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Libro de Resúmenes / Book of Abstracts (Español/English)

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Resumenes 84<br />

⎧dx<br />

⎛ x ⎞ qx<br />

⎪ = r⎜1<br />

− ⎟(<br />

x − m)<br />

x − y<br />

⎪ dt ⎝ K ⎠ x + a<br />

⎪<br />

X µ : ⎨<br />

⎪<br />

⎪dy<br />

⎛ y ⎞<br />

= s<br />

⎪ ⎜<br />

⎜1−<br />

⎟ y<br />

⎩ dt ⎝ n x ⎠<br />

7<br />

where ( , , , , , , ) + ℜ ∈<br />

= n s a b q K r µ and the parameters have different biological<br />

meanings. By means <strong>of</strong> a diffeomorphism (Chicone 1999, Guckenheimer<br />

and Holmes 1983), we make the study in the topologically equivalent<br />

system given by:<br />

⎧du<br />

2<br />

⎪ = ( ( 1−<br />

u)(<br />

u − M )( u + A)<br />

− v)<br />

u<br />

dτ<br />

⎪<br />

Yη<br />

: ⎨<br />

⎪ dv<br />

⎪ = B(<br />

u − v)(<br />

u + A)<br />

v<br />

⎩dτ<br />

We prove that the Allee effect produces a great modification in the behavior<br />

<strong>of</strong> May-Holling-Tanner mo<strong>de</strong>l, analysed in (Sáez and González-Olivares<br />

1999), where it was <strong>de</strong>monstrated the existence <strong>of</strong> two limit cycles<br />

surrounding the unique equilibrium point at the interior <strong>of</strong> the first<br />

quadrant, for a set <strong>of</strong> parameter values, showing that local stability does<br />

not imply global stability <strong>of</strong> the equilibrium point.<br />

In the mo<strong>de</strong>l studied here varied dynamics appear that are not<br />

topologically equivalent to the original one, for some we give the respective<br />

ecological interpretation. Among other results we have that:<br />

1. For any parameter values the singularity (0, 0) is a non-hyperbolic<br />

attractor (Chicone 1999, Guckenheimer and Holmes 1983), and (1,0) is an<br />

hyperbolic saddle point.<br />

2. There exists a set <strong>of</strong> parameter for which two equilibrium point in the<br />

interior <strong>of</strong> the first quadrant exists; also an unique or one having multiplicity<br />

two can exist.<br />

3. When we have an unique positive equilibrium point <strong>of</strong> multiplicity two, it<br />

occurs the codimension 2 saddle-no<strong>de</strong> bifurcation (Chicone 1999).<br />

4. When two positive equilibrium points exist one <strong>of</strong> them is always a<br />

hyperbolic saddle point and the nature <strong>of</strong> the other <strong>de</strong>pends on sign <strong>of</strong><br />

trace; in this case there exists an unique limit cycle obtained via Hopf<br />

bifurcation.<br />

System Yn is highly sensitive to initial conditions and as the origin is<br />

always an attractor the possibility <strong>of</strong> extinction <strong>of</strong> both populations is large<br />

<strong>de</strong>pending mainly on the predator-prey ratio.<br />

Referencias<br />

[1] Arrowsmith, D. K., Place, C. M. 1992. Dynamical System. Differential<br />

equations, maps and chaotic behaviour. Chapman and Hall.<br />

[2] Chicone C. 1999. Ordinary differential equations with applications, Text in<br />

Applied Mathematics 34, Springer.<br />

[3] Clark, C. W. 1990. Mathematical Bioeconomic: The optimal management <strong>of</strong><br />

renewable resources, (second edition). John Wiley and Sons.

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