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Reviewed document: A STUDY ON PERIODIC BOUNDARY VALUE PROBLEM.docx
Processing date: 19.5.2021 5:59 CEST
A total of 88 sentences were analysed. As a result 71 sentences (80,68%) were found in other documents.
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Reference documents
The following list contains titles and addresses of documents in which similar sentences were found. With a click on the number of found sentences („x Sentences”) the corresponding sentences are highlighted in the document as well as in the navigation bar by a colored border Another click on „x Sentences” resets the highlighting. By clicking on ✓ each source document can be hidden in the report so that they are not counted as similarities. The same applies to found sentences which may be marked as valid citations. A second click on the symbold reverts this process again.
46 Sentences were found in a text with the title: „PERIODIC BOUNDARY VALUE PROBLEM FOR ... - IRJMETS”, located at:✓
https://irjmets.com/rootaccess/forms/uploads/IRJMETS960448.pdf
20 Sentences were found in a text with the title: „Periodic boundary value problems for first-order impulsive difference equations with time delay”, located at:✓
https://doaj.org/article/44b36bdcf33443f193e93510ff509cbc
18 Sentences were found in a text with the title: „Periodic boundary value problems for first-order impulsive ...”, located at:✓
https://advancesindifferenceequations.springeropen.com/articles/10.1186/s13662-018-1539-5
https://link.springer.com/article/10.1186/s13662-018-1539-5
https://www.semanticscholar.org/paper/Periodic-boundary-value-problems-for-first-order-Tian-Wang/90f52c39b391149bd4d047e3711d6fe2e25e51e8
https://www.researchgate.net/journal/Advances-in-Difference-Equations-1687-1847/publication/323559736_Periodic_boundary_value_problems_for_first-order_impulsive_difference_equations_with_time_delay/links/5fc46bc5299bf104cf941a9d/Periodic-boundary-value-problems-for-first-order-impulsive-difference-equations-with-time-delay.pdf
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4 Sentences were found in a text with the title: „Periodic boundary value problems for first-order ... - X-MOL”, located at:✓
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2 Sentences were found in a text with the title: „Periodic boundary value problem for first-order impulsive ...”, located at:✓
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2 Sentences were found in a text with the title: „Monotone iterative technique for initial-value problems of ...”, located at:✓
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2 Sentences were found in a text with the title: „Impulsive Boundary Value Problems for First-order Ordinary ...”, located at:✓
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Subsequent the examined text extract:
A STUDY ON PERIODIC BOUNDARY VALUE PROBLEM FOR FIRST ORDER IMPULSIVE DIFFERENTIAL EQUATIONS AT VARIABLE TIME
Dr. R. SEENIVASAN.
Asst. Professor, Dept of Mathematical Economics, School of Economics, M.K.University, Madurai – 625 021.
see666@rediffmail.com
ABSTRACT:
This paper focuses on a certain type of periodic boundary value problems for first-order impulsive difference equations with time delay. Notions of lower and upper solutions are introduced, with which two new comparison theorems are established. Using Schaefer’s fixed point theorem, sufficient conditions for the existence and uniqueness of solutions to the corresponding linear problem of the boundary value problem are derived. By utilizing monotone iterative methods combined with the methods of lower and upper solutions, an existence theorem of extremal solutions to first-order impulsive difference equations with delay is obtained. These results extend some existing results in the literature. An interesting example is also given to verify the results obtained. This paper deals with existence results for a periodic boundary value problem and the corresponding initial value problem for first order impulsive differential equations at variable time.
Keywords: Difference equations , Time delay Periodic boundary value problem, Impulsive Differential equation.
