Show that this system has a limit cycle in the first quadrant.

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The full question reads as follows:



Consider the predator-prey model



$$dotx = x left(6-x-frac3y1+x right), doty = y(x-2)$$



Assume that all positive solutions are bounded. (a) Find all critical points and determine their local stability. (b) Show that this system has a limit cycle in the first quadrant.



I have finished part (a) and found that $(0,0)$ is a saddle, $(6,0)$ is a saddle, and $(2,4)$ is an unstable focus. I have attempted to do part (b) using some phase plane analysis, but I am looking for a more definite way to prove this. Thanks in advance for any help!







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  • It appears to me that the "focus"--if it is a focus (I say this because I haven't checked, I'm going with what you wrote)--is at $(2, 4)$, not $(2, 3)$. This is why I'm not sure what type of critical point this is, since I'm not sure we got the coordinates right!
    – Robert Lewis
    Jul 24 at 2:00






  • 1




    Just edited, but my question still stands. Thanks Robert!
    – obewanjacobi
    Jul 24 at 3:47










  • Which tools do you know to prove the existence of a cycle?
    – Did
    Jul 24 at 17:32










  • By the way: (2,4) a stable focus, are you sure about this?
    – Did
    Jul 24 at 17:34






  • 1




    According to Mathematica, the eigenvalues at $(2,4)$ are $frac13(1pm isqrt71)$, so $(2,4)$ is an unstable focus.
    – user539887
    Jul 24 at 19:40














up vote
2
down vote

favorite
1












The full question reads as follows:



Consider the predator-prey model



$$dotx = x left(6-x-frac3y1+x right), doty = y(x-2)$$



Assume that all positive solutions are bounded. (a) Find all critical points and determine their local stability. (b) Show that this system has a limit cycle in the first quadrant.



I have finished part (a) and found that $(0,0)$ is a saddle, $(6,0)$ is a saddle, and $(2,4)$ is an unstable focus. I have attempted to do part (b) using some phase plane analysis, but I am looking for a more definite way to prove this. Thanks in advance for any help!







share|cite|improve this question





















  • It appears to me that the "focus"--if it is a focus (I say this because I haven't checked, I'm going with what you wrote)--is at $(2, 4)$, not $(2, 3)$. This is why I'm not sure what type of critical point this is, since I'm not sure we got the coordinates right!
    – Robert Lewis
    Jul 24 at 2:00






  • 1




    Just edited, but my question still stands. Thanks Robert!
    – obewanjacobi
    Jul 24 at 3:47










  • Which tools do you know to prove the existence of a cycle?
    – Did
    Jul 24 at 17:32










  • By the way: (2,4) a stable focus, are you sure about this?
    – Did
    Jul 24 at 17:34






  • 1




    According to Mathematica, the eigenvalues at $(2,4)$ are $frac13(1pm isqrt71)$, so $(2,4)$ is an unstable focus.
    – user539887
    Jul 24 at 19:40












up vote
2
down vote

favorite
1









up vote
2
down vote

favorite
1






1





The full question reads as follows:



Consider the predator-prey model



$$dotx = x left(6-x-frac3y1+x right), doty = y(x-2)$$



Assume that all positive solutions are bounded. (a) Find all critical points and determine their local stability. (b) Show that this system has a limit cycle in the first quadrant.



I have finished part (a) and found that $(0,0)$ is a saddle, $(6,0)$ is a saddle, and $(2,4)$ is an unstable focus. I have attempted to do part (b) using some phase plane analysis, but I am looking for a more definite way to prove this. Thanks in advance for any help!







share|cite|improve this question













The full question reads as follows:



Consider the predator-prey model



$$dotx = x left(6-x-frac3y1+x right), doty = y(x-2)$$



Assume that all positive solutions are bounded. (a) Find all critical points and determine their local stability. (b) Show that this system has a limit cycle in the first quadrant.



