Global Attractivity in a Nonlinear Difference Equation and Applications to a Biological Model

Similar documents
Global Attractivity in a Higher Order Difference Equation with Applications

Global Attractivity of a Higher-Order Nonlinear Difference Equation

Asymptotic Behavior of a Higher-Order Recursive Sequence

GLOBAL ATTRACTIVITY IN A NONLINEAR DIFFERENCE EQUATION

ON A DIFFERENCE EQUATION WITH MIN-MAX RESPONSE

Global Attractivity in a Higher Order Nonlinear Difference Equation

Stability In A Nonlinear Four-Term Recurrence Equation

OscillationofNonlinearFirstOrderNeutral Di erenceequations

ON THE STABILITY OF SOME SYSTEMS OF EXPONENTIAL DIFFERENCE EQUATIONS. N. Psarros, G. Papaschinopoulos, and C.J. Schinas

A System of Difference Equations with Solutions Associated to Fibonacci Numbers

ON THE OSCILLATION OF THE SOLUTIONS TO LINEAR DIFFERENCE EQUATIONS WITH VARIABLE DELAY

ON THE RATIONAL RECURSIVE SEQUENCE X N+1 = γx N K + (AX N + BX N K ) / (CX N DX N K ) Communicated by Mohammad Asadzadeh. 1.

Oscillation of second-order nonlinear difference equations with sublinear neutral term

On the Dynamics of a Rational Difference Equation, Part 1

Dynamics of a Rational Recursive Sequence

Global Attractivity of a Rational Difference Equation

Global Asymptotic Stability of a Nonlinear Recursive Sequence

Two Modifications of the Beverton Holt Equation

Dynamics of higher order rational difference equation x n+1 = (α + βx n )/(A + Bx n + Cx n k )

Oscillatory Behavior of Third-order Difference Equations with Asynchronous Nonlinearities

Oscillation Criteria for Delay and Advanced Difference Equations with General Arguments

The main objective of this work is to establish necessary and sufficient conditions for oscillations of (1.1), under the assumptions

Attractivity of the Recursive Sequence x n+1 = (α βx n 1 )F (x n )

Anna Andruch-Sobi lo, Ma lgorzata Migda. FURTHER PROPERTIES OF THE RATIONAL RECURSIVE SEQUENCE x n+1 =

Oscillation Criteria for Delay Neutral Difference Equations with Positive and Negative Coefficients. Contents

ON THE RECURSIVE SEQUENCE x n+1 = A x n. 1. Introduction Our aim in this paper is to establish that every positive solution of the equation

Pacific Journal of Mathematics

Global dynamics of two systems of exponential difference equations by Lyapunov function

Research Article Global Attractivity of a Higher-Order Difference Equation

The Fibonacci sequence modulo π, chaos and some rational recursive equations

Nonhyperbolic Dynamics for Competitive Systems in the Plane and Global Period-doubling Bifurcations

DYNAMICS AND BEHAVIOR OF HIGHER ORDER AND NONLINEAR RATIONAL DIFFERENCE EQUATION

Global Attractivity, Oscillations and Chaos in A Class of Nonlinear, Second Order Difference Equations

On the Third Order Rational Difference Equation

ON THE GLOBAL ATTRACTIVITY AND THE PERIODIC CHARACTER OF A RECURSIVE SEQUENCE. E.M. Elsayed

ARCHIVUM MATHEMATICUM (BRNO) Tomus 32 (1996), 13 { 27. ON THE OSCILLATION OF AN mth ORDER PERTURBED NONLINEAR DIFFERENCE EQUATION

A Note on the Positive Nonoscillatory Solutions of the Difference Equation

ON THE RATIONAL RECURSIVE SEQUENCE. 1. Introduction

Discrete Population Models with Asymptotically Constant or Periodic Solutions

Oscillation Criteria for Certain nth Order Differential Equations with Deviating Arguments

ON THE BEHAVIOR OF SOLUTIONS OF LINEAR NEUTRAL INTEGRODIFFERENTIAL EQUATIONS WITH UNBOUNDED DELAY

WEAK CONVERGENCE THEOREMS FOR EQUILIBRIUM PROBLEMS WITH NONLINEAR OPERATORS IN HILBERT SPACES

Asymptotic stability of solutions of a class of neutral differential equations with multiple deviating arguments