INTRODUCTION:
While the previous chapter was devoted to ordinary differential equations and inclusions involving impulses, our attention in this chapter is turned to functional differential equations and inclusions each undergoing impulse effects. These equations and inclusions have played an important role in areas involving hereditary phenomena for which a delay argument arises in the modelling equation or inclusion. There are also a number of applications in which the delayed argument occurs in the derivative of the state variable, which are sometimes modelled by neutral differential equations or neutral differential inclusions. This chapter presents a theory for the existence of solutions of impulsive functional differential equations and inclusions, including scenarios of neutral equations, as well as semilinear models. The methods used throughout the chapter range over applications of the Leray-Schauder nonlinear alternative, Schaefer’s fixed point theorem, a Martelli fixed point theorem for multivalued condensing maps, and a Covitz-Nadler fixed point theorem for multivalued maps. There exist several papers about boundary value problems with impulsive effects at fixed points. Our aim consists in applying these principles and introducing some new results in this direction to develop the method of upper and lower solutions in order to find an existence result for the following periodic boundary value problem with impulses at variable times, Consider the periodic boundary value problem with impulses at variable times,
𝑢 ′ (t) = f (t, u (t)), t ϵ J, t ≠ γ (u (t)) --------------------(1)
u (t+) = u (t) + I (u (t)), t = γ (u (t)), ---------------------(2)
u (0) =u (T),--------------------------------------------------- (3)
where J = [0, T], f ϵ C (J x R, R), I ϵ C1 (R,R),
and γ ϵ C1 (R, R).
Periodic boundary value problems for first order functional differential equations with impulse
Mathematics of computing
Mathematical analysis
Numerical analysis
Numerical differentiation
Existence results for the initial value problem corresponding to Periodic boundary value problem The initial value problem corresponding to the periodic boundary value problem (1.1) – (1.3) is of the form
uˈ (t) = f (t, u (t)), t ≥ t0, t ≠ γ (u (t)) ------------------(1.1.1)
u (t+) = u (t) + I (u (t)), t = γ (u (t)), -------------------(1.1.2)
u (t0 +) = u0,---------------------------------------------- (1.1.3)
with (t0, u0) ϵ J x R.
Theorem 1.1.1.
Let α, β ϵ PC (J, R)
such that αˈ (t) ≤ f (t, α (t)), t ϵ J, t ≠ γ (α (t))----------------------- (1.1.4)
α (t+) ≤ α (t) + I (α (t)), t = γ (α (t))------------------------ (1.1.5)
and
βˈ (t) ≥ f (t, β (t)), t ϵ J, t ≠ γ (β (t))---------------------- (1.1.6)
β (t+) ≥ β (t) + I (β (t)), t = γ (β (t)).----------------------- (1.1.7)
Assume that the following conditions are satisfied:
(H0) γˈ (β (t)) βˈ(t) < 1, for all t ϵ J.
(H1) γˈ (x) f (t, x) < 1 for all t ϵ J. for all x ϵ R.
(H2) γ (x) is increasing and γ (α (0+)) > 0.
(H3) I* (x) = x + I (x) is increasing and (I*) ˈ (x) f (t, x) > f (t, I* (x)).
Then the solution u (t) of equation (4.1), (4.2) with u (0+) = u0 satisfies α (0+) ≤ u0 ≤ β (0+) implies
α (t) ≤ u (t) ≤ β (t), for all t ϵ J
Then α (t) ≤ u (t), for t ϵ J.
Proof:
The proof of the theorem is divided into two steps.
Step 1:
To prove α (0+) ≤ u0 implies α (t) ≤ u (t), for all t ϵ J.
Let α (t) and u (t) do not hit the curve σ: t = γ (x) for t ϵ (0, T).
Thus, we consider at least one of them meets σ.
Since γ is increasing and γ-1(0) < α (0+), α (t) hits the curve σ first.
Therefore there exists t1 ϵ (0, T) such that t1 = γ (α (t1)).
Using α (t) ≤ u (t) on (0, t1) and I (x) ≤ 0,
α (t1 +) ≤ α (t1) + I (α (t1))
≤ α (t1) ≤ u (t1).
To prove α (t) hits σ exactly once, let p (t) = t – γ (α (t)). If α (t1 +) = α(t1),
then γ (α (t1 +) = γ (α (t1)) = t1. (1.1.8)
Using the mean value theorem, there exists a point ζ ϵ (α (t1 +), α (t1)) such that γ (α (t1)) – γ (α (t1 + ) = γˈ (ζ ) [ α (t1) – α (t1 +) ] > 0.