I have finished part (a) and found that $(0,0)$ is a saddle, $(6,0)$ is a saddle, and $(2,4)$ is an unstable focus. I have attempted to do part (b) using some phase plane analysis, but I am looking for a more definite way to prove this. Thanks in advance for any help!









share|cite|improve this question












share|cite|improve this question




share|cite|improve this question








edited Jul 25 at 1:46
























asked Jul 24 at 1:22









obewanjacobi

310110




310110











  • It appears to me that the "focus"--if it is a focus (I say this because I haven't checked, I'm going with what you wrote)--is at $(2, 4)$, not $(2, 3)$. This is why I'm not sure what type of critical point this is, since I'm not sure we got the coordinates right!
    – Robert Lewis
    Jul 24 at 2:00






  • 1




    Just edited, but my question still stands. Thanks Robert!
    – obewanjacobi
    Jul 24 at 3:47










  • Which tools do you know to prove the existence of a cycle?
    – Did
    Jul 24 at 17:32










  • By the way: (2,4) a stable focus, are you sure about this?
    – Did
    Jul 24 at 17:34






  • 1




    According to Mathematica, the eigenvalues at $(2,4)$ are $frac13(1pm isqrt71)$, so $(2,4)$ is an unstable focus.
    – user539887
    Jul 24 at 19:40
















  • It appears to me that the "focus"--if it is a focus (I say this because I haven't checked, I'm going with what you wrote)--is at $(2, 4)$, not $(2, 3)$. This is why I'm not sure what type of critical point this is, since I'm not sure we got the coordinates right!
    – Robert Lewis
    Jul 24 at 2:00






  • 1




    Just edited, but my question still stands. Thanks Robert!
    – obewanjacobi
    Jul 24 at 3:47










  • Which tools do you know to prove the existence of a cycle?
    – Did
    Jul 24 at 17:32










  • By the way: (2,4) a stable focus, are you sure about this?
    – Did
    Jul 24 at 17:34






  • 1




    According to Mathematica, the eigenvalues at $(2,4)$ are $frac13(1pm isqrt71)$, so $(2,4)$ is an unstable focus.
    – user539887
    Jul 24 at 19:40















It appears to me that the "focus"--if it is a focus (I say this because I haven't checked, I'm going with what you wrote)--is at $(2, 4)$, not $(2, 3)$. This is why I'm not sure what type of critical point this is, since I'm not sure we got the coordinates right!
– Robert Lewis
Jul 24 at 2:00




It appears to me that the "focus"--if it is a focus (I say this because I haven't checked, I'm going with what you wrote)--is at $(2, 4)$, not $(2, 3)$. This is why I'm not sure what type of critical point this is, since I'm not sure we got the coordinates right!
– Robert Lewis
Jul 24 at 2:00




1




1




Just edited, but my question still stands. Thanks Robert!
– obewanjacobi
Jul 24 at 3:47




Just edited, but my question still stands. Thanks Robert!
– obewanjacobi
Jul 24 at 3:47












Which tools do you know to prove the existence of a cycle?
– Did
Jul 24 at 17:32




Which tools do you know to prove the existence of a cycle?
– Did
Jul 24 at 17:32












By the way: (2,4) a stable focus, are you sure about this?
– Did
Jul 24 at 17:34




By the way: (2,4) a stable focus, are you sure about this?
– Did
Jul 24 at 17:34




1




1




According to Mathematica, the eigenvalues at $(2,4)$ are $frac13(1pm isqrt71)$, so $(2,4)$ is an unstable focus.
– user539887
Jul 24 at 19:40




According to Mathematica, the eigenvalues at $(2,4)$ are $frac13(1pm isqrt71)$, so $(2,4)$ is an unstable focus.
– user539887
Jul 24 at 19:40










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Assume that all solutions starting in $mathbbR^2_+ := , (x, y) : x ge 0, y ge 0 ,$ are bounded for $t > 0$. It follows then that the domain of any such solution contains $[0, infty)$, and that the $omega$-limit set is compact and nonempty.



