New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations

New efficient conditions are obtained sufficient for the solvability as well as unique solvability of a nonlocal boundary-value problem for nonlinear functional differential equations. Отримано новi ефективнi умови розв’язностi, а також єдиної розв’язностi нелокальних граничних задач для нелiнiйних...

Повний опис

Збережено в:
Бібліографічні деталі
Опубліковано в: :Нелінійні коливання
Дата:2008
Автор: Oplustil, Z.
Формат: Стаття
Мова:Англійська
Опубліковано: Інститут математики НАН України 2008
Онлайн доступ:https://nasplib.isofts.kiev.ua/handle/123456789/178203
Теги: Додати тег
Немає тегів, Будьте першим, хто поставить тег для цього запису!
Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations / Z. Oplustil // Нелінійні коливання. — 2008. — Т. 11, № 3. — С. 365-386. — Бібліогр.: 12 назв. — англ.

Репозитарії

Digital Library of Periodicals of National Academy of Sciences of Ukraine
_version_ 1859610667085987840
author Oplustil, Z.
author_facet Oplustil, Z.
citation_txt New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations / Z. Oplustil // Нелінійні коливання. — 2008. — Т. 11, № 3. — С. 365-386. — Бібліогр.: 12 назв. — англ.
collection DSpace DC
container_title Нелінійні коливання
description New efficient conditions are obtained sufficient for the solvability as well as unique solvability of a nonlocal boundary-value problem for nonlinear functional differential equations. Отримано новi ефективнi умови розв’язностi, а також єдиної розв’язностi нелокальних граничних задач для нелiнiйних функцiонально-диференцiальних рiвнянь.
first_indexed 2025-11-28T11:17:51Z
format Article
fulltext UDC 517.9 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR FUNCTIONAL DIFFERENTIAL EQUATIONS* ЗНОВI УМОВИ РОЗВ’ЯЗНОСТI НЕЛОКАЛЬНИХ ГРАНИЧНИХ ЗАДАЧ ДЛЯ НЕЛIНIЙНИХ ФУНКЦIОНАЛЬНО-ДИФЕРЕНЦIАЛЬНИХ РIВНЯНЬ Z. Opluštil Inst. Math. Technická 2, 616 69 Brno, Czech Republic e-mail: oplustil@fme.vutbr.cz New efficient conditions are obtained sufficient for the solvability as well as unique solvability of a nonlocal boundary-value problem for nonlinear functional differential equations. Отримано новi ефективнi умови розв’язностi, а також єдиної розв’язностi нелокальних гра- ничних задач для нелiнiйних функцiонально-диференцiальних рiвнянь. 1. Introduction and notation. On the interval [a, b], we consider the functional differential equation u′(t) = F (u)(t), (1) where F : C([a, b]; R) → L([a, b]; R) is a continuous (in general) nonlinear operator. As usual, by a solution of this equation we understand an absolutely continuous function u : [a, b] → R satisfying the equality (1) almost everywhere on [a, b].Along with the equation (1), we consider the nonlocal boundary condition h(u) = ϕ(u), (2) where h : C([a, b]; R) → R is a (non-zero) linear bounded functional and ϕ : C([a, b]; R) → R is a continuous (in general) nonlinear functional. The question on the solvability of various types of initial and boundary-value problems for functional differential equations and their systems is a classical topic in the theory of differential equations (see, e.g., [1 – 11] and references therein). There is a lot of interesting general results but only a few efficient conditions