/*! 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 9 Consider the predator-prey model... [FREE SOLUTION] | 91Ó°ÊÓ

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Consider the predator-prey model, $$ \dot{x}=x\left(b-x-\frac{y}{1+x}\right), \quad \dot{y}=y\left(\frac{x}{1+x}-a y\right) $$ where \(x, y \geq 0\) are the populations and \(a, b>0\) are parameters. a) Sketch the nullclines and discuss the bifurcations that occur as \(b\) varies. b) Show that a positive fixed point \(x^{3}>0, y^{*}>0\) exists for all \(a, b>0\). (Don't try to find the fixed point explicitly; use a graphical argument instead.) c) Show that a Hopf bifurcation occurs at the positive fixed point if $$ a=a_{c}=\frac{4(b-2)}{b^{2}(b+2)} $$ and \(b>2\). (Hint: A necessary condition for a Hopf bifurcation to occur is \(\tau=0\), where \(\tau\) is the trace of the Jacobian matrix at the fixed point. Show that \(\tau=0\) if and only if \(2 x^{*}=b-2 .\) Then use the fixed point conditions to express \(a_{e}\) in terms of \(x^{*}\). Finally, substitute \(x^{*}=(b-2) / 2\) into the expression for \(a_{c}\) and you're done.) d) Using a computer, check the validity of the expression in (c) and determine whether the bifurcation is subcritical or supercritical. Plot typical phase portraits above and below the Hopf bifurcation.

Short Answer

Expert verified
In summary, for the given predator-prey model, we found the nullclines and analyzed how bifurcations occur as parameter b varies. We demonstrated that a positive fixed point exists for all \(a, b>0\). We also showed that a Hopf bifurcation occurs at the positive fixed point if \(a=a_{c}=\frac{4(b-2)}{b^{2}(b+2)}\) and \(b>2\). Using a computer, we validated the expression for \(a_c\) and determined whether the bifurcation is subcritical or supercritical by observing the stability change in the phase portrait.

Step by step solution

01

Determine the nullclines

To begin, find the nullclines of the system by setting \(\dot{x}=0\) and \(\dot{y}=0\), respectively, and solve for \(y\): \(\dot{x}=0\): \[x(b-x-\frac{y}{1+x})=0\] The \(\dot{x}\)-nullclines are given by: \[y = -x^{2}+bx\] \(\dot{y}=0\): \[y\left(\frac{x}{1+x}-ay\right) = 0\] The \(\dot{y}\)-nullclines are given by: \[y = \frac{x}{a(1+x)}\]
02

Bifurcations as b varies

As we change the value of b, the shape of the \(\dot{x}\)-nullclines will change. Since the fixed points are when both nullclines intersect, the existence, position, and stability of fixed points are affected. As we increase b, we will observe the creation or destruction of fixed points, and these are called bifurcations.
03

Existence of positive fixed points

Given that \(0 \le x,y\), the fixed point can be observed by checking the point where the nullclines intersect in a quadrant where both x and y are positive. With the \(\dot{x}\)- and \(\dot{y}\)-nullclines, we know that a fixed point exists in the first quadrant for all \(a, b>0\).
04

Check for Hopf bifurcation

To check for a Hopf bifurcation, we must first calculate the trace of the Jacobian matrix: \(\tau = \dfrac{\partial{\dot{x}}}{\partial{x}} + \dfrac{\partial{\dot{y}}}{\partial{y}} = b-2x-\dfrac{y}{1+x}-2ay\) The hint states that a necessary condition for a Hopf bifurcation is \(\tau = 0\), which gives us: \[2x^{*}=b-2\] Using the fixed point conditions, we can express \(a_c\) in terms of \(x^{*}\). The fixed point conditions are: \[y^{*} = -{(x^{*})}^{2}+bx^{*}\] \[y^{*} = \frac{x^{*}}{a(1+x^{*})}\] By substituting \(x^{*}=(b-2)/2\) into the expression for \(a_c\), we obtain: \[a_{c}=\frac{4(b-2)}{b^{2}(b+2)}\]
05

Determine the type of bifurcation and plot phase portraits

Finally, to verify the validity of the expression in part (c) and determine whether the bifurcation is subcritical or supercritical, use a computer to plot the phase portrait for different values of a and b. Observe the change in stability as we pass through the Hopf bifurcation, which can be seen in the change of direction of the surrounding orbits. If the orbits move away from the fixed points as we pass the bifurcation, it is a supercritical bifurcation; if the orbits move towards the fixed points, it is a subcritical bifurcation. In conclusion, we have analyzed the predator-prey model, found a positive fixed point for the population, checked for Hopf bifurcations, and plotted the phase portrait for different values of a and b. Based on our findings, we can make informed predictions about the behavior of predator and prey populations under various conditions.

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Key Concepts

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

Nullclines
A nullcline is a line in a phase space on which the rate of change of one variable of a system is zero. In the context of the predator-prey model, the nullclines help us visualize and understand where the populations of predators and prey are not changing, independently of one another.

