Abstract
We investigate the nonautonomous difference equation with real initial conditions and coefficients which are in general functions of n and/or the state variables , and satisfy . We also obtain some global results about the behavior of solutions of the nonautonomous non-homogeneous difference equation where are functions of n and/or the state variables , with . Our results are based on the explicit formulas for solutions. We illustrate our results by numerous examples.
JEL Classification:
AMS 2010 Mathematics Subject Classification: 39A10; 39A20; 39A30
1. Introduction
We investigate the global behavior of the second order difference equation
where the functions , are such that
Here, the functions are in general functions of n and/or the state variables . So Equation (1) is indeed a nonautonomous equation. It can also be an equation of order higher than two. As we have shown in [1] if , then the zero equilibrium of Equation (1) is globally asymptotically stable, and if , then the zero equilbrium of Equation (1) is stable. Furthermore, as we have shown in [1], if , where r is a constant independent of n and the state variables, then Equation (1) has unbounded solutions. Thus, the most interesting case is when condition (2) is satisfied. This case was addressed in [1] for the general k-th order difference equation, and some attractivity results of the equilibrium solutions were given there. However, a restriction that was imposed. Similar results were obtained in [2] where attractivity results of the periodic solutions were obtained.
When Equation (1) is a linear equation with constant coefficients, condition (2) implies that we have the non-hyperbolic case since would be a characteristic root. In general, difference equations can be very sensitive to any kind of perturbations in the non-hyperbolic case as we can see from the following two examples:
Example 1.
Consider the difference equation
Starting with the two initial conditions we obtain the corresponding solution to be . The limiting case of Equation (3), as , is the equation
where every non-constant solution is the period-two solution .
Example 2.
Consider the difference equation
Starting with two initial conditions we obtain the corresponding solution to be . The limiting case of Equation (4), as , is the equation
where every non-constant solution is given as:
Thus the limiting equation has all solutions asymptotic to .
Example 3.
The following two difference equations
and
where , which have respective linearizations
and
with the condition (2) satisfied, possible models in population dynamics as all transition functions are Holling type functions, see [3] for further references.
There are many ways that a general second order difference equation of the form
where f is a real function from to , can be transformed into the linearized form (1). See [1,2,4] for linearization methods based on algebraic manipulations and especially [5] for symmetries based methods.
The linear Equation (1) can also be used to obtain generalized identities which can be used to study the behavior of the solutions of the difference equation, see [1,2]. Identities are the building blocks of semicycle analysis, method of invariants and rate of convergence. See [4,6,7,8,9,10,11,12,13,14].
We also extend our investigation to the second order nonautonomous non-homogeneous difference equation
where and are real valued functions which depend on n and satisfy condition (2).
The technique which will be used to obtain our results is based on the explicit formulas for the solutions of Equations (1) and (7). These formulas are of independent interest and can be used in a variety of situations.
We illustrate our results with several examples.
2. Invariants
Our first result gives a connection between Equation (1) under the condition (2) and the existence of an invariant.
Lemma 1.
Proof.
Second, assume that Equation (1) has an invariant of the form . Then the following relation must be satisfied
If is not a constant for all , then . Thus
Since by condition (2) for all then Equation (1) becomes
which by substitution in Equation (9) gives
and so for all .
Note that the invariant must hold for every solution of Equation (1) including the infinite number of constant solutions . Thus for all , so is a constant for . ☐
Remark 1.
The restriction that and are constants is a severe restriction, yet the obtained invariant can be useful. This invariant will be used to reduce the order of difference Equation (1) resulting in first order linear difference equation which is solvable. See Proposition 1 and Corollary 2.
Lemma 1 can be extended to any three term difference equation of the form
where and such that with
Lemma 2.
Proof.
Then Equation (12) is an invariant. Indeed
Second, assume that Equation (12) is an invariant of Equation (10). If is not a constant for all , then is a function of n that is, . Then Equation (10) with condition (11) becomes
and implies that for
Therefore for all , which completes the proof. ☐
3. Representation of Solutions
Next we give some basic results on the representation of the solutions of Equation (13). These results have importance of their own and have straight-forward extensions to the difference equations in linear normed spaces.
Lemma 3.
Consider the difference equation
where and are real valued functions for , . Then for
- (a)
- where by definition when ;
- (b)
- where by definition when .
Proof.
