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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. $$ \left[\begin{array}{rr} -1 & 0 \\ 3 & -3 \end{array}\right] $$

Short Answer

Expert verified
The equilibrium point at the origin is a stable node.

Step by step solution

01

Identify matrix \( \mathbf{A} \)

The matrix \( \mathbf{A} \) given in the problem is \( \begin{bmatrix} -1 & 0 \ 3 & -3 \end{bmatrix} \). Our goal is to analyze this system at the equilibrium point \((0,0)\).
02

Find Eigenvalues

To find the eigenvalues, we solve the characteristic equation \( \det(\mathbf{A} - \lambda \mathbf{I}) = 0 \). The identity matrix \( \mathbf{I} \) for our system is \( \begin{bmatrix} 1 & 0 \ 0 & 1 \end{bmatrix} \). Thus, \( \mathbf{A} - \lambda \mathbf{I} = \begin{bmatrix} -1 - \lambda & 0 \ 3 & -3 - \lambda \end{bmatrix} \). Calculating the determinant gives us \((-1 - \lambda)(-3 - \lambda) = 0\). Solve for \( \lambda \) to find: \(\lambda_1 = -1\), \(\lambda_2 = -3\).
03

Determine Equilibrium Point Type

The eigenvalues \(\lambda_1 = -1\) and \(\lambda_2 = -3\) are both real and negative. This implies that the equilibrium point at the origin is a **stable node**. This is because negative eigenvalues indicate solutions will decay towards zero.
04

Plot Phase Plane (with pplane6)

In pplane6, the phase portrait can be plotted by entering the system matrix and using the linear system choice from the Gallery menu. Since the equilibrium point is a stable node, the trajectories will spiral in towards the origin, following the directions determined by the eigenvectors.

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Key Concepts

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

Equilibrium Point
In the context of linear systems, the **equilibrium point** is where the system rests naturally, meaning no changes occur over time. For a 2-dimensional linear system like the one in this exercise, the equilibrium point is at the origin \((0,0)\). At this point, the system of differential equations sets to zero, indicating a stationary state. To determine the type of equilibrium point, we examine the eigenvalues of the system's matrix. Specifically, the signs of the eigenvalues tell us about the behavior of system trajectories near this point:
  • If all eigenvalues are negative, as in our example, the equilibrium point is a **stable node**. All trajectories converge to this point, implying decay towards it over time.
  • Positive eigenvalues indicate an **unstable node**, where trajectories diverge away from the point.
  • If eigenvalues have mixed signs, the equilibrium point could be a **saddle point**.
In our exercise, both eigenvalues are negative, confirming a stable node. Understanding these types helps predict system behavior without plotting every trajectory.
Eigenvalues
**Eigenvalues** are critical in determining the stability and nature of a linear system's equilibrium point. They are derived from the system matrix via the characteristic equation. In this exercise, the matrix is \[\begin{bmatrix} -1 & 0 \ 3 & -3 \end{bmatrix}.\]To calculate the eigenvalues, we subtract \( \lambda \mathbf{I} \) from \(\mathbf{A} \), where \(\lambda \) is a scalar and \(\mathbf{I} \) is the identity matrix. Solving the determinant of this modified matrix gives us the eigenvalues.In this case, solving the determinant of \(\mathbf{A} - \lambda \mathbf{I} = 0\) results in \(\lambda_1 = -1\)and \(\lambda_2 = -3\).The negative signs of both eigenvalues are important. They indicate that over time, the system will stabilize at the equilibrium point, making the origin a stable node. The concept of eigenvalues extends to various fields, providing insight into system dynamics quickly and succinctly.
Phase Plane Analysis
**Phase Plane Analysis** provides a visual representation of a system's dynamics. It maps out the trajectories of differential equations on a coordinate plane, offering an intuitive grasp of the system's behavior.For our exercise, plotting this for the matrix \(\mathbf{A} = \begin{bmatrix} -1 & 0 \ 3 & -3 \end{bmatrix}\) reveals a stable node at the origin. The direction and curvature of trajectories illustrate how solutions approach this point over time.In practice, we use tools like pplane6 to automatically generate phase portraits. This involves feeding the system matrix into the software and instructing it to display the trajectories. The trajectories will indicate paths solutions take as time progresses:
  • Solutions spiral or curve depending on eigenvectors and their directions.
  • Trajectories heading towards the origin confirm stability.
  • Systems with complex eigenvalues show spiraling behavior.
Phase plane analysis is invaluable for predicting long-term behavior without solving the differential equations manually. It simplifies understanding how different initial conditions can evolve within the system.