Necessary and Sufficient Conditions for Oscillation of Certain Higher Order Partial Difference Equations

Existence of Almost Periodic Solutions of Discrete Ricker Delay Models

Characterization of quadratic mappings through a functional inequality

Research Article On the Difference Equation x n 1 x n x n k / x n k 1 a bx n x n k

Research Article Asymptotic Behavior of the Solutions of System of Difference Equations of Exponential Form

Global Behavior of a Higher Order Rational Difference Equation

ASYMPTOTIC BEHAVIOR OF SOLUTIONS OF DISCRETE VOLTERRA EQUATIONS. Janusz Migda and Małgorzata Migda

Review Article Solution and Attractivity for a Rational Recursive Sequence

LOCAL STABILITY IMPLIES GLOBAL STABILITY IN SOME ONE-DIMENSIONAL DISCRETE SINGLE-SPECIES MODELS. Eduardo Liz. (Communicated by Linda Allen)

Discrete Halanay-type inequalities and applications

Two Rational Recursive Sequences

SOME FIXED POINT RESULTS FOR ADMISSIBLE GERAGHTY CONTRACTION TYPE MAPPINGS IN FUZZY METRIC SPACES

Research Article Global Attractivity and Periodic Character of Difference Equation of Order Four

ASYMPTOTIC BEHAVIOUR OF SECOND-ORDER DIFFERENCE EQUATIONS

M.ARCIERO, G.LADAS AND S.W.SCHULTZ

HOMEWORK ASSIGNMENT 6

ON GAP FUNCTIONS OF VARIATIONAL INEQUALITY IN A BANACH SPACE. Sangho Kum and Gue Myung Lee. 1. Introduction

Qualitative analysis of discrete nonlinear delay survival red blood cells model

Stability of a Class of Singular Difference Equations

Boundedness of solutions to a retarded Liénard equation

On Existence of Positive Solutions for Linear Difference Equations with Several Delays

GLOBAL DYNAMICS OF THE SYSTEM OF TWO EXPONENTIAL DIFFERENCE EQUATIONS

An iterative method for fixed point problems and variational inequality problems

Trichotomy of a system of two difference equations

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS

Initial value problems for singular and nonsmooth second order differential inclusions

Oscillation criteria for second-order half-linear dynamic equations on time scales

h(x) lim H(x) = lim Since h is nondecreasing then h(x) 0 for all x, and if h is discontinuous at a point x then H(x) > 0. Denote

Math 140A - Fall Final Exam

On The Convergence Of Modified Noor Iteration For Nearly Lipschitzian Maps In Real Banach Spaces

Positive Solutions of a Third-Order Three-Point Boundary-Value Problem

Research Article Global Stability and Oscillation of a Discrete Annual Plants Model

MULTIPLE POSITIVE SOLUTIONS FOR FOURTH-ORDER THREE-POINT p-laplacian BOUNDARY-VALUE PROBLEMS

INVARIANT CURVES AND FOCAL POINTS IN A LYNESS ITERATIVE PROCESS

Fixed point iteration Numerical Analysis Math 465/565

Invariants for Some Rational Recursive Sequences with Periodic Coefficients

MATH 202B - Problem Set 5

On a Fuzzy Logistic Difference Equation

On the stability of solutions of a system of differential equations

Math 328 Course Notes

Positive solutions of BVPs for some second-order four-point difference systems

Research Article Oscillation Criteria of Certain Third-Order Differential Equation with Piecewise Constant Argument

Research Article On Boundedness of Solutions of the Difference Equation x n 1 px n qx n 1 / 1 x n for q>1 p>1

Some Integral Inequalities with Maximum of the Unknown Functions

Convergence and Oscillation in a Rational Fourth Order Difference Equation

Disconjugate operators and related differential equations

Necessary and Sufficient Condition for Oscillation Solution of Nonlinear Second Order Difference Equations

Functions of several variables of finite variation and their differentiability

LYAPUNOV-RAZUMIKHIN METHOD FOR DIFFERENTIAL EQUATIONS WITH PIECEWISE CONSTANT ARGUMENT. Marat Akhmet. Duygu Aruğaslan