Set , in Equation (13). We obtain:
which is a first order linear nonautonomous non-homogeneous difference equation whose solution is
From Lemma 3 we can obtain an explicit formula for the solution of the difference Equation (7) where and are real valued functions which depend on n and satisfy condition (2). For convenience of notation set and at . Taking into account that Equation (7) becomes
By Lemma 3 part (b) with we get that for
and so for
4. Main Results
In this section we present our main results. Consider Equation (7) where the function , in which case Equation (7) becomes
Remark 2.
Theorem 1.
Let and assume that . Assume that either or for some .
- (1)
- Suppose that for .
- (a)
- If and for , then ;
- (b)
- If and for , then ;
- (2)
- Suppose that for and converges.
- (3)
- Suppose that for all , and let .
- (4)
- Suppose that for finite number of
- (5)
- Suppose that for .
- (6)
- Suppose that for . Assume that for eitherorThen every solution of Equation (18) is unbounded.
Proof.
For convenience of notation set and at each . For let be the sum of positive terms and let be the sum of negative terms.
- (1)
- Suppose that for . Then for . By Lemma 3 part (b) we get that forIf for some , then let N be the first such that . Then forObserve that for and for . Thus for and for .
- (a)
- Assume that and . Then for
Thus as .- (b)
- Assume that and . Then for
Thus as . - (2)
- Suppose that for and converges. Then for . By Lemma 3 (b) with we have that forObserve that for , . Hence the series converges by the comparison test for series to the limiting value.
- (a)
- If for , then converges to a limit as . Now assume that for . Observe that for and for any , such that we have the following:
When is odd, thenWhen is even, thenHence for and for any , such that andand so forThus the seriesconverges by comparison test and so converges to a finite limit.- (b)
- Assume that for . Then there exists such that . From part (a) we have that for ,
Then for , andand soIf , thenThus for .Now assume that . From part (a) (with ) we have that forThus for .Thus forand so every solution is bounded. - (3)
- Suppose that for all . Then Equation (18) becomes , and so , from which (a), (b) and (c) follow.
- (d)
- Let and assume that for and . Equation (18) gives for ,
- (4)
- Suppose that for finite number of . By Lemma 3 part (b) with we get thatLet be the first n such that and let , be the last such that . Then .
- (5)
- Suppose that for all . Then Equation (18) becomes . Thus for
- (a)
- If for all , then and for .
- (b)
- If , then as . If , then as .
- (c)
- If converges and converges, then and converge as .
- (6)
- Suppose that for all . Then for all . From Lemma 3 part (b) with we get that forObserve that for and for any fixed N. Let N be the first such that . Suppose that N is even. Then for we have thatFor
- (a)
- Assume that . Then for
Thus as .- (b)
- Assume that . Then for
Thus as .Now suppose that N is odd. Then for we have thatFor- (a)
- Assume that . Then for
Thus as .- (b)
- Assume that . Then for
Thus as . ☐
Example 4.
The difference equation
where , when rewritten as
satisfies all conditions of Theorem 1 part (2a) when , that is and and so every solution of Equation (21), when converges to a limit point.
In addition, Equation (21) implies
which shows that when (resp. ) the solution is increasing (resp. decreasing) and so it has to have a finite or infinite limit.
Suppose that . Assume that and . Then and so there exists such that for . Thus for
Therefore by Theorem 1 part (2a) .
Now suppose that . Assume that such that . Then and so for . Thus by Theorem 1 part (1a) .
In some very special cases of the terms in Equation (18) one can obtain results not included in Theorem 1. We illustrate this with the following result.
Theorem 2.
Consider the difference equation
where such that for all . Let . Then every solution of Equation (24) is unbounded provided one of the following holds:
- (1)
- Assume that and either , where or , where for ;
- (2)
- Assume that for .
- (a)
- Suppose that for all eitherand or and ;
- (b)
- Suppose that for all eitherand or and .
Proof.
First we rewrite Equation (24) in the form
Let (resp. ) be the sum of positive (resp. negative) terms.
- (1)
- Assume that for . Setting Lemma 3 part (b) implies forSince for , then the series converges as .If for and , thenThus as .If for and , thenThus as .
- (2)
- Assume that for .
- (a)
- By Lemma 3 part (b) with we get that for
Observe that the series converges by the alternating series test.If and , then forThus as .If and , then forThus as .- (b)
- By Lemma 3 part (b) with we get that for
If and , then forThus as .If and , then forThus as . ☐
Remark 3.
