to the nature of the eigenvalues.
Stability Analysis
Stability analysis helps determine how a system responds to small disturbances. For the given linear system, stability is assessed by examining the sign of the eigenvalues. Here's what our analysis showed:
  • Both eigenvalues are negative (\( \lambda_1 = -2 \) and \( \lambda_2 = -3 \)), which points to a 'stable node.'
  • This means that any deviation from the equilibrium (the origin) leads to forces that drive the state back towards this point.
Systems with all negative eigenvalues will exhibit convergence to the equilibrium, implying long-term predictability and lack of oscillations or spirals away from the point. This exercise reaffirms that stability analysis is pivotal for discerning the enduring behavior of dynamical systems.

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Most popular questions from this chapter

In Exercises 31-34 we consider the effect of a non-linear perturbation which leaves the Jacobian at \((0,0)\) unchanged. The theory predicts that, in (maybe very small) neighborhoods of equilibrium points where the eigenvalues of the Jacobian are non-zero and not equal, a non-linear system will act very much like the linear system associated with the Jacobian. We will use pplane6 to verify this by performing steps i), ii), and iii) below for the system in the indicated exercise. i) Make up a perturbation for the system that vanishes to second order at the origin. As an example, instead of the system in Exercise 21 consider the perturbed system $$ \begin{aligned} &x^{\prime}=x+y-x y \\ &y^{\prime}=-18 x+10 y-x^{2}-y^{2} \end{aligned} $$ ii) Show that the Jacobian of the perturbed system at the origin is the same as that of the unperturbed system. iii) Starting with the display rectangle \(-5 \leq x \leq 5,-5 \leq y \leq 5\), zoom in square to smaller squares centered at \((0,0)\) until the solution curves look like those of the linear system. Exercise 23 .

In Exercises \(1-4\), without the aid of technology, using only your algebra skills, sketch the nullclines and find the equilibrium point(s) of the assigned system. Indicate the flow of the the vector field along each nullcline, similar to that shown in Figure 13.1. Check your result with pplane6. If the Symbolic Toolbox is available, use the solve command to find the equilibrium point(s). $$ \begin{aligned} &x^{\prime}=2 x+y \\ &y^{\prime}=4 x+2 y \end{aligned} $$

In Exercises \(21-30\), perform steps i) and ii) for the linear system $$ \mathbf{x}^{\prime}=\mathbf{A x}, $$ where \(\mathbf{A}\) is the given matrix. i) Find the type of the equilibrium point at the origin. Do this without the aid of any technology or pplane6. You may, of course, check your answer using pplane. ii) Use pplane6 to plot several solution curves - enough to fully illustrate the behavior of the system. You will find it convenient to use the "linear system" choice from the Gallery menu. If the eigenvalues are real, use the "Keyboard input" option to include straight line solutions starting at \(\pm 10\) times the eigenvectors. If the equilibrium point is a saddle point, compute and plot the separatrices. $$ \left[\begin{array}{ll} 2 & -2 \\ 4 & -4 \end{array}\right] $$

In contrast to Exercises \(31-34\), consider the system $$ \begin{aligned} &x^{\prime}=y+a x^{3} \\ &y^{\prime}=-x \end{aligned} $$ for the three values 0,10 and \(-10\) of the parameter \(a\). a) Show that all three systems have the same Jacobian matrix at the origin. What type of equilibrium point at \((0,0)\) is predicted by the eigenvalues of the Jacobian? b) Use pplane6 to find evidence that will enable you to make a conjecture as to the type of the equilibrium point at \((0,0)\) in each of the three cases. c) Consider the function \(h(x, y)=x^{2}+y^{2}\). In each of the three cases, restrict \(h\) to a solution curve and differentiate the result with respect to \(t\) (Recall: \(d h / d t=(\partial h / \partial x)(d x / d t)+(\partial h / \partial y)(d y / d t))\). Can you use the result to verify the conjecture you made in part b)? Hint: Note that \(h(x, y)\) measures the distance between the origin and \((x, y)\). d) Does the Jacobian predict the behavior of the non-linear systems in this case?

It is a nice exercise to classify linear systems based on their position in the trace-determinant plane. Consider the matrix $$ A=\left[\begin{array}{ll} a & b \\ c & d \end{array}\right] $$ a) Show that the characteristic polynomial of the matrix \(A\) is \(p(\lambda)=\lambda^{2}-T \lambda+D\), where \(T=a+d\) is the trace of \(A\) and \(D=\operatorname{det}(A)=a d-b c\) is the determinant of \(A\). b) We know that the characteristic polynomial factors as \(p(\lambda)=\left(\lambda-\lambda_{1}\right)\left(\lambda-\lambda_{2}\right)\), where \(\lambda_{1}\) and \(\lambda_{2}\) are the eigenvalues. Use this and the result of part (a) to show that the product of the eigenvalues is equal to the determinant of matrix A. Note: This is a useful fact. For example, if the determinant is negative, then you must have one positive and one negative eigenvalue, indicating a saddle equilibrium point. Also, show that the sum of the eigenvalues equals the trace of matrix \(A\). c) Show that the eigenvalues of matrix \(A\) are given by the formula $$ \lambda=\frac{T \pm \sqrt{T^{2}-4 D}}{2} $$ Note that there are three possible scenarios. If \(T^{2}-4 D<0\), then there are two complex eigenvalues. If \(T^{2}-4 D>0\), there are two real eigenvalues. Finally, if \(T^{2}-4 D=0\), then there is one repeated eigenvalue of algebraic multiplicity two. d) Draw a pair of axes on a piece of poster board. Label the vertical axis \(D\) and the horizontal axis \(T\). Sketch the graph of \(T^{2}-4 D=0\) on your poster board. The axes and the parabola defined by \(T^{2}-4 D=0\) divide the trace- determinant plane into six distinct regions, as shown in Figure 13.17. e) You can classify any matrix \(A\) by its location in the trace-determinant plane. For example, if $$ A=\left[\begin{array}{rr} 1 & 2 \\ -3 & 2 \end{array}\right] $$ then \(T=3\) and \(D=8\), so the point \((T, D)\) is located in the first quadrant. Furthermore, \((3)^{2}-4(8)<\) 0 , placing the point \((3,8)\) above the parabola \(T^{2}-4 D=0\). Finally, if you substitute \(T=3\) and \(D=8\) into the formula \(\lambda=\left(T \pm \sqrt{T^{2}-4 D}\right) / 2\), then you get eigenvalues that are complex with a positive real part, making the equilibrium point of the system \(\mathbf{x}^{\prime}=A \mathbf{x}\) a spiral source. Use pplane6 to generate a phase portrait of this particular system and attach the printout to the poster board at the point \((3,8)\). f) Linear systems possess a small number of distinctive phase portraits. Each of these is graphically different from the others, but each corresponds to the pair of eigenvalues and their multiplicities. For each case, use pplane 6 to construct a phase portrait, and attach a printout at its appropriate point \((T, D)\) in your poster board trace-determinant plane. Hint: There are degenerate cases on the axes and the parabola. For example, you can find degenerate cases on the parabola in the first quadrant that separate nodal sources from spiral sources. There are also a number of interesting degenerate cases at the origin of the trace-determinant plane. One final note: We have intentionally used the words "small number of distinctive cases"' so as to spur argument amongst our readers when working on this activity. What do you think is the correct number?

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