Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

(a) Find the eigenvalues and eigenvectors. (b) Classify the critical point \((0,0)\) as to type and determine whether it is stable, asymptotically stable, or unstable. (c) Sketch several trajectories in the phase plane and also sketch some typical graphs of \(x_{1}\) versus \(t .\) (d) Use a computer to plot accurately the curves requested in part (c). \(\frac{d \mathbf{x}}{d t}=\left(\begin{array}{rr}{-1} & {-1} \\ {0} & {-0.25}\end{array}\right) \mathbf{x}\)

Short Answer

Expert verified
Question: Determine the eigenvalues, eigenvectors, type, and stability of the critical point (0,0) for the given matrix $A = \begin{pmatrix} -1 & -1 \\ 0 & -0.25 \end{pmatrix}$. Provide a rough sketch of the trajectories in the phase plane and a rough sketch of the graph of \(x_{1}\) versus \(t\).

Step by step solution

01

Determine the characteristic equation

To find the eigenvalues, first, we need to find the determinant of \((A - \lambda I)\) where \(A\) is the given matrix, and \(\lambda\) is the eigenvalue. $A = \begin{pmatrix} -1 & -1 \\ 0 & -0.25 \end{pmatrix}$, $I = \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix}$, and $(A-\lambda I) = \begin{pmatrix} -1-\lambda & -1 \\ 0 & -0.25-\lambda \end{pmatrix}\(. The characteristic equation is formed by setting the determinant of \)(A - \lambda I)$ to zero.
02

Compute the eigenvalues

For the characteristic equation, we have \(|A - \lambda I|= (-1-\lambda)(-0.25-\lambda) - (0)(-1) = 0\). Solving for \(\lambda\), we get \(\lambda_{1}=-1\) and \(\lambda_{2}=-0.25\).
03

Compute the eigenvectors

To find the eigenvectors corresponding to each eigenvalue, we need to solve the following equation with each eigenvalue: \((A - \lambda_{i} I) v_{i}=0\). 1. For \(\lambda_{1}=-1\), we have $(A - \lambda_{1} I) v_{1} = \begin{pmatrix} 0 & -1 \\ 0 & 0.75 \end{pmatrix} v_{1}=0\(, which gives us \)v_{1}= \begin{pmatrix} 1 \\ 0 \end{pmatrix}$. 2. For \(\lambda_{2}=-0.25\), we have $(A - \lambda_{2} I) v_{2} = \begin{pmatrix} -0.75 & -1 \\ 0 & 0 \end{pmatrix} v_{2}=0\(, which gives us \)v_{2}= \begin{pmatrix} 1 \\ 0.75 \end{pmatrix}$. So, the eigenvalues are \(\lambda_{1} = -1\) and \(\lambda_{2} = -0.25\), and their respective eigenvectors are $v_{1} = \begin{pmatrix} 1 \\ 0 \end{pmatrix}\( and \)v_{2} = \begin{pmatrix} 1 \\ 0.75 \end{pmatrix}$. #b: Classifying the critical point#
04

Determine the type of critical point

The critical point is classified based on its eigenvalues. Since both eigenvalues are real and have the same sign, the critical point is a node. Since they are both negative, it is a stable node.
05

Determine the stability of the critical point

We can determine the stability of the critical point based on the value of the eigenvalues. Since both eigenvalues are negative, the critical point \((0,0)\) is asymptotically stable. #c: Sketching trajectories and graph of \(x_{1}\) vs. \(t\)
06

Sketching the trajectories

The two eigenvectors are $v_{1} = \begin{pmatrix} 1 \\ 0 \end{pmatrix}\( and \)v_{2} = \begin{pmatrix} 1 \\ 0.75 \end{pmatrix}\(. \)v_{1}\( gives the horizontal trajectories, while \)v_{2}$ gives the slanted trajectories. The trajectories will converge towards the critical point (0,0) as it is an asymptotically stable node. These trajectories will give us a rough sketch of the phase plane.
07

Sketching the graph of \(x_{1}\) vs \(t\)

The graph of \(x_{1}\) versus \(t\) will be exponentially decaying since the eigenvalues are negative. The rate of decay is determined by the eigenvalues, so we will have two curves that decay at different rates - one with a rate of \(-1\) (the curve from \(\lambda_{1}=-1\)) and another with a rate of \(-0.25\) (the curve from \(\lambda_{2}=-0.25\)). For part (d), use a suitable software like MATLAB, Python, or Wolfram Alpha to plot the curves mentioned in part (c) for an accurate plot.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