is known, namely, in the case where the boundary condition considered is nonlocal. In [12], we studied the question on the unique solvability of the problem (1), (2) in the linear case, i.e., in the case where the operator F is linear and ϕ ≡ Const. We found out that it is very useful to consider the boundary condition (2) as a nonlocal perturbation of the two-point condition u(a)− λu(b) = ϕ(u) (3) ∗ Published results were acquired using the subsidization of the Ministry of Education, Youth and Sports of the Czech Republic, research plan MSM 0021630518 “Simulation modelling of mechatronic systems”. c© Z. Opluštil, 2008 ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 365 366 Z. OPLUŠTIL with λ ∈ R. In this paper, the results stated in [3] concerning the problem (1), (3) are gen- eralized, and new efficient conditions are thus found sufficient for the solvability and unique solvability of the problem (1), (2). The following notation is used in the sequel. 1. R is the set of all real numbers, R+ = [0,+∞[. 2. C([a, b]; R) is the Banach space of continuous functions v : [a, b] → R with the norm ‖v‖C = max {|v(t)| : t ∈ [a, b]}. 3. C([a, b]; R+) = {u ∈ C([a, b]; R) : u(t) ≥ 0 for t ∈ [a, b]}. 4. L([a, b]; R) is the Banach space of Lebesgue integrable functions p : [a, b] → R with the norm ‖p‖L = ∫ b a |p(s)| ds. 5. L([a, b]; R+) = { p ∈ L([a, b]; R) : p(t) ≥ 0 for almost all t ∈ [a, b] } . 6.Lab is the set of linear operators ` : C([a, b]; R) → L([a, b]; R) for which there is a function η ∈ L([a, b]; R+) such that |`(v)(t)| ≤ η(t)‖v‖C for a.e. t ∈ [a, b] and all v ∈ C([a, b]; R). 7.Pab is the set of operators ` ∈ Lab transforming the setC([a, b]; R+) into the setL([a, b]; R+). 8. Fab is the set of linear bounded functionals h : C([a, b]; R) → R. 9. PFab is the set of functionals h ∈ Fab transforming the set C([a, b]; R+) into the set R+. 10. Bi hc = {u ∈ C([a, b]; R) : (−1)i+1h(u)sgn ( (2 − i)u(a) + (i − 1)u(b) ) ≤ c}, where h ∈ Fab, c ∈ R, i = 1, 2. 11. K([a, b]×A;B), where A,B ⊆ R, is the set of function f : [a, b]×A → B satisfying the Carathéodory conditions, i.e., f(·, x) : [a, b] → B is a measurable function for all x ∈ A, f(t, ·) : A → B is a continuous function for almost every t ∈ [a, b], and for every r > 0 there exists qr ∈ L([a, b]; R+) such that |f(t, x)| ≤ qr(t) for a.e. t ∈ [a, b] and all x ∈ A, |x| ≤ r. 2. Main results. As it was said above, the boundary condition (2) is considered as a non-local perturbation of the two-point condition (3). Therefore, we assume in the sequel that the linear functional h appearing in (2) is defined by the formula h(v) = u(a)− λv(b)− h0(v) + h1(v) for v ∈ C([a, b]; R), (4) where λ > 0 and h0, h1 ∈ PFab. Moreover, the following assumptions are used: (H1) F : C([a, b]; R) → L([a, b]; R) is a continuous operator such that the relation sup { |F (v)(·)| : v ∈ C([a, b]; R), ‖v‖C ≤ r } ∈ L([a, b]; R+) is satisfied for every r > 0. (H2) ϕ : C([a, b]; R) → R is a continuous functional such that the condition sup { |ϕ(v)| : v ∈ C([a, b]; R), ‖v‖C ≤ r } < +∞ holds for every r > 0. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 367 Before formulation of the main results we introduce the following notation. Having λ > 0 and h ∈ Fab, we put α(λ, h) = ( 1− h(1) ) min { 1, 1 λ } , (5) β(λ, h) = ( λ− h(1) ) min { 1, 1 λ } . (6) Moreover, for any functional h given by the formula (4), we define the function ω0(· ;h) by setting ω0(x;h) =  ( x+ 1 λh0(1) )( 1− h0(1) ) 1− h0(1)− x − ( 1 λ h1(1) + 1− λ λ ) if λ ≤ 1, ( 1− λ+ h1(1) ) x < ( 1− h(1) )( 1− h0(1) ) ,( x+ h0(1) )( 1− h0(1) ) 1− h0(1)− x − ( h1(1) + 1− λ ) if λ ≤ 1, ( 1− λ+ h1(1) ) x ≥ ( 1− h(1) )( 1− h0(1) ) ,( x+ λ− 1 + h0(1) )( 1− h0(1) ) 1− h0(1)− λx − h1(1) if λ > 1, λh1(1)x < ( 1− h(1) )( 1− h0(1) ) , ( x+ λ−1 λ + 1 λh0(1) )( 1− h0(1) ) 1− h0(1)− λx − 1 λ h1(1) if λ > 1, λh1(1)x ≥ ( 1− h(1) )( 1− h0(1) ) . In this section, we formulate all the results, the proofs are postponed till Section 5 below. Theorem 1. Let c ∈ R+, the assumptions (H1) and (H2) be satisfied, and let the functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ PFab are such that h(1) ≥ 0, (7) h0(1) < 1, h1(1) ≤ λ. (8) Let, moreover, the condition ϕ(v)sgn v(a) ≤ c for v ∈ C([a, b]; R) (9) be fulfilled and there exist `0, `1 ∈ Pab (10) such that, on the set B1 hc([a, b]; R), the inequality( F (v)(t)− `0(v)(t) + `1(v)(t) ) sgn v(t) ≤ q(t, ‖v‖C) for a.e. t ∈ [a, b] (11) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 368 Z. OPLUŠTIL holds, where the function q ∈ K([a, b]× R+; R+) satisfies lim x→+∞ 1 x b∫ a q(s, x) ds = 0. (12) If, in addition, ‖`0(1)‖L < α(λ, h0), (13) ω0(‖`0(1)‖L;h) < ‖`1(1)‖L < 2 √ α(λ, h0)− ‖`0(1)‖L − h1(1)min { 1, 1 λ } (14) then the problem (1), (2) has at least one solution. Theorem 2. Let c ∈ R+, the assumptions (H1) and (H2) be satisfied, and let the functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ PFab satisfy the relations (7) and (8). Let moreover, the condition ϕ(v)sgn v(b) ≥ −c for v ∈ C([a, b]; R) be fulfilled and there exist `0, `1 ∈ Pab such that, on the set B2 hc([a, b]; R), the inequality( F (v)(t)− `0(v)(t) + `1(v)(t) ) sgn v(t) ≥ −q(t, ‖v‖C) for a.e. t ∈ [a, b] holds, where the function q ∈ K([a, b]× R+; R+) satisfies (12). If, in addition, ‖`1(1)‖L < β(λ, h1) (15) and α(λ, h0) β(λ, h1)− ‖`1(1)‖L − 1 < ‖`0(1)‖ < < 2 √ β(λ, h1)− ‖`0(1)‖L − h0(1)min { 1, 1 λ } (16) then the problem (1), (2) has at least one solution. Now we establish theorems concerning the unique solvability of the problem (1), (2). Theorem 3. Let the assumptions (H1) and (H2) be satisfied and a functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ PFab satisfy the relations (7) and (8). Let, moreover, the condition ( ϕ(v)− ϕ(w) ) sgn ( v(a)− w(a) ) ≤ 0 for v, w ∈ C([a, b]; R) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 369 be fulfilled and there exist `0, `1 ∈ Pab such that, on the set B1 hc([a, b]; R) with c = |ϕ(0)|, the inequality( F (v)(t)− F (w)(t)− `0(v − w)(t) + `1(v − w)(t) ) sgn ( v(t)− w(t) ) ≤ 0 for a.e. t ∈ [a, b] holds. If, in addition, the conditions (13) and (14) are fulfilled then the problem (1), (2) is uniquely solvable. Theorem 4. Let the assumptions (H1) and (H2) be satisfied and the functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ PFab satisfy the relations (7) and (8). Let, moreover, the condition ( ϕ(v)− ϕ(w) ) sgn ( v(b)− w(b) ) ≥ 0 for v, w ∈ C([a, b]; R) be fulfilled and there exist `0, `1 ∈ Pab such that, on the set B2 hc([a, b]; R) with c = |ϕ(0)|, the inequality( F (v)(t)− F (w)(t)− `0(v − w)(t) + `1(v − w)(t) ) sgn ( v(t)− w(t) ) ≥ 0 for a.e. t ∈ [a, b] holds. If, in addition, the conditions (15) and (16) are fulfilled then the problem (1), (2) is uniquely solvable. Remark 1. Let the functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ ∈ PFab. Define the operator ψ : L([a, b]; R) → L([a, b]; R) by setting ψ(z)(t) df= z(a+ b− t), t ∈ [a, b], for an arbitrary z ∈ L([a, b]; R). Let ω be the restriction of ψ to the space C([a, b]; R), and F̂ (z)(t) df= −ψ ( F (ω(z)) ) (t) for a.e. t ∈ [a, b] and all z ∈ C([a, b]; R), ĥ(z) df= z(a)− 1 λ z(b) + 1 λ h0 ( ω(z) ) − 1 λ h1 ( ω(z) ) for z ∈ C([a, b]; R), ϕ̂(z) df= − 1 λ ϕ(ω(z)) for z ∈ C([a, b]; R). It is not difficult to verify that if u is a solution to the problem (1), (2) then the function v df= ω(u) is a solution to the problem v′(t) = F̂ (v)(t), ĥ(v) = ϕ̂(v), (17) and vice versa, if v is a solution to the problem (17) then the function u df= ω(v) is a solution to the problem (1), (2). Therefore, using the above transformation, we can immediately derive conditions for the solvability and unique solvability of the problem (1), (2) in the case where h(1) ≤ 0 (we do not formulate them here in detail). ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 370 Z. OPLUŠTIL 3. An example. As an example, on the interval [0, 1], we consider the integro-differential equation u′(t) = d cos(2πt) 1∫ 0 u(τ(s))√ s ds− g1(t)u(t)eu 2(ω(t)) + g2(t)|u(t)|ν (18) subjected to the nonlocal boundary condition u(0) = 1 2 u(1) + k 1∫ 0 sin(2πs)u(s) ds− u(0)eu(1/4) + arctg u ( 1 2 ) , (19) where d, k ∈ R+, ν ∈ [0, 1[, g1, g2 ∈ L([0, 1]; R), and τ, ω : [0, 1] → [0, 1] are measurable functions. Theorem 1 yields the following corollary. Corollary 1. Let the function g1 be nonnegative on [0, 1] and the numbers d and k satisfy k ≤ π 2 , d < π − k 2 , (20) and (d+ k)(π − k) π − k − 2d − ( k + π 2 ) < d < 2 √ π(π − k − 2d)− k 2 . (21) Then the problem (18), (19) has at least one solution. 4. Auxiliary propositions. The main results are proved using a lemma on a priory estimate stated in [6] by Kiguradze and Půža. This lemma can be formulated as follows. Lemma 1 ([6], Corollary 2). Let there exist a positive number ρ and an operator ` ∈ Lab such that homogeneous problem u′(t) = `(u)(t), h(u) = 0 (22) has only the trivial solution, and, for every δ ∈ ]0, 1[, an arbitrary function u ∈ C̃([a, b]; R) satisfying the relations u′(t) = `(u)(t) + δ[F (u)(t)− `(u)(t)] for a.e. t ∈ [a, b], h(u) = δϕ(u) (23) admits the estimate ‖u‖C ≤ ρ. (24) Then the problem (1), (2) has at least one solution. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 371 Definition 1. Let i ∈ {1, 2}, h ∈ Fab. We say that an operator ` ∈ Lab belongs to the set Ui(h), if there exists r > 0 such that, for arbitrary q∗ ∈ L([a, b]; R+) and c ∈ R+, every function u ∈ C̃([a, b]; R) satisfying the inequalities (−1)i+1h(u)sgn ( (2− i)u(a) + (i− 1)u(b) ) ≤ c, (25) (−1)i+1 ( u′(t)− `(u)(t) ) sgnu(t) ≤ q∗(t) for a.e. t ∈ [a, b] (26) admits the estimate ‖u‖C ≤ r(c+ ‖q∗‖L). (27) Lemma 2. Let i ∈ {1, 2}, c ∈ R+, the assumptions (H1) and (H2) be satisfied, and (−1)i+1ϕ(v)sgn ( (2− i)v(a) + (i− 1)v(b) ) ≤ c for v ∈ C([a, b]; R). (28) Let, moreover, there exist ` ∈ Ui(h) such that, on the set Bi hc([a, b]; R), the inequality (−1)i+1 ( F (v)(t)− `(v)(t) ) sgn v(t) ≤ q(t, ‖v‖C) for a.e. t ∈ [a, b] (29) is fulfilled. Then the problem (1), (2) has at least one solution. Proof. First note that, due to the condition ` ∈ Ui(h), the homogeneous problem (22) has only the trivial solution. Let r be the number appearing in Definition 1. According to (12), there exists ρ > 2rc such that 1 x b∫ a q(s, x) < 1 2r for x > ρ. Now assume that a function u ∈ C̃([a, b]; R) satisfies (23) for some δ ∈ ]0, 1[. Then, according to (28), u satisfies inequality (25), i.e., u ∈ Bi hc([a, b]; R). By (29), we obtain that inequality (26) is fulfilled with q∗ ≡ q(· , ‖u‖C). Hence, by virtue of the condition ` ∈ Ui(λ) and the definition of the number ρ, we get the estimate (24). Since ρ depends neither on u nor on δ, it follows from Lemma 1 that the problem (1), (2) has at least one solution. Lemma 3. Let i ∈ {1, 2}, the assumptions (H1) and (H2) be satisfied, and let the relation (−1)i+1 ( ϕ(u1)− ϕ(u2) ) sgn ( (2− i)(u1(a)− u2(a)) + (i− 1)(u1(b)− u2(b)) ) ≤ 0 (30) hold for every u1, u2 ∈ C([a, b]; R). Let, moreover, there exist ` ∈ Ui(λ) such that, on the set Bi hc([a, b]; R) with c = |ϕ(0)|, the inequality (−1)i+1 ( F (u1)(t)− F (u2)(t)− `(u1 − u2)(t) ) sgn ( u1(t)− u2(t) ) ≤ 0 (31) is fulfilled for a.e. t ∈ [a, b]. Then the problem (1), (2) is uniquely solvable. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 372 Z. OPLUŠTIL Proof. It follows from the condition (30) that the inequality (28) is fulfilled, where c = = |ϕ(0)|. Using (31), we get that, on the set Bi hc([a, b]; R), the inequality (29) holds, where q ≡ ≡ |F (0)|. Consequently, all the assumptions of Lemma 2 are fulfilled, and thus the problem (1), (2) has at least one solution. It remains to show that problem (1), (2) has at most one solution. Let u1, u2 be arbitrary solutions of the problem (1), (2). Put u(t) = u1(t) − u2(t) for t ∈ ∈ [a, b]. Then, by virtue of (30) and (31), we get u1, u2 ∈ Bi hc([a, b]; R) and (−1)i+1h(u)sgn ( (2− i)u(a) + (i− 1)u(b) ) ≤ 0, (−1)i+1 ( u′(t)− `(u)(t) ) sgnu(t) ≤ 0 for a.e. t ∈ [a, b]. The last relations, together with the assumption ` ∈ Ui(λ), result in u ≡ 0. Consequently, u1 ≡ u2. Lemma 4. Let the functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ ∈ PFab satisfy the conditions (7) and (8). Let, moreover, the operator ` admit the representation ` = `0−`1, where `0 and `1 are such that the conditions (10), (13), and (14) hold. Then ` belongs to the set U1(h). Proof. Let c ∈ R+, q∗ ∈ L([a, b]; R+), and u ∈ C̃([a, b]; R) satisfy (25) and (26) with i = 1. We shall show that (27) holds, where r depends only on ‖`0(1)‖L, ‖`1(1)‖L, λ, h0(1), and h1(1). It is clear that u′(t) = `0(u)(t)− `1(u)(t) + q̃(t) for a.e. t ∈ [a, b], (32) where q̃(t) = u′(t)− `(u)(t) for a.e. t ∈ [a, b]. (33) From (25) and (26) we get( u(a)− λu(b)− h0(u) + h1(u) ) sgnu(a) ≤ c (34) and q̃(t)sgnu(t) ≤ q∗(t) for a.e. t ∈ [a, b]. (35) First suppose that u does not change its sign. Put M = max {|u(t)| : t ∈ [a, b]}, m = min{|u(t)| : t ∈ [a, b]} (36) and choose t1, t2 ∈ [a, b] such that t1 6= t2 and |u(t1)| = M, |u(t2)| = m. (37) It is clear that M ≥ 0, m ≥ 0, and either t1 < t2 (38) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 373 or t1 > t2. (39) Moreover, according to (10), (35), and (36), from (32) we obtain |u(t)|′ ≤ M `0(1)(t)−m`1(1)(t) + q∗(t) for a.e. t ∈ [a, b]. (40) If u(a) = 0 then m = 0 and the integration of (40) from a to t1, on account of (37), yields M ≤ M t1∫ a `0(1)(s) ds+ t1∫ a q∗(s) ds. By virtue of (13), it follows from the last inequality that ‖u‖C = M ≤ r0(‖q∗‖+ c), where r0 = [1− ‖`0(1)‖L]−1. Consequently, the estimate (27) holds with r = r0. If u(a) 6= 0 then, according to (34), we obtain |u(a)| ≤ λ|u(b)|+ h0(|u|)− h1(|u|) + c, and thus |u(a)| − |u(b)| ≤ h0(|u|)− h1(|u|) + |u(b)|(λ− 1) + c (41) and |u(a)| − |u(b)| ≤ 1 λ h0(|u|)− 1 λ h1(|u|) + |u(a)|λ− 1 λ + c λ . (42) Let first (38) hold. Then the integration of (40) from a to t1 and from t2 to b results in M − |u(a)| ≤ M t1∫ a `0(1)(s) ds+ t1∫ a q∗(s) ds, |u(b)| −m ≤ M b∫ t2 `0(1)(s) ds+ b∫ t2 q∗(s) ds. Summing two last inequalities, we get M −m+ |u(b)| − |u(a)| ≤ M ∫ J `0(1)(s) ds+ ∫ J q∗(s) ds, (43) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 374 Z. OPLUŠTIL where J = [a, t1] ∪ [t2, b]. Let λ ≤ 1. Taking into account (10) and (41), we obtain from (43) that M −m− h0(|u|) + h1(|u|)− |u(b)|(λ− 1)− c ≤ M b∫ a `0(1)(s) ds+ b∫ a q∗(s) ds. From the last inequality, according to (36), we get M(1− h0(1))−m(λ− h1(1))− c ≤ M‖`0(1)‖L + ‖q∗‖L. Due to (7), the last inequality implies (M −m)(1− h0(1)) ≤ M‖`0(1)‖L + ‖q∗‖L + c. (44) Let λ > 1. From (43), in view of (7), (42), and (36), it follows that 1 λ (M −m)(1− h0(1))− c ≤ M‖`0(1)‖L + ‖q∗‖L, which, together with (44), yields min { 1, 1 λ } (M −m)(1− h0(1)) ≤ M‖`0(1)‖L + ‖q∗‖L + c. Now suppose that (39) is fulfilled. Then the integration of (40) from t2 to t1, on account of (10) and (36), yields min { 1, 1 λ } (M −m)(1− h0(1))− c ≤ M −m ≤ M‖`0(1)‖L + ‖q∗‖L. Therefore, in both cases (38) and (39), the inequality min { 1, 1 λ } (M −m)(1− h0(1)) ≤ M‖`0(1)‖L + ‖q∗‖L + c (45) holds. On the other hand, the integration of (40) from a to b, yields |u(b)| − |u(a)| ≤ M‖`0(1)‖L −m‖`1(1)‖L + ‖q∗‖L. (46) Now we shall divide the discussion into the following four cases: Case (a): λ ≤ 1 and (1− λ+ h1(1))‖`0(1)‖L < (1− h(1))(1− h0(1)). Using (42) and (36) in (46), we get m ≤ M(h0(1) + λ‖`0(1)‖L) + c+ λ‖q∗‖L λ‖`1(1)‖L + h1(1)− λ+ 1 . ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 375 On the other hand, (45) implies M(1− h0(1)− ‖`0(1)‖L) ≤ m(1− h0(1)) + c+ ‖q∗‖L. (47) Hence, on account of the first inequality in (14), we have ‖u‖C = M ≤ r1(c+ ‖q∗‖L)(λ‖`1(1)‖L + h1(1)− h0(1)− λ+ 2), where r1 = [ (1− h0(1)− ‖`0(1)‖L)(λ‖`1(1)‖L + h1(1)− λ+ 1)× × (−(1− h0(1))(h0(1) + λ‖`0(1)‖L)) ]−1 > 0, and thus the estimate (27) holds, where r is defined by r = r1(λ‖`1(1)‖L + h1(1)− h0(1)− λ+ 2). Case (b): λ ≤ 1 and (1−λ+h1(1))‖`0(1)‖L ≥ (1−h(1))(1−h0(1)). As above, (45) implies (47). If we use the estimate (41) in (46), according to (36), we obtain m ≤ M(h0(1) + ‖`0(1)‖L) + c+ ‖q∗‖L ‖`1(1)‖L + h1(1)− λ+ 1 . From the last inequality, the first inequality in (14), and (47) we get ‖u‖C = M ≤ r2(c+ ‖q∗‖L)(‖`1(1)‖L + h1(1)− h0(1)− λ+ 2), where r2 = [ (1− h0(1)− ‖`0(1)‖L)(‖`1(1)‖L + h1(1)− λ+ 1)× × (−(1− h0(1))(h0(1) + ‖`0(1)‖L)) ]−1 > 0, and thus the estimate (27) holds, where r is defined by r = r2(λ‖`0(1)‖L + h1(1)− h0(1)− λ+ 2). Case (c): λ > 1 and λh1(1)‖`0(1)‖L < (1−h(1))(1−h0(1)). From (46), in view of (41), and (36), it follows that m ≤ M(h0(1) + ‖`0(1)‖L + λ− 1) + c+ ‖q∗‖L ‖`1(1)‖L + h1(1) . On the other hand from the (45) we have M(1− h0(1)− λ‖`0(1)‖L) ≤ m(1− h0(1)) + λ(c+ ‖q∗‖L). (48) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 376 Z. OPLUŠTIL Hence, on account of (14), the relation ‖u‖C = M ≤ r3(c+ ‖q∗‖L)(λ‖`1(1)‖L + λh1(1) + 1− h0(1)), is satisfied, where r3 = [ (1− h0(1))(‖`1(1)‖L + h1(1)− h0(1)− λ+ 1− ‖`0(1)‖L)× × (−λ‖`0(1)‖L(h1(1) + ‖`1(1)‖L)) ]−1 > 0, and thus the estimate (27) holds, where r is defined by r = r3(λ‖`1(1)‖L + λh1(1) + 1− h0(1)). Case (d): λ > 1 and λh1(1)‖`0(1)‖L ≥ (1 − h(1))(1 − h0(1)). As above, (45) yields (48). If we use estimate (42) in (46), according to (36), we obtain m ≤ M(h0(1) + λ‖`1(1)‖L + λ− 1) + c+ λ‖q∗‖L λ‖`1(1)‖L + h1(1) . From the last inequality and (48), in view of (14), it follows that ‖u‖C = M ≤ r4λ(c+ ‖q∗‖L)(λ‖`1(1)‖L + h1(1) + 1− h0(1)), where r4 = [ (1− h0(1)− λ‖`0(1)‖L)(λ‖`1(1)‖L + h1(1))× × (−(λ‖`0(1)‖L + λ− 1 + h0(1))(1− h0(1))) ]−1 > 0, and thus the estimate (27) holds, where r is defined by r = r4λ(λ‖`1(1)‖L + h1(1) + 1− h0(1)). Therefore, in all cases (a) – (d), the estimate (27) holds. Now suppose that u changes its sign. Put M = max{u(t) : t ∈ [a, b]}, m = −min{u(t) : t ∈ [a, b]} (49) and choose tM , tm ∈ [a, b] such that u(tM ) = M, u(tm) = −m. (50) Obviously, M > 0, m > 0, and either tm < tM (51) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 377 or tm > tM . (52) First suppose that (51) holds. It is clear that there exists α2 ∈ ]tm, tM [ such that u(t) > 0 for α2 < t ≤ tM , u(α2) = 0. (53) Let α1 = inf{t ∈ [a, tm] : u(s) < 0 for t ≤ s ≤ tm}. Obviously, u(t) < 0 for α1 < t ≤ tm and u(α1) = 0 if α1 > a. (54) Put α3 = { b, if u(b) ≥ 0, inf{t ∈ ]tM , b] : u(s) < 0 for t ≤ s ≤ b}, if u(b) < 0. It is clear that if α3 < b then u(t) < 0 for α3 < t ≤ b, u(α3) = 0. (55) The integration of (32) from α1 to tm, from α2 to tM , and from α3 to b, in view of (10), (35), (49), (50), and (53) – (55), yields u(α1) +m ≤ m tm∫ α1 `0(1)(s) ds+M tm∫ α1 `1(1)(s) ds+ tm∫ α1 q∗(s) ds, (56) M ≤ M tM∫ α2 `0(1)(s) ds+m tM∫ α2 `0(1)(s) ds+ tM∫ α2 q∗(s) ds, (57) u(α3)− u(b) ≤ m b∫ α3 `0(1)(s) ds+M b∫ α3 `1(1)(s) ds+ b∫ α3 q∗(s) ds. (58) If u(b) ≥ 0 or u(a) ≥ 0 then, according to (34), (49), (54), and the assumption λ > 0, we obtain u(α1) ≥ −c−mh0(1)−Mh1(1), and thus from (56) we find −c−mh0(1)−Mh1(1) +m ≤ ≤ max {1, λ} m tm∫ α1 `0(1)(s) ds+M tm∫ α1 `1(1)(s) ds+ tm∫ α1 q∗(s) ds . ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 378 Z. OPLUŠTIL Hence, min { 1, 1 λ }( −c−mh0(1)−Mh1(1) +m ) ≤ ≤ m ∫ J `0(1)(s) ds+M ∫ J `1(1)(s) ds+ ∫ J q∗(s) ds, (59) where J = [α1, tm] ∪ [α3, b]. Let u(b) < 0 and u(a) < 0.Multiplying both sides of (58) by λ and taking (55) into account, we get −λu(b) ≤ λ m b∫ α3 `0(1)(s) ds+M b∫ α3 `1(1)(s) ds+ b∫ α3 q∗(s) ds  . Summing the last inequality and (56), according to (34), (49), and (54), we can verify that the inequality (59) is fulfilled, where J = [α1, tm] ∪ [α3, b]. From (57) and (59) we get M(1− C1) ≤ mA1 + ‖q∗‖L + c, (60) m(α(λ, h0)−D1) ≤ M ( B1 + h1(1)min { 1, 1 λ }) + ‖q∗‖L + c, (61) where A1 = tM∫ α2 `1(1)(s) ds, B1 = ∫ J `1(1)(s) ds and C1 = tM∫ α2 `0(1)(s) ds, D1 = ∫ J `0(1)(s) ds. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 379 Due to (13), it is clear that C1 < 1 and D1 < α(λ, h0). Consequently, (60) and (61) imply 0 < M(1− C1)(α(λ, h0)−D1) ≤ ≤ A1 [ M ( B1 + min { 1, 1 λ } h1(1) ) + ‖q∗‖L + c ] + (‖q∗‖L + c)(α(λ, h0)−D1) ≤ ≤ MA1 ( B1 + min { 1, 1 λ } h1(1) ) + (‖q∗‖L + c)(1 + ‖`1(1)‖L), (62) 0 < m(α(λ, h0)−D1)(1− C1) ≤ ≤ ( B1 + min { 1, 1 λ } h1(1) ) (mA1 + ‖q∗‖L + c) + c+ ‖q∗‖L ≤ ≤ mA1 ( B1 + min { 1, 1 λ } h1(1) ) + (‖q∗‖L + c)(1 + h1(1) + ‖`1(1)‖L). Obviously, (1− C1)(α(λ, h0)−D1) ≥ α(λ, h0)− (C1 +D1) ≥ α(λ, h0)− ‖`0(1)‖L > 0 and 4A1 ( B1 + min { 1, 1 λ } h1(1) ) ≤ ( A1 +B1 + min { 1, 1 λ } h1(1) )2 ≤ ≤ ( ‖`1(1)‖L + min { 1, 1 λ } h1(1) )2 . By the last inequalities and the second inequality in (14), from (62) we get M ≤ r5(‖`1(1)‖L + 1)(‖q∗‖L + c), m ≤ r5(‖`1(1)‖L + 1 + h1(1))(‖q∗‖L + c), where r5 = ( α(λ, h0)− ‖`0(1)‖L − (‖`1(1)‖L + min{1, 1 λ}h1(1))2 4 )−1 . Consequently, the estimate (27) holds, where r is given by r = r5(‖`1(1)‖L + 1 + h1(1)). If (52) holds, the validity of the estimate (27) can be proved analogously. The lemma is proved. Lemma 5. Let the functional h be defined by the formula (4), where λ > 0 and h0, h1 ∈ ∈ PFab satisfy the conditions (7) and (8). Let, moreover, the operator ` admit the representation ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 380 Z. OPLUŠTIL ` = `0−`1, where `0 and `1 are such that the conditions (10), (15), and (16) hold. Then ` belongs to the set U2(h). Proof. Let c ∈ R+, q ∗ ∈ L([a, b]; R+), and u ∈ C̃([a, b]; R) satisfy (25) and (26) with i = 2, i.e., h(u)sgnu(b) ≥ −c and ( u′(t)− `(u)(t) ) sgnu(t) ≥ −q∗(t) for a.e. t ∈ [a, b]. We shall show that (27) holds, where r depends only on ‖`0(1)‖L, ‖`1(1)‖L λ, h0(1), and h1(1). Obviously, u satisfies (32), where q̃ is defined by (33). Clearly, −q̃(t) sgnu(t) ≤ q∗(t) for a.e. t ∈ [a, b] (63) and (−u(a) + λu(b) + h0(u)− h1(u)) sgnu(b) ≤ c. (64) First suppose that u does not change its sign. Define numbers M and m by (36) and choose t1, t2 ∈ [a, b] such that t1 6= t2 and (37) is fulfilled. Obviously, M ≥ 0, m ≥ 0, and either (38) or (39) holds. Moreover, according to (10), (36), and (63), from (32) we get −|u(t)|′ ≤ M `1(1)(t)−m`0(1)(t) + q∗(t) for a.e. t ∈ [a, b]. (65) If u(b) = 0 then m = 0 and the integration of (32) from t1 to b, on account of (37), yields M ≤ M b∫ t1 `1(1)(s) ds+ b∫ t1 q∗(s) ds. From the last inequality, in view of (15), it follows that ‖u‖C = M ≤ r0(‖q∗‖+ c), where r0 = [1− ‖`1(1)‖L]−1 . Consequently, the estimate (27) holds with r = r0. If u(b) 6= 0 then, according to (64), we obtain λ|u(b)| − |u(a)| ≤ h1(|u|)− h0(|u|) + c, (66) and thus |u(b)| − |u(a)| ≤ h1(|u|)− h0(|u|) + |u(b)|(1− λ) + c (67) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 381 and λ (|u(b)| − |u(a)|) ≤ h1(|u|)− h0(|u|) + |u(a)|(1− λ) + c. (68) Let first (39) hold. The integration of (65) from a to t2 and from t1 to b, in view of (10) and (37), results in |u(a)| −m ≤ M t2∫ a `1(1)(s) ds+ t2∫ a q∗(s) ds, and M − |u(b)| ≤ M b∫ t1 `1(1)(s) ds+ b∫ t1 q∗(s) ds. (69) Multiplying both sides of (69) by λ and summing the last inequalities, in view of (10), (36), and (66), we get M (λ− h1(1)−max{1, λ}‖`1(1)‖L) ≤ m(1− h0(1)) + c+ max{1, λ}‖q∗‖L. Hence, by virtue of (5) and (6), we obtain M(β(λ, h1)− ‖`1(1)‖L) ≤ mα(λ, h0) + c+ ‖q