Journal of Inequalities in Pure and Applied Mathematics

Homework #2 Solutions Due: September 5, for all n N n 3 = n2 (n + 1) 2 4

Unconditional convergence of difference equations

Thai Journal of Mathematics Volume 14 (2016) Number 1 : ISSN

Stability of Adjointable Mappings in Hilbert

Properties of some nonlinear partial dynamic equations on time scales

FRACTAL GEOMETRY, DYNAMICAL SYSTEMS AND CHAOS

f(x) f(z) c x z > 0 1

Transcription:

International Journal of Difference Equations ISSN 0973-6069, Volume 9, Number 2, pp. 233 242 (204) http://campus.mst.edu/ijde Global Attractivity in a Nonlinear Difference Equation and Applications to a Biological Model Chuanxi Qian Mississippi State University Department of Mathematics and Statistics Mississippi State, MS 39762, USA qian@math.msstate.edu Abstract Consider the following difference equation of order k + x n+ = f(x n ) + g(x n k ), n = 0,,..., where f, g : [0, ) [0, ) are continuous functions, and k is a nonnegative integer. We establish a sufficient condition for the global attractivity of positive solutions of this equation. Our result can be applied to the following biological model e p qxn x n+ = ax2 n + c, n = 0,,..., p qxn b + x n + e where 0 < a <, b, c, p and q are positive constants, whose dynamics of solutions has been studied in [8] recently. A new global stability result for the positive solutions of this model is obtained, which is a significant improvement of the corresponding result obtained in [8]. AMS Subject Classifications: 39A0, 92D25. Keywords: Higher order difference equation, biological model, global attractivity, positive equilibrium. Introduction The dynamics of positive solutions of the difference equation x n+ = e p qxn ax2 n + c, n = 0,,..., (.) p qxn b + x n + e Received March 3, 204; Accepted June, 204 Communicated by Gerasimos Ladas

234 Chuanxi Qian where 0 < a <, b, c, p and q are positive constants, is studied in [8] recently. Eq. (.) is a biological model derived from the evaluation of a perennial grass [3]. The boundedness and the persistence of positive solutions, the existence, the attractivity and the global asymptotic stability of the unique positive equilibrium and the existence of periodic solutions have been discussed in [8]. Motivated by the work in [8], we study here the asymptotic behavior of positive solutions of the following general higher order difference equation x n+ = f(x n ) + g(x n k ), n = 0,,..., (.2) where f, g : [0, ) [0, ) are continuous functions with f nondecreasing and k is a nonnegative integer. Clearly, Eq. (.) is a special case of Eq. (.2) with f(x) = ax2 b + x, g(x) = c e p qx + e p qx and k = 0. In this paper, we will establish a sufficient condition for the global attractivity of positive solutions of Eq. (.2). In particular, by applying our result to Eq. (.), we will obtain a new result on the globally asymptotic stability of positive solutions of Eq. (.), which is a significant improvement of the corresponding result obtained in [8]. Because of its theoretical interest and many applications, the study of difference equations has become an active area of research, see, for example, [ 3] and references cited therein. Recently, the asymptotic behavior of positive solutions of the higher order difference equation x n+ x n = p n [f(x n k ) g(x n+ )], n = 0,,..., (.3) where k {0,,...}, f, g [[0, ), [0, )] with g nondecreasing, and {p n } is a nonnegative sequence, is studied and some global attractivity results are obtained in [7]. These results may be applied to several difference equations derived from mathematical biology. However, Eq. (.) can not be written in the form (.3) and so the results obtained in [7] cannot be applied to this case. 2 Main Results In this section, we establish a sufficient condition for the global attractivity of positive solutions of Eq. (.2). In the following discussion, we assume that Eq. (.2) has a unique positive equilibrium x, that is, x is the only positive solution of the equation n f(x) + g(x) = x. In addition, we adopt the notation a n = 0 whenever m > n. Theorem 2.. Assume that f(x) is nondecreasing and there is a positive number a < such that f(x) ax and f(x) ax is nonincreasing for x 0. Suppose also that (x x)(f(x) + g(x) x) < 0 for x > 0 and x x, (2.) i=m