This implies that p (t1) = t1 – γ (α (t1 +)) ≥ t1 – γ (α (t1 +)) ≥ t1 – t1 = 0 (using 1.1.8) Differentiating with respect to t pˈ(t) ≥ 1 – γˈ( α(t)) f (t, α(t)) > 0. (using H1) As a consequence, p (t) > 0, for all t > t1 Therefore, α (t) does not hit σ for t > t1. If u (t) ≠ γ (u (t)) for t ϵ J, using α (t1 + ) ≤ u (t1) and the comparison principle for ordinary differential equations α (t) ≤ u (t), for all t ϵ J.
Now assume that there exists t2 ϵ (t1, T) such that u (t2) = γ (u (t2)).
Since u (t1) ≥ α (t1 + ), it follows that α (t) ≤ u (t) for t ϵ (t1 t2).
To show that u (t2 +) = I*(u (t2)) ≥ α (t2), (1.1.9)
suppose that (1.1.9) is not true.
Since α (t1) ≤ u ( t1) and I* is increasing, α (t1 1) ≤ I* (α (t1)) ≤ I*(u (t1)).
Then there exists one point s ϵ (t1, t2) such that α(s) = I*(u (s))
and α (t) > I* (u (t)) for s < t ≤ t2.
Differentiating with respect to s
αˈ(s) ≥ (I*) ˈ(u (s)) uˈ(s)
= (I*)ˈ(u (s)) f (s, u (s))
> f (s, I*(u (s))) (using condition (H3))
= f (s, α (s)),
since α (s) = I*(u (s)).
But this is contradiction to αˈ (t) ≤ f (t, α (t)) and hence (1.1.9) follows.
Hence u (t) hits σ only for t = t2 and then α (t2 +) implies α (t) ≤ u (t)
for all t ϵ ( t2 , T).
Hence the proof of step one.
Step 2:
To prove β (0+) ≥ u0 implies β (t) ≥ u (t), for all t ϵ J. The proof of this step will follow the same procedure as in step one. The main difference is that the graph of the function β can meet the curve σ several times. It is easy to see that u (t) hits σ before than β (t).
Let t2 = γ (u (t2)).
u (0+) ≤ β (0+) implies u (t) ≤ β (t), for all t ϵ [ 0, t2].
But
u (t2 +) = u (t2) + I (u (t2)) (using (1.1.9))
≤ u (t2) ≤ β (t2). If β (t) does not hit σ,
then u (t2 +) ≤ β (t2) → u (t) ≤ β (t), for all t ϵ (t2, T].
Now assume that there exists one-point t3 ϵ (t2, T) such that t3 = γ (β (t3)).
Since u (t2 +) ≤ β (t2), u (t) ≤ β (t), for all t ϵ [t2, t3].
Using equations (4.1.6), (4.1.7), condition (H3) and the same arguments employed in step one it can be proved that β (t3 +) ≥ I* (β (t3)) ≥ u (t3).
This implies, u (t) does not meet σ for t > t3, but the condition (H1) does not assure the same for β (t).
Therefore, there are two possibilities:
β ( t3 +) < β (t3).
In this case, it is possible to prove that β (t) does not meet σ for t > t3 and
thus β (t3 +) ≥ u (t3) implies that β (t) ≥ u (t) for every t ϵ ( t3, T].
The proof of this assertion is very similar to the corresponding one in the first step, using
the condition (H0) instead of (H1).
β (t3 +) ≥ β (t3).
If β (t) does not hit σ for t > t3, then the proof is over.
suppose that there exists one-point t4 ϵ (t3, T) such that t4 = γ (β ( t4)).
In this case it follows that β (t) ≥ u (t) for all t ϵ (t3, t4) and it remains to show that I* (β (t4)) ≥ u (t4). For it, since I* is increasing, I* (β (t3 +)) ≥ I* (β (t3)) ≥ u (t3).
Suppose that I* (β (t4)) ≥ u (t4), using the condition (H3) and proceeding as in step one,
we get a contradiction.
Therefore, (β (t4 +)) ≥ I* (β (t4)) ≥ u (t4),
Employing the same procedures successively,
u (t) ≤ β (t) for all t ϵ J.
The proof is complete.
Result 1.1.1.
The conclusions of theorem (4.1.1) remain valid, for the function
γ ϵ C1 (R, (0, + ∞)), instead of assuming the condition γ (α ( 0+)) > 0.
Result 1.1.2.