Let $L$ stand for the $omega$-limit set of some point, $(x_0, y_0)$, sufficiently close to the unstable focus $(2,4)$. By the Poincaré–Bendixson theorem, $L$ is either a limit cycle, or a heteroclinic cycle, (EDIT: or a homoclinic loop), or an equilibrium.



$L$ cannot be an equilibrium. Indeed, there are three possibilities: either $L = (0, 0)$, or $L = (6,0)$, or else $L = (2, 4)$. In the first two cases, the equilibria are saddles, so $(x_0, y_0)$ must belong to the stable manifold, which means either $, (0, y) : y > 0 ,$ or $, (x, 0) : x in (0, 6) cup (6, infty) ,$. In the third case, the only point whose $omega$-limit set is $(2,4)$ is $(2,4)$ itself.



We proceed now to excluding the case of heteroclinic cycle (EDIT: or homoclinic loop). But the only possible connection is from $(0, 0)$ to $(6,0)$, so there are no heteroclinic cycles.



Consequently, $L$ is a limit cycle surrounding $(2,4)$.



Below is a sketch of the phase portrait:



enter image description here



Incidentally, it is not so easy to show that all solutions starting in $mathbbR^2_+$ are bounded for positive times. The OP gave that as an assumption, but it should follow somehow from the form of the system.






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    1 Answer
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    up vote
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    down vote



    accepted










    Assume that all solutions starting in $mathbbR^2_+ := , (x, y) : x ge 0, y ge 0 ,$ are bounded for $t > 0$. It follows then that the domain of any such solution contains $[0, infty)$, and that the $omega$-limit set is compact and nonempty.



    Let $L$ stand for the $omega$-limit set of some point, $(x_0, y_0)$, sufficiently close to the unstable focus $(2,4)$. By the Poincaré–Bendixson theorem, $L$ is either a limit cycle, or a heteroclinic cycle, (EDIT: or a homoclinic loop), or an equilibrium.



    $L$ cannot be an equilibrium. Indeed, there are three possibilities: either $L = (0, 0)$, or $L = (6,0)$, or else $L = (2, 4)$. In the first two cases, the equilibria are saddles, so $(x_0, y_0)$ must belong to the stable manifold, which means either $, (0, y) : y > 0 ,$ or $, (x, 0) : x in (0, 6) cup (6, infty) ,$. In the third case, the only point whose $omega$-limit set is $(2,4)$ is $(2,4)$ itself.



    We proceed now to excluding the case of heteroclinic cycle (EDIT: or homoclinic loop). But the only possible connection is from $(0, 0)$ to $(6,0)$, so there are no heteroclinic cycles.



    Consequently, $L$ is a limit cycle surrounding $(2,4)$.



    Below is a sketch of the phase portrait:



    enter image description here



    Incidentally, it is not so easy to show that all solutions starting in $mathbbR^2_+$ are bounded for positive times. The OP gave that as an assumption, but it should follow somehow from the form of the system.






    share|cite|improve this answer



























      up vote
      1
      down vote



      accepted










      Assume that all solutions starting in $mathbbR^2_+ := , (x, y) : x ge 0, y ge 0 ,$ are bounded for $t > 0$. It follows then that the domain of any such solution contains $[0, infty)$, and that the $omega$-limit set is compact and nonempty.



      Let $L$ stand for the $omega$-limit set of some point, $(x_0, y_0)$, sufficiently close to the unstable focus $(2,4)$. By the Poincaré–Bendixson theorem, $L$ is either a limit cycle, or a heteroclinic cycle, (EDIT: or a homoclinic loop), or an equilibrium.



      $L$ cannot be an equilibrium. Indeed, there are three possibilities: either $L = (0, 0)$, or $L = (6,0)$, or else $L = (2, 4)$. In the first two cases, the equilibria are saddles, so $(x_0, y_0)$ must belong to the stable manifold, which means either $, (0, y) : y > 0 ,$ or $, (x, 0) : x in (0, 6) cup (6, infty) ,$. In the third case, the only point whose $omega$-limit set is $(2,4)$ is $(2,4)$ itself.