Global Attractivity in a Nonlinear Difference Equation 235 and that g is L-Lipschitz with [ ] L <. Then every positive solution {x n } of Eq. (.2) converges to x as n. Proof. First, we show that {x n } is bounded. Otherwise, there is a subsequence {x ni } of {x n } such that x ni > max{x n : k n < n i }, i =, 2,..., and lim i x ni =. From Eq. (.2) we see that and so it follows that g(x ni k) + f(x ni ) x ni = f(x ni ) f(x ni ) 0 g(x ni k) x ni f(x ni ). (2.2) Since f(x) ax is nondecreasing, x f(x) is increasing. Then (2.2) yields Hence, g(x ni k) > x ni k f(x ni k ). f(x ni k) + g(x ni k ) x ni k > 0 which, in view of (2.), implies that x ni k < x. Then it follows that {g(x ni k )} is bounded which clearly contradicts (2.2) since x ni f(x ni ) x ni ax ni as i. Hence, {x n } must be bounded. Now, we are ready to show that x n x as n. First, we assume that {x n } is a nonoscillatory (about x) solution. Suppose that x n x is eventually nonnegative. The proof for the case that x n x is eventually nonpositive is similar and will be omitted. Let lim sup n x n = A. Then x A <. Clearly, it suffices to show that A = x. First, we assume that {x n } is nonincreasing eventually. Then lim x n = A. If A > x, n then by noting (2.), it follows from Eq. (.2) that x n+ x 0 = n (f(x i ) + g(x i k ) x i ) as n, i=0 which is a contradiction. Hence, A = x.

236 Chuanxi Qian Next, assume that {x n } is not eventually nonincreasing. Then, there is a subsequence {x nm } of {x n } such that Hence, it follows from Eq. (.2) that and so lim x n m = A and x nm > x m nm, m = 0,,.... g(x nm k) + f(x nm ) x nm = f(x nm ) f(x nm ) 0, m = 0,,..., Since x nm k x, and it follows that g(x nm k) x nm f(x nm ), m = 0,,.... (2.3) g(x nm k) + f(x nm k) x nm k 0 Hence, in view of (2.3) and (2.4), we see that g(x nm k) x nm k f(x nm k). (2.4) x nm k f(x nm k) x nm f(x nm ). By noting that x f(x) is increasing, we see that x nm k x nm which yields lim m x n m k = A. Then by taking limit on both sides of (2.3), we find that g(a) + f(a) A 0 which implies that A x. Hence, A = x. Finally, assume that {x n } is a solution of Eq. (.2) and oscillates about x. Let y n = x n x. Then {y n } satisfies y n+ = f(y n + x) f( x) + g(y n k + x) g( x), n = 0,,..., (2.5) and {y n } oscillates about zero. Since {x n } is bounded, there is a positive constant M such that y n = x n x M, n = 0,,.... Then by noting the Lipschitz property of g, we see that g(y n k + x) g( x) L y n k LM, n k. Let y l and y s be two consecutive members of the solution {y n } with N 0 < l < s such that y l 0, y s+ 0 and y n > 0 for l + n s. (2.6) Let y r = max{y l+, y l+2,..., y s } (2.7)

Global Attractivity in a Nonlinear Difference Equation 237 where y r is chosen as the first one to reach the maximum among y l+, y l+2... y s. We claim that r (l + ) k. (2.8) Suppose, for the sake of contradiction, that r (l + ) > k. Then, y r > y r k > 0. By noting y r k + x > x and (2.), we see that Since f(x) x is decreasing, g(y r k + x) + f(y r k + x) (y r k + x) < 0. (2.9) f(y r k + x) (y r k + x) > f(y r + x) (y r + x) and then it follows from (2.9) that However, on the other hand, (2.5) yields g(y r k + x) + f(y r + x) (y r + x) < 0. g(y r k + x) + f(y r + x) (y r + x) = f(y r + x) f(y r + x) 0 which contradicts (2.9). Hence, (2.8) holds. Now, observe that y n+y n = f(y n + x) f( x) ay n + g(y n k + x) g( x) and so it follows that y n+ a y n n+ a = n a [f(y n+ n + x) f( x) ay n ] + a [g(y n+ n k + x) g( x)]. Summing up from l to r, we see that y r a r y l a l = r and so ( y r = a r y l a + r l a [f(y r j+ j + x) f( x) ay j ] + a [f(y r j+ j + x) f( x) ay j ] + a j+ [g(y j k + x) g( x)] ) a [g(y j+ j k + x) g( x)] ( = a r y l a + l a [f(y r 2 l+ l + x) f( x) ay l ] + a [f(y j+ j + x) f( x) ay j ] ) + r a j+ [g(y j k + x) g( x)] ( = a r a [f(y l+ l + x) f( x)] + + r r 2 a [f(y j+ j + x) f( x) ay j ] ) a j+ [g(y j k + x) g( x)]. (2.0)