The same arguments employed in the proof of theorem (1.1.1) permit us to show its validity when we consider several curves σk : t = γk (x), k = 1,2,…p and the corresponding impulses Ik satisfying the same conditions that γ and I satisfy respectively, together with the following assumptions,
γ k (x) < γ k+1 (x), k = 1,2,., p –1.
(ii) γ k+1 (I* (x)) > γ k (x), k = 1, 2,…, p –1.
Result 1.1.3.
Although condition (H0) may seem very restrictive to find the function β,
if β can be defined as β (t) = C, where C is a constant such that f (t, c) ≤ 0 on J,
then we have
(a) βˈ(t) = 0 ≥ f (t, β (t)).
(b) β (t+) = β (t) ≥ β (t) + I (β (t)), whenever I ϵ C1 ( R, Rˈ),
(c ) γˈ (β (t)) βˈ(t) = 0 < 1.
Theorem 1.1.2.
Let α, β ϵ PC (J, R) such that
αˈ(t) ≤ f ( t, α (t)), t ϵ J, t ≠ γ (α (t)) -----------------------(1.1.10)
αˈ(t+) ≤ α (t) + I (α(t)), t = γ (α (t))--------------------------- (1.1.11)
and
βˈ(t) ≥ f (t, β (t)), t ϵ J, t ≠ γ (β (t))---------------------------- (1.1.12)
βˈ(t+) ≥ β (t) + I (β (t)), t = γ (β (t)) ---------------------------(1.1.13)
Assume that the following conditions are satisfied:
(H0) γˈ (α (t)) αˈ(t) < 1, for all t ϵ J.
(H1) γˈ(x) f (t, x) < 1, for all t ϵ J, for all x ϵ R.
(H2) γ (x) is decreasing and γ (β ( 0+)) < 0.
(H3) I* (x) = x + I (x) is increasing and ( I*)ˈ(x) f (t, x) < f (t, I* (x)).
Then the solutions u (t) of (4.1), (4.2) with u (0+) = u0 satisfies
α (0+) ≤ u (0) ≤ β (0+) implies α (t) ≤ u(t) ≤ β(t), for all t ϵ J.
Proof:
Step 1:
To prove α (0+) ≤ u0 implies α (t) ≤ u (t), for all t ϵ J.
Let α (t) and u (t) do not hit the curve σ : t = γ (x) for t ϵ ( 0, T).
Then α (t) ≤ for t ϵ J.
Thus, we can consider at least one of them hits σ.
Since γ is decreasing and γ-1 (0) > α (0+), α (t) hits the curve σ first.
Therefore, there exists t1 ϵ (0, T) such that t1 = γ (α (t1)).
Using α (t) ≤ u (t) on (0, t1) and I (x) ≤ 0,
α (t1 +) ≤ α (t1) + I (α (t1)) ≤
α (t1) ≤ u (t1).
To prove α (t) hits σ exactly once, let p (t) = t – γ (α (t)).
If α (t1 +) ≤ α (t1), then γ (α (t1 +) = γ (α (t1)) = t1. (1.1.14)
Using the mean value theorem, there exists a point ξ ϵ (α (t1 +), α (t1)) Such that γ (α (t1)) – γ (α (t1 +)) = γˈ ( ϵ ) [α (t1) – α (t1 +) ] < 0. (1.1.15)
This implies that
p (t1) = t1 – γ (α (t1 +)) ≤ t1 – γ (α (t1))
≤ t1 – t1 = 0. (using (1.1.14))
Differentiating with respect to
t pˈ(t) ≥ 1 – γˈ(α (t)) f ( t, α (t)) > 0. (using condition H1)
As a consequence, p (t) > 0, for all t > t1.
Therefore α (t) does not hit σ for t > t1.
If u (t) ≠ γ (u (t)) for t ϵ J,
using α (t1 +) ≤ u (t1), and the comparison principle for ordinary differential equations α (t) ≤ u (t), for all t ϵ J.
Now assume that there exists t2 ϵ [t1, T] such that u (t2) = γ (u (t2)). Since u (t1) ≥ α (t1 +), it follows that α (t) ≤ u (t) for t ϵ (t1, t2). To show that u (t2 +) = I*(u (t2)) ≥ α (t2), (1.1.16)
suppose that (1.1.16) is not true.