Key Concepts

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

Critical Points
Critical points play a crucial role when analyzing dynamic systems like the one described by the given matrix equation. The critical point we're focusing on is **(0,0)**, a point where the system settles when there are no external inputs. Critical points are sometimes referred to as equilibrium points. These points represent states where the system doesn't evolve further unless disturbed. To classify this critical point, we mainly rely on the eigenvalues and eigenvectors derived from the system's matrix. Eigenvalues give us a clear picture of the system's behavior around the critical point. Here,
  • Eigenvalue \( \lambda_1 = -1 \)
  • Eigenvalue \( \lambda_2 = -0.25 \)
Both eigenvalues are real and negative, indicating that any motion starting nearby will converge to the critical point. Each eigenvalue corresponds to a direction in which the system moves—indicating either convergence or divergence relative to the critical point.
Stability Analysis
Stability analysis helps determine how a system responds over time when it's slightly disturbed from its equilibrium state. For systems like the one we're handling, eigenvalues provide significant insights into stability. The type of eigenvalues indicates if the critical point is stable, unstable, or asymptotically stable. For the critical point (0,0), both eigenvalues \( \lambda_1 = -1 \) and \( \lambda_2 = -0.25 \) are negative. This tells us:
  • The system is asymptotically stable. This means any trajectory starting from a nearby point in the phase plane will eventually return to the critical point over time.
  • The negativity of the eigenvalues implies the trajectories decay over time without oscillating, leading them to the equilibrium point smoothly.
In practical terms, if this system represented, say, a population or temperature model, it would return to equilibrium without wild fluctuations, indicating robustness against small disturbances.
Phase Plane Trajectories
Visualizing the behavior of a system can be made easier through phase plane trajectories. The phase plane is essentially a graphical representation of the system's possible states plotted with respect to time. For our system:
  • The eigenvector associated with \( \lambda_1 = -1 \) is \( \begin{pmatrix} 1 \ 0 \end{pmatrix} \), leading to horizontal trajectories approaching the critical point. These directions highlight the system's fast-decay path.
  • The eigenvector for \( \lambda_2 = -0.25 \) is \( \begin{pmatrix} 1 \ 0.75 \end{pmatrix} \), showing slanted paths that approach more gradually due to the slower decay rate.
Both sets of trajectories converge to the critical point, illustrating the system's stability clearly. In this visualization, you will see trajectories of different curvature and speeds of convergence, all directed towards (0,0). By observing these trajectories and how they behave over time, we fully appreciate the system's built-in damping characteristics.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

(a) By solving the equation for \(d y / d x,\) show that the equation of the trajectories of the undamped pendulum of Problem 19 can be written as $$ \frac{1}{2} y^{2}+\omega^{2}(1-\cos x)=c $$ where \(c\) is a constant of integration. (b) Multiply Eq. (i) by \(m L L^{2} .\) Then express the result in terms of \(\theta\) to obtain $$ \frac{1}{2} m L^{2}\left(\frac{d \theta}{d t}\right)^{2}+m g L(1-\cos \theta)=E $$ where \(E=m L^{2} c .\) (c) Show that the first term in Eq. (ii) is the kinetic energy of the pendulum and that the second term is the potential energy due to gravity. Thus the total energy \(E\) of the pendulum is constant along any trajectory; its value is determined by the initial conditions.

In this problem we show how small changes in the coefficients of a system of linear equations can affect the nature of a critical point when the eigenvalues are equal. Consider the system $$ \mathbf{x}^{\prime}=\left(\begin{array}{cc}{-1} & {1} \\ {0} & {-1}\end{array}\right) \mathbf{x} $$ Show that the eigenvalues are \(r_{1}=-1, r_{2}=-1\) so that the critical point \((0,0)\) is an asymptotically stable node. Now consider the system $$ \mathbf{x}^{\prime}=\left(\begin{array}{cc}{-1} & {1} \\ {-\epsilon} & {-1}\end{array}\right) \mathbf{x} $$ where \(|\epsilon|\) is arbitrararily small. Show that if \(\epsilon>0,\) then the eigenvalues are \(-1 \pm i \sqrt{\epsilon}\), so that the asymptotically stable node becomes an asymptotically stable spiral point. If \(\epsilon<0,\) then the roots are \(-1 \pm \sqrt{|\epsilon|},\) and the critical point remains an asymptotically stable node.

(a) Find an equation of the form \(H(x, y)=c\) satisfied by the trajectories. (b) Plot several level curves of the function \(H\). These are trajectories of the given system. Indicate the direction of motion on each trajectory. $$ d x / d t=y, \quad d y / d t=2 x+y $$

(a) Determine all critical points of the given system of equations. (b) Find the corresponding linear system near each critical point. (c) Find the eigenalues of each linear system. What conclusions can you then draw about the nonlinear system? (d) Draw a phase portrait of the nonlinear system to confirm your conclusions, or to extend them in those cases where the linear system does not provide definite information about the nonlinear system. $$ d x / d t=2 x+y+x y^{3}, \quad d y / d t=x-2 y-x y $$

As mentioned in the text, one improvement in the predator-prey model is to modify the equation for the prey so that it has the form of a logistic equation in the absence of the predator. Thus in place of Eqs. ( 1 ) we consider the system $$ d x / d t=x(a-\sigma x-\alpha y), \quad d y / d t=y(-c+\gamma x) $$ where \(a, \sigma, \alpha, c,\) and \(\gamma\) are positive constants. Determine all critical points and discuss their nature and stability characteristics. Assume that \(a / \sigma \gg c / \gamma .\) What happens for initial data \(x \neq 0, y \neq 0 ?\)

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free