In Theorem 1 cases (2) and (6) the existence of r is a sufficient condition but not a necessary condition. To show this for case (2) consider Equation (3) where . Since as , there is no r such that . Rewriting Equation (3) as
we find its solution as
which converges to a constant.
Now for the case (5), consider the difference equation
Clearly as and there is no r such that .
Example 5.
Consider the following equation
where is a real sequence, which depends on n and on one or more state variables . An immediate application of Theorem 1 with , leads to the following result for Equation (26). Here r is a positive constant.
Corollary 1.
The global behavior of Equation (26) is as follows:
- (a)
- If for , then every non-constant solution of Equation (26) is unbounded.
- (b)
- If for , then every non-constant solution of Equation (26) converges to a limit.
- (c)
- If for all , then .
- (d)
- If for a finite number of , then every solution of Equation (26) is eventually equal to a constant.
- (e)
- If for , then every non-constant solution of Equation (26) is a period-two solution.
- (f)
- If for , then every non-constant solution of Equation (26) is unbounded.
In the case when Equation (1) has periodic coefficients it can be reduced to an associated system of second order equations with constant coefficients which can be solved. We illustrate this case by the Example 6.
Example 6.
Consider the following second order equation
where and for all . Assume that and are period-two sequences, that is
A straight-forward simplification leads to the following autonomous system for even and odd indexed terms:
Let . Then Equation (27) is equivalent with the autonomous equation
In view of Lemma 1 and Theorem 1, we have the following result.
Proposition 1.
Consider Equation (27) with period-two coefficients where and for all . Then
Proof.
By Theorem 1 with , we have
Now by using Equation (17), Lemma 1 and Theorem 1 we can obtain explicitly the behavior of the solutions of Equation (1) when and are periodic and condition (2) is satisfied.
Corollary 2.
Let and let , . Consider Equation (27) where for all and that
- (a)
- If either or , then every non-constant solution of Equation (27) is unbounded.
- (b)
- If , then every non-constant solution of Equation (27) is periodic of period . In particular, the periodic solution is whereand .
- (c)
- If , then every non-constant solution of Equation (27) converges to a limit, that is
Proof.
Then for
Indeed for , we have that for
Now from Equation (29) when we have that for
Now continuing this process we get that for
Observe that since for , then
Similarly, we can show that for
For let . Then for , and . Thus for Equation (34) becomes
- (a)
- (b)
- (c)
- Suppose that . Then by Theorem 1 part (2), where and , every non-constant solution of Equation (35) converges to a limit point. Let for . Then by Lemma 1
Thus for
and so for
Then for and after simplifying terms we obtain
It should be noticed that by using Equation (37) and the initial conditions we also get Equation (38) for the cases . Thus for
Since all subsequences have the same limit, we finally obtain the formula for the limit. ☐
Example 7.
Consider the difference equation
where
Assume that and . Then the solution of Equation (40) is periodic of period 5, that is the solution is
Thus from Corollary 2 we obtain the following:
Remark 4.
The same idea applies to Equation (15) with . For example, if there exists a constant r such that and , then the solutions of Equation (15) will converge to a limit even though there may be some for some . Since Equation (15) is used extensively to obtain our results, the behavior of the solutions of Equations (1), (17), (18) and (24) will depend on the product of the coefficients rather than the individual coefficients.
If for some , then the solution of Equation (27) eventually becomes constant as the following result shows.
Theorem 3.
Suppose that for all and for some . Let N be the first k such that . Then the solution of Equation (27) eventually becomes a constant. More precisely for
5. Conclusions
In this paper we consider the general nonautonomous second order difference Equation (1) where the functions satisfy condition (2). The condition (2) implies the existence of an invariant which then reduces Equation (1) to the first order nonautonomous difference equation such as Equation (13) which has closed form solution (14). Using the closed form solution we were able to obtain the global behavior of solutions of some nonautonomous second order difference equations, such as Equation (26). The different types of asymptotic dynamics that the general nonautonomous second order difference Equation (1) exhibits are either convergence to a constant or a to a period-two sequence, divergence to , or eventual equality to a constant or a period-two sequence. Some results are given for the case when the coefficients of Equation (1) are periodic sequences when one can reduce the dynamics to the autonomous case, but our technique here was based on explicit solutions formula, see Example 6. The presented results have potential to be extended to systems of difference equations.
Author Contributions
Both authors contributed equally in the writing of this article.
Conflicts of Interest
The authors declare no conflict of interest.
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