Since α (t1) ≤ u (t1) and I* is decreasing
α (t1 +) ≤ I* (α (t1)) ≤ I* ( u (t1)).
Then there exists one point s ϵ (t1, t2) such that α (s) = I* (u (s)) and α (t) > I* (u (t)) for s < t ≤ t2. αˈ (s) ≥ (I*)ˈ ( u (s)) uˈ (s) = (I*)ˈ (u (s)) f (s, u (s)) > f (s, I* (u (s))) (using condition (H3)) = f (s, α (s)),
since α (s) =I* (u (s)).
But this is a contraction to αˈ(t) ≤ f (t, α (t)) and hence (1.1.16) follows.
Hence u (t) hits σ only for t = t2 and then α (t2) ≤ u (t2 +) implies α (t) ≤ u (t)
for all t ϵ [ t2, T].
Hence the proof of step one.
Step 2:
To prove β (0+) ≥ u0 implies β (t) ≥ u (t), for all t ϵ J.
The proof of this step will follow the same procedure as in step one.
The main difference is that the graph of the function β can meet the curve σ several times.
It is easy to see that u (t) hits σ before than β (t).
Let t2 = γ (u (t2)).
It follows that u (0+) ≤ β (0+) implies u (t) ≤ β (t), for all t ϵ [0, t2].
But, u (t2 +) = u (t2) + I (u (t2))
≤ u (t2) ≤ β (t2).
If β (t) does not hit σ, then u (t2 +) ≤ β (t2) ≤ β (t), for all t ϵ (t2, T].
Now assume that there exists one-point t3 ϵ [t2, T] such that t3 = γ (β (t3)).
Since u (t2 +) ≤ β (t2), then u (t) ≤ β (t), for all t ϵ [t2, t3].
Using (4.1.12), (4.1.13), condition (H3) and the same arguments employed in step one it can be proved that β (t3 +) ≥ I*( β (t3)) ≥ u (t3).
This implies that u (t) does not meet σ for t > t3, but the condition (H1) does not assure the same β (t).
Therefore, there are two possibilities:
β (t3 +) < β (t).
In this case, it is possible to prove that β (t) does not meet σ for t > t3, and thus β (t3 +) ≥ u (t3), implies that β (t) ≥ u (t) for every t ϵ (t3, T].
The proof of this assertion is very similar to the corresponding one in the first
step, using the condition (H0) instead of (H1). (b) β (t3 +) ≥ β (t3). If β (t) does not hit σ for t > t3, the proof is over. Suppose that there exists one point t4 ϵ (t3, T) such that t4 = γ (β (t4)). In this case, which implies that β (t) ≥ u (t) for all t ϵ (t3, t4) and it remains to prove that
I* (β (t4)) ≥ u (t4). For it, since I* is increasing,
I* (β (t3 +)) ≥ I* (β (t3)) ≥ u (t3).
Suppose that I* (β (t4)) < u (t4), using the condition (H3) and proceeding as in
step one, we get a contradiction.
Therefore, β (t4 +) ≥ I* (β (t4)) ≥ u (t4).
Employing the same procedures successively, u (t) ≤ β (t) for all t ϵ J.
Hence the proof.
CONCLUSION :
The theme of the paper is a study on periodic boundary value problems for first-order impulsive delay difference equations. It is well recognized that the theory of impulsive equations offers a general framework for the mathematical modeling of many real-world phenomena where the states undergo abrupt changes. Such equations have extensive applications in economics, dynamic systems, optimal control, medicine, population dynamics, and many other fields. In particular, in recent years, there has been an increasing interest in extending impulsive differential equations to time-delay systems and boundary value problems. On the other hand, difference equations play an important role in many fields such as numerous settings and forms, computing, electrical circuit analysis, biology, etc. However, there are not many related results for impulsive difference equations and impulsive delay difference equations. These motivated us to work on the present topic.
In this paper, we studied impulsive delay difference equations with periodic boundary conditions. Based on the new concepts of lower and upper solutions, we established two new comparison principles. With these, we constructed monotone sequences from a corresponding linear equation and established the existence of extremal solutions by utilizing the monotone iterative technique. An example was given to illustrate the results obtained. It is reckoned that these results may play an important role in the theory of difference equations, and are useful in many practical problems in the aforesaid fields.
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