Abstract:Abstract. In this paper we developed an integrating factor matrix method to derive conditions for the existence of first integrals. We use this novel method to obtain first integrals, along with the conditions for their existence, for two and three dimensional Lotka-Volterra systems with constant terms. The results are compared to previous results obtained by other methods.
“…, x d ) a polynomial (usually though not always of degree 1 with constant term allowed). Results along this line include those of Cairó and co-workers [29][30][31][32], who in many cases used the classical technique of Darboux polynomials (DPs) [33]; and recent results based on an integrating factor technique [34]. In the case when d = 3 and a single first integral of a form similar to (1.2) is known to exist, there has been some work on the construction of a second, functionally independent first integral of a less algebraic form, involving a quadrature [35][36][37][38].…”
“…, x d ) a polynomial (usually though not always of degree 1 with constant term allowed). Results along this line include those of Cairó and collaborators (Cairó & Feix 1992;Cairó et al 1999;Cairó 2000;Cairó & Llibre 2000), who in many cases used the classical technique of Darboux polynomials (Goriely 2001); and results based on an integrating factor technique (Saputra et al 2010). When d = 3 and a single first integral of a form similar to (1.2) exists, there has been some work on the construction of a second, functionally independent first integral of a more complicated and less algebraic form (Grammaticos et al 1990;Goriely 1992;Gao 2000;Bustamante & Hojman 2003).…”
“…A d = 3 counterpart to their d = 2 analysis, which is lengthy, is not yet available. The many possible configurations of invariant planes have not been fully classified, though partial results have been obtained (Cairó 2000;Saputra et al 2010).…”
The general solutions of many three-dimensional Lotka-Volterra systems, previously known to be at least partially integrable, are constructed with the aid of special functions. Examples include certain ABC and May-Leonard systems. The special functions used are elliptic and incomplete beta functions. In some cases, the solution is parametric, with the independent and dependent variables expressed as functions of a 'new time' variable. This auxiliary variable satisfies a nonlinear third-order differential equation of a generalized Schwarzian type, and results of Carton-LeBrun on the equations of this type that have the Painlevé property are exploited, so as to produce solutions in closed form. For several especially difficult Lotka-Volterra systems, the solutions are expressed in terms of Painlevé transcendents. An appendix on incomplete beta functions and closed-form expressions for their inverses is included.
“…, x d ) a polynomial (usually though not always of degree 1 with constant term allowed). Results along this line include those of Cairó and co-workers [29][30][31][32], who in many cases used the classical technique of Darboux polynomials (DPs) [33]; and recent results based on an integrating factor technique [34]. In the case when d = 3 and a single first integral of a form similar to (1.2) is known to exist, there has been some work on the construction of a second, functionally independent first integral of a less algebraic form, involving a quadrature [35][36][37][38].…”
“…, x d ) a polynomial (usually though not always of degree 1 with constant term allowed). Results along this line include those of Cairó and collaborators (Cairó & Feix 1992;Cairó et al 1999;Cairó 2000;Cairó & Llibre 2000), who in many cases used the classical technique of Darboux polynomials (Goriely 2001); and results based on an integrating factor technique (Saputra et al 2010). When d = 3 and a single first integral of a form similar to (1.2) exists, there has been some work on the construction of a second, functionally independent first integral of a more complicated and less algebraic form (Grammaticos et al 1990;Goriely 1992;Gao 2000;Bustamante & Hojman 2003).…”
“…A d = 3 counterpart to their d = 2 analysis, which is lengthy, is not yet available. The many possible configurations of invariant planes have not been fully classified, though partial results have been obtained (Cairó 2000;Saputra et al 2010).…”
The general solutions of many three-dimensional Lotka-Volterra systems, previously known to be at least partially integrable, are constructed with the aid of special functions. Examples include certain ABC and May-Leonard systems. The special functions used are elliptic and incomplete beta functions. In some cases, the solution is parametric, with the independent and dependent variables expressed as functions of a 'new time' variable. This auxiliary variable satisfies a nonlinear third-order differential equation of a generalized Schwarzian type, and results of Carton-LeBrun on the equations of this type that have the Painlevé property are exploited, so as to produce solutions in closed form. For several especially difficult Lotka-Volterra systems, the solutions are expressed in terms of Painlevé transcendents. An appendix on incomplete beta functions and closed-form expressions for their inverses is included.
“…This type of dynamical systems occurs frequently in applications especially in the mathematical models for population biology [Jansen, 2001;Saputra et al, 2010a;De Witte et al, 2014] and for the spread of diseases [Chitnis et al, 2006;Llensa et al, 2014]. It is because in population models, if a species dies out it cannot be regenerated therefore it is always natural to have coordinate axes as the invariant manifold.…”
We investigate a dynamical system having a special structure namely a codimension-one invariant manifold that is preserved under the variation of parameters. We derive conditions such that bifurcations of codimension-one and of codimension-two occur in the system. The normal forms of these bifurcations are derived explicitly. Both local and global bifurcations are analyzed and yield the transcritical bifurcation as the codimension-one bifurcation while the saddle-node–transcritical interaction and the Hopf–transcritical interactions as the codimension-two bifurcations. The unfolding of this degeneracy is also analyzed and reveal global bifurcations such as homoclinic and heteroclinic bifurcations. We apply our results to a modified Lotka–Volterra model and to an infection model in HIV diseases.
“…Recently, there appear several papers about searching for inverse integrating factors of high order autonomous differential systems or using inverse integrating factors to study the systems. For example, in [14], the authors developed an integrating factor matrix method to derive conditions for the existence of first integrals, and used the method to study the integrability of two and three dimensional Lotka-Volterra systems with constant terms. We gave a method for deriving integrating factor by using invariant manifolds of system in [10].…”
The inverse integrating factor for some classes of higher order autonomous differential systems is studied in this paper. Some sufficient conditions on the existence of the inverse integrating factors of certain classes of n-th order autonomous differential systems are presented. Also, the explicit forms of the inverse integrating factors can be shown. Simultaneously, some related examples are given to illustrate the feasibility and the effectiveness of the proposed results.
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