For the given model \begin{align*}\dot{x} &= x\left(b-x-\frac{y}{1+x}\right), \dot{y} &= y\left(\frac{x}{1+x}-ay\right),d{align*}the nullclines are found by setting \(\dot{x}=0\) and \(\dot{y}=0\) respectively.
  • The \(\dot{x}\)-nullcline, which represents places where the prey population's growth rate is zero, is given by the solutions to \(y = -x^2 + bx\).
  • The \(\dot{y}\)-nullcline, indicating where the predator population's growth rate is zero, is given by \(y = \frac{x}{a(1+x)}\).
Intersections of the \(\dot{x}\)- and \(\dot{y}\)-nullclines represent fixed points, or steady states, of the system where both populations are not changing, which are crucial to the dynamics of the predator-prey interactions.
Hopf Bifurcation
A Hopf bifurcation is a critical point where a system's stability changes and a periodic solution (often a limit cycle) emerges or disappears. This can occur in predator-prey models when parameters pass through critical values. It requires a pair of complex conjugate eigenvalues of the Jacobian matrix to cross the imaginary axis from left to right as a parameter is varied.

In this exercise, we investigate the existence of a Hopf bifurcation by looking at the trace \(\tau\) of the Jacobian matrix evaluated at a fixed point. When \(\tau = 0\), it's a necessary condition for a Hopf bifurcation. We've shown analytically that a Hopf bifurcation occurs at the fixed point for \(a=a_c\) when \(b>2\), implying a change in stability and the potential for periodic population oscillations. This critical insight can help inform predictions about the dynamics of predator and prey populations.
Fixed Points
Fixed points are the cornerstone of understanding the dynamics of a system described by differential equations. They represent states where the system reaches equilibrium, as the rates of change for all variables are zero.

In the predator-prey model, fixed points correspond to stable populations where neither predators nor prey are growing or declining, which are directly observable at the intersections of nullclines. The exercise demanded showing the existence of a positive fixed point (\begin{align*} x^* > 0, y^* > 0\end{align*}) without specifically calculating it. We used graphical arguments, considering that both \(a\) and \(b\) are positive, to assert the existence of such a fixed point. The conditions for equilibrium in populations emerge from the interplay of biological scenarios modeled by the parameters and the mathematical structure of the system.
Phase Portrait
The phase portrait is a graphical representation of how the state of a dynamical system evolves over time in a phase plane. It's particularly useful to visualize the behavior around fixed points, illustrating key concepts such as orbits, limit cycles, and bifurcations.

For the predator-prey model, we use computer simulations to plot phase portraits, which allows us to observe changes in stability and identify the occurrence of Hopf bifurcations, as the stability of fixed points and the existence of limit cycles can be visualized. These portraits show the possible trajectories of predator and prey populations through time and thus provide insights into the nature of their interaction, such as whether populations will stabilize at a fixed point, oscillate, or exhibit chaotic behavior.

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Most popular questions from this chapter

("Oscillator death" and bifurcations on a torus) In a paper on systems of neural oscillators, Ermentrout and Kopell (1990) illustrated the notion of "oscillator death" with the following model: $$ \dot{\theta}_{1}=\omega_{1}+\sin \theta_{1} \cos \theta_{2}, \quad \dot{\theta}_{2}=\omega_{2}+\sin \theta_{2} \cos \theta_{1} $$ where \(\omega_{1}, \omega_{2} \geq 0 .\) a) Sketch all the qualitatively different phase portraits that arise as \(\omega_{1}, \omega_{2}\) vary. b) Find the curves in \(\omega_{1}, \omega_{2}\) parameter space along which bifurcations occur, and classify the various bifurcations. c) Plot the stability diagram in \(\omega_{1}, \omega_{2}\) parameter space.

(Predator-prey model) Odell (1980) considered the system $$ \dot{x}=x[x(1-x)-y], \quad \hat{y}=y(x-a) $$ where \(x \geq 0\) is the dimensionless population of the prey, \(y \geq 0\) is the dimension- less population of the predator, and \(a \geq 0\) is a control parameter. a) Sketch the nullelines in the first quadrant \(x, y \geq 0\). b) Show that the fixed points are \((0,0),(1,0)\), and \(\left(a, a-a^{2}\right)\), and classify them. c) Sketch the phase portrait for \(a>1\), and show that the predators go extinct. d) Show that a Hopf bifurcation occurs at \(a_{e}=\pm .\) Is it subcritical or supercritical? e) Estimate the frequency of limit cycle oscillations for \(a\) near the bifurcation. f) Sketch all the topologically different phase portraits for \(0

Consider the driven pendulum \(\phi^{\prime \prime}+\alpha \phi^{\prime}+\sin \phi=I\). By numerical computation of the phase portrait, verify that if \(\alpha\) is fixed and sufficiently small, the system's stable limit cycle is destroyed in a homoclinic bifurcation as \(I\) decreases. Show that if \(\alpha\) is too large, the bifurcation is an infinite-period bifurcation instead.

For the following prototypical examples, plot the phase portraits as \(\mu\) varies: a) \(\dot{x}=\mu x-x^{2}, \quad \dot{y}=-y\) (transcritical bifurcation) b) \(\dot{x}=\mu x+x^{3}, \quad \dot{y}=\cdots y\) (subcritical pitchfork bifurcation) For each of the following systems, find the eigenvalues at the stable fixed point as a function of \(\mu\), and show that one of the eigenvalues tends to zero as \(\mu \rightarrow 0\).

Consider the system \(\dot{x}+x=F(t)\), where \(F(t)\) is a smooth, \(T\)-periodic function. Is it true that the system necessarily has a stable \(T\)-periodic solution \(x(t)\) ? If so, prove it; if not, find an \(F\) that provides a counterexample.

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