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Most popular questions from this chapter

Duffing 's equation is $$ m x^{\prime \prime}+c x^{\prime}+k x+l x^{3}=F(t) $$ When \(k>0\) this equation models a vibrating spring, which could be soft \((l<0)\) or hard \((l>0)\) (See Student Project #1 in Chapter 8). When \(k<0\) the equation arises as a model of the motion of a long thin elastic steel beam that has its top end embedded in a pulsating frame (the \(F(t)\) term), and its lower end hanging just above two magnets which are slightly displaced from what would be the equilibrium position. We will be looking at the unforced case (i.e. \(F(t)=0\) ), with \(m=1\). The system corresponding to Duffing's equation is available in the Gallery menu. a) This is the case of a hard spring with \(k=16\), and \(l=4\). Use pplane 6 to plot the phase planes of some solutions with the damping constant \(c=0,1\), and 4. In particular, find all equilibrium points. b) Do the same for the soft spring with \(k=16\) and \(l=-4\). Now there will be a pair of saddle points. Find them and plot the stable/unstable orbits. c) Now consider the case when \(k=-1\), and \(l=1\). For each of the cases \(c=0, c=0.2\), and \(c=1\), use pplane6 to analyze the system. In particular, find all equilibrium points and determine their types. Plot stable/unstable orbits where appropriate, and plot typical orbits. d) With \(c=0.2\) in part c), there are two sinks. Determine the basins of attraction of each of these sinks. Indicate these regions on a print out of the phase plane.

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.

Consider the nonlinear system $$ \begin{aligned} &x^{\prime}=x(1-x)-x y, \\ &y^{\prime}=y(2-y)+2 x y . \end{aligned} $$ Show that \((-1 / 3,4 / 3)\) is an equilibrium point of the system. a) Without the use of technology, calculate the Jacobian of the system at the equilibrium point \((-1 / 3\), \(4 / 3)\). What is the equation of the linearization at this equilibrium point? Use [v,e]=eig( \(\mathrm{J})\) to find the eigenvalues and eigenvectors of this Jacobian. b) Enter the system in pplane6. Find the equilibrium point at \((-1 / 3,4 / 3)\). Does the data in the Equilibrium point data window agree with your findings in part (a)? Note: The eigenvalues of the Jacobian predict classification of the equilibrium point. In this case, the point \((-1 / 3,4 / 3)\) is a saddle because the eigenvalues are real and opposite in sign. c) Display the linearization. Does the equation of the linearization agree with your findings in part (a)?

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. $$ \left[\begin{array}{rr} 1 & 1 \\ -18 & 10 \end{array}\right] $$

This is another example of how a system can change as a parameter is varied. Consider the system $$ \begin{aligned} &x^{\prime}=a x+y-x\left(x^{2}+y^{2}\right) \\ &y^{\prime}=-x+a y-y\left(x^{2}+y^{2}\right) \end{aligned} $$ for \(a=0\), and \(a=\pm 0.1\). Use the display rectangle \(-1 \leq x \leq 1\), and \(-1 \leq y \leq 1\), and plot enough solutions in each case to describe behavior of the system. Describe what happens as the parameter \(a\) varies from negative values to positive values. (This is an example of a Hopf bifurcation.) Hint: Look for something completely new, something other than an equilibrium point.

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