238 Chuanxi Qian Then by noting (2.6), f(x) is nondecreasing and f(x) ax is nonincreasing, we see that f(y l + x) f( x) 0 and f(y j + x) f( x) ay j 0, j = l +,..., r. Hence, it follow from (2.0) that and so r y r a r a [g(y j+ j k + x)) g( x))] [ ] y n LM, l n s. [ ] LM Since y l and y s are two arbitrary members of the solution with property (2.6), we see that there is a positive integer N N 0 such that y n [ ]ML, n N. Then, by a similar argument, it can be shown that there is a positive integer N N 0 such that y n [ ]ML, n N. Hence, there is a positive integer N N 0 such that [ ] y n LM, n N. (2.) Now, by noting the Lipschitz property of f(x) and (2.), we see that [ ] g(y n k + x) g( x) L y n k L 2 M, n N + k. Let y l and y s be two consecutive members of the solution {y n } with t 0 l < s such that (2.6) holds. Let y r be defined by (2.7). By a similar argument, we may show that (2.8) holds and ([ ] 2 y r L) M. Then it follows that y n ( [ ]L)2 M, l n s and so again by noting y l and y s are two arbitrary members of the solution with property (2.6), there is a positive integer N 2 N + k such tat y n ([ ]L)2 M, n N 2. Similarly, it can be shown that there is a positive integer N 2 N + K such that y n ([ ]L)2 M, n N 2. Hence, there is a positive integer N 2 N + k such that y n ([ ]L)2 M, n N 2. Finally, by induction, we find that for any positive integer m, there is a positive integer N m with N m as m such that ([ ] m y n L) M, n N m.

Global Attractivity in a Nonlinear Difference Equation 239 [ ] Then, by noting the hypotheses L <, we see that y n 0 as n, and so it follows that x n x as n. The proof is complete. 3 Applications Consider the difference equation x n+ = e p qx n k ax2 n + c, n = 0,,..., (3.) b + x n + e p qx n k where 0 < a <, b, c, p and q are positive constants, and k is a nonnegative integer. Eq. (3.) is in the form of (.2) with f(x) = ax2 b + x Clearly, f is increasing and f(x) ax. By noting we see that f(x) ax is decreasing. Let p qx e and g(x) = c + e. p qx (f(x) ax) = ab2 (b + x) < 0 2 e p qx F (x) = ax2 b + x + c x. + ep qx It is easy to check that F (0) > 0, lim x F (x) = and F (x) < 0. Hence, there is a unique positive number x such that F ( x) = 0, that is, Eq. (3.) has a unique positive equilibrium x, and Now, observe that (x x)(f(x) + g(x) x) < 0, x > 0 and x x. e p qx g (x) = cq ( + e p qx ) and 2 g (x) = cq 2 ep qx ( e p qx ). ( + e p qx ) 3 By noting that x = p q is the only point such that g (x) = 0, we see that g (x) takes maximum when x = p q and g ( p q ) = cq 4. Hence, g is L-Lipschitz with L = cq 4. Then by Theorem 2., we have that following conclusion immediately. Theorem 3.. Assume that [ ] cq 4 <. (3.2) Then every positive solution {x n } of Eq. (3.) tends to its positive equilibrium x as n.