      We proceed now to excluding the case of heteroclinic cycle (EDIT: or homoclinic loop). But the only possible connection is from $(0, 0)$ to $(6,0)$, so there are no heteroclinic cycles.



      Consequently, $L$ is a limit cycle surrounding $(2,4)$.



      Below is a sketch of the phase portrait:



      enter image description here



      Incidentally, it is not so easy to show that all solutions starting in $mathbbR^2_+$ are bounded for positive times. The OP gave that as an assumption, but it should follow somehow from the form of the system.






      share|cite|improve this answer

























        up vote
        1
        down vote



        accepted







        up vote
        1
        down vote



        accepted






        Assume that all solutions starting in $mathbbR^2_+ := , (x, y) : x ge 0, y ge 0 ,$ are bounded for $t > 0$. It follows then that the domain of any such solution contains $[0, infty)$, and that the $omega$-limit set is compact and nonempty.



        Let $L$ stand for the $omega$-limit set of some point, $(x_0, y_0)$, sufficiently close to the unstable focus $(2,4)$. By the Poincaré–Bendixson theorem, $L$ is either a limit cycle, or a heteroclinic cycle, (EDIT: or a homoclinic loop), or an equilibrium.



        $L$ cannot be an equilibrium. Indeed, there are three possibilities: either $L = (0, 0)$, or $L = (6,0)$, or else $L = (2, 4)$. In the first two cases, the equilibria are saddles, so $(x_0, y_0)$ must belong to the stable manifold, which means either $, (0, y) : y > 0 ,$ or $, (x, 0) : x in (0, 6) cup (6, infty) ,$. In the third case, the only point whose $omega$-limit set is $(2,4)$ is $(2,4)$ itself.



        We proceed now to excluding the case of heteroclinic cycle (EDIT: or homoclinic loop). But the only possible connection is from $(0, 0)$ to $(6,0)$, so there are no heteroclinic cycles.



        Consequently, $L$ is a limit cycle surrounding $(2,4)$.



        Below is a sketch of the phase portrait:



        enter image description here



        Incidentally, it is not so easy to show that all solutions starting in $mathbbR^2_+$ are bounded for positive times. The OP gave that as an assumption, but it should follow somehow from the form of the system.






        share|cite|improve this answer















        Assume that all solutions starting in $mathbbR^2_+ := , (x, y) : x ge 0, y ge 0 ,$ are bounded for $t > 0$. It follows then that the domain of any such solution contains $[0, infty)$, and that the $omega$-limit set is compact and nonempty.



        Let $L$ stand for the $omega$-limit set of some point, $(x_0, y_0)$, sufficiently close to the unstable focus $(2,4)$. By the Poincaré–Bendixson theorem, $L$ is either a limit cycle, or a heteroclinic cycle, (EDIT: or a homoclinic loop), or an equilibrium.



        $L$ cannot be an equilibrium. Indeed, there are three possibilities: either $L = (0, 0)$, or $L = (6,0)$, or else $L = (2, 4)$. In the first two cases, the equilibria are saddles, so $(x_0, y_0)$ must belong to the stable manifold, which means either $, (0, y) : y > 0 ,$ or $, (x, 0) : x in (0, 6) cup (6, infty) ,$. In the third case, the only point whose $omega$-limit set is $(2,4)$ is $(2,4)$ itself.



        We proceed now to excluding the case of heteroclinic cycle (EDIT: or homoclinic loop). But the only possible connection is from $(0, 0)$ to $(6,0)$, so there are no heteroclinic cycles.



        Consequently, $L$ is a limit cycle surrounding $(2,4)$.



        Below is a sketch of the phase portrait:



        enter image description here



        Incidentally, it is not so easy to show that all solutions starting in $mathbbR^2_+$ are bounded for positive times. The OP gave that as an assumption, but it should follow somehow from the form of the system.







        share|cite|improve this answer















        share|cite|improve this answer



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        edited Aug 2 at 11:09


























        answered Jul 24 at 20:36









        user539887

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