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(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. $$ d x / d t=x-y^{2}, \quad d y / d t=y-x^{2} $$

Short Answer

Expert verified
2. What is the Jacobian matrix? 3. What are the eigenvalues for each critical point? 4. What type of critical points are (0,0) and (1,1)? 5. How can we draw a phase portrait of the nonlinear system? Answers: 1. The critical points of the system are (0,0) and (1,1). 2. The Jacobian matrix is given by: $$ J(x,y) = \begin{pmatrix} 1 & -2y\\ -2x & 1 \end{pmatrix} $$ 3. The eigenvalues are λ₁ = 1 (double) for the critical point (0,0), and λ₂ = -1, λ₃ = 3 for the critical point (1,1). 4. The critical point (0,0) is an unstable improper node, and the critical point (1,1) is a saddle point, which is also unstable. 5. To draw a phase portrait of the nonlinear system, we can use computer software like MATLAB or Mathematica, or sketch the directions of the vector field while considering the behavior of trajectories around the critical points.

Step by step solution

01

Step 1. Determine all critical points:

To find the critical points, we need to set both dx/dt and dy/dt equal to zero and solve the system of equations. $$ \begin{cases} x - y^2 = 0\\ y - x^2 = 0 \end{cases} $$ Since both equations are equal to zero, we can set them equal to each another: $$ x^2 = y^2 $$ It implies that \(x = y\) or \(x = -y\). Substituting these conditions back into original equations, we obtain the critical points: \((0,0)\) and \((1,1)\).
02

Step 2. Find the corresponding linear system near each critical point:

To find the linear system near each critical point, we need to compute the Jacobian matrix of the original system: $$ J(x,y) = \begin{pmatrix} \frac{\partial (x-y^2)}{\partial x} & \frac{\partial (x-y^2)}{\partial y}\\ \frac{\partial (y-x^2)}{\partial x} & \frac{\partial (y-x^2)}{\partial y} \end{pmatrix} = \begin{pmatrix} 1 & -2y\\ -2x & 1 \end{pmatrix} $$ Evaluate the Jacobian matrix at the critical points \((0,0)\) and \((1,1)\): $$ J(0,0) = \begin{pmatrix} 1 & 0\\ 0 & 1 \end{pmatrix}, \quad J(1,1) = \begin{pmatrix} 1 & -2\\ -2 & 1 \end{pmatrix} $$
03

Step 3. Find the eigenvalues of each linear system:

To find the eigenvalues of each linear system, we need to compute the determinant: $$ \det(J - \lambda I) = (1-\lambda)^2 - (-2y)(-2x) = \lambda^2 - 2\lambda + 1 - 4xy $$ For the critical points \((0,0)\) and \((1,1)\), we have: $$ \det(J(0,0) - \lambda I) = \lambda^2 - 2\lambda + 1\\ \det(J(1,1) - \lambda I) = \lambda^2 - 2\lambda - 3 $$ The eigenvalues are the roots of these characteristic equations: $$ \lambda^2 - 2\lambda + 1 = (\lambda - 1)^2\\ \lambda^2 - 2\lambda - 3 = (\lambda+1)(\lambda-3) $$ Thus, eigenvalues are \(\lambda_1 = 1\) (double) for the critical point \((0,0)\) and \(\lambda_2 = -1, \lambda_3 = 3\) for the critical point \((1,1)\).
04

Step 4. Analyze the nonlinear system based on the eigenvalues:

Since eigenvalues for the critical point \((0,0)\) are positive and double, the point \((0,0)\) is an unstable improper node. For the critical point \((1,1)\), since one eigenvalue is positive and the other is negative, the point \((1,1)\) is a saddle point which is also unstable.
05

Step 5. Draw a phase portrait of the nonlinear system:

Drawing the phase portrait would confirm that \((0,0)\) is an unstable improper node and \((1,1)\) is a saddle point. In this case, the phase portrait can be drawn using computer software like MATLAB or Mathematica, or by sketching the directions of the vector field and considering the behavior of trajectories around the critical points. It would show that trajectories near \((0,0)\) move away from the point, and the system's state moves along its eigendirections at the saddle point \((1,1)\).

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Most popular questions from this chapter

(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. $$ d x / d t=x-x^{2}-x y, \quad d y / d t=3 y-x y-2 y^{2} $$

show that the given system has no periodic solutions other than constant solutions. $$ d x / d t=x+y+x^{3}-y^{2}, \quad d y / d t=-x+2 y+x^{2} y+y^{3} / 3 $$

Can be interpreted as describing the interaction of two species with population densities \(x\) and \(y .\) In each of these problems carry out the following steps. (a) Draw a direction field and describe how solutions seem to behave. (b) Find the critical points. (c) For each critical point find the corresponding linear system. Find the eigenvalues and eigenvectors of the linear system; classify each critical point as to type, and determine whether it is asymptotically stable, or unstable. (d) Sketch the trajectories in the neighborhood of each critical point. (e) Draw a phase portrait for the system. (f) Determine the limiting behavior of \(x\) and \(y\) as \(t \rightarrow \infty\) and interpret the results in terms of the populations of the two species. $$ \begin{array}{l}{d x / d t=x(1.5-0.5 y)} \\ {d y / d t=y(-0.5+x)}\end{array} $$

(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.

The system $$ x^{\prime}=3\left(x+y-\frac{1}{5} x^{3}-k\right), \quad y^{\prime}=-\frac{1}{3}(x+0.8 y-0.7) $$ is a special case of the Fitahugh-Nagumo equations, which model the transmission of neural impulses along an axon. The parameter \(k\) is the external stimulus. (a) For \(k=0\) show that there is one critical point. Find this point and show that it is an asymptotically stable spiral point. Repeat the analysis for \(k=0.5\) and show the critical point is now an unstable spiral point. Draw a phase portrait for the system in each case. (b) Find the value \(k_{0}\) where the critical point changes from asymptotically stable to unstable. Draw a phase portrait for the system for \(k=k_{0}\). (c) For \(k \geq k_{0}\) the system exhibits an asymptotically stable limit cycle. Plot \(x\) versus \(t\) for \(k=k_{0}\) for several periods and estimate the value of the period \(T\). (d) The limit cycle actually exists for a small range of \(k\) below \(k_{0}\). Let \(k_{1}\) be the smallest value of \(k\) for which there is a limit cycle. Find \(k_{1}\).

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