240 Chuanxi Qian We claim that (3.2) is also a sufficient condition for the positive equilibrium x to be globally asymptotically stable when k = 0 or k =. In fact, when k = 0, (3.2) reduces to cq < 4 and the linearized equation of (3.) about the equilibrium x is ( ) a x 2 + 2ab x x n+ = cq x ( x + b) 2 ( + ) 2 n. (3.3) It is obvious that since By noting cq < 4, we see that a x 2 + 2ab x ( x + b) 2 a x 2 + 2ab x ( x + b) 2 cq ( + ) < 2 < x2 + 2b x ( x + b) 2 <. cq ( + ) < 4 2 ( + ) < + a x2 + 2ab x 2 ( x + b) 2 and so Hence, it follows that < a x2 + 2ab x ( x + b) 2 a x 2 + 2ab x ( x + b) 2 cq ( + ). 2 cq ( + ) 2 < and so the zero solution of Eq. (3.3) is asymptotically stable. By the linearization stability theory, the equilibrium x of Eq. (3.) is locally asymptoticly stable. Then by combining this fact and Theorem 3., we see that the equilibrium x of Eq. (3.) is globally asymptoticly stable. When k =, (3.2) reduces to cq < 4 and the linearized equation of (3.) about + a the equilibrium x is x n+ = a x2 + 2ab x ( x + b) 2 It is well known (see, for example [6]) for the linear equation x n cq ( + ) x n. (3.4) 2 y n+ + αy n + βy n = 0, where α and β are constants, a necessary and sufficient condition for the asymptotic stability is α < + β < 2.

Global Attractivity in a Nonlinear Difference Equation 24 Hence, by noting that under the condition cq < 4 + a, a x 2 + 2ab x ( x + b) 2 < + cq ( + ) < + 4 2 ( + ) 2, 2 we see that the zero solution of Eq. (3.4) is asymptoticly stable. Then it follows that the equilibrium x of Eq. (3.) is locally asymptotically stable, which together with Theorem 3. implies that x is globally asymptotically stable. Remark 3.2. In particular, when k = 0, Eq. (3.) reduces to the first order difference equation x n+ = ax2 n e p qxn + c, n = 0,,... (3.5) p qxn b + x n + e which is a biological model mentioned in Section. It has been shown in [8] that if cq < 2(), (3.6) then the positive equilibrium x of Eq. (3.5) is globally asymptotically stable. Clearly, our condition cq < 4 is a significant improvement of (3.6). References [] H. A. El-Morshedy and E. Liz, Convergence to equilibria in discrete population models, J. Diff. Equ. Appl. 2(2005), 7 3. [2] H. A. El-Morshedy and E. Liz, Globally attracting fixed points in higher order discrete population models, J. Math. Biol. 53(2006), 365 384. [3] J. R. Graef and C. Qian, Global stability in a nonlinear difference equation, J. Diff. Equ. Appl. 5(999), 25 270. [4] A. F. Ivanov, On global stability in a nonlinear discrete model, Nonlinear Anal. 23(994), 383 389. [5] G. Karakostas, Ch. G. Philos and Y. G. Sficas, The dynamics of some discrete population models, Nonlinear Anal. 7(99), 069 084. [6] V. L. Kocic and G. Ladas, Global Behavior of Nonlinear Difference Equations of Higher Order with Applications, Kluwer Academic Publishers, Dordrecht, 993. [7] S. Padhi and C. Qian, Global attractivity in a higher order nonlinear difference equation, Dyn. Contin. Discrete Impuls. Syst. 9(202), 95 06. [8] G. Papaschinopoulos, C. J. Schinas and G. Ellina, On the dynamics of the solutions of a biological model, J. Diff. Equ. Appl., to appear.

242 Chuanxi Qian [9] C. Qian, Global attractivity in a higher order difference equation with applications, Int. J. Qual. Theory Diff. Equ. Appl. (2007), 23 222. [0] C. Qian, Global attractivity in a higher order difference equation with variable coefficients, J. Diff. Equ. Appl. 8(202), 2 32. [] S. Stević, On positive solutions of a (k + ) th order difference equation, Appl. Math. Lett 9(2006), 427 43. [2] S. Stević, On a class of higher-order difference equations, Chaos Solutions Fractals 42(2009), 38 45. [3] D. Tilman and D. Wedin, Oscillations and chaos in the dynamics of a perennial grass, Nature 353(99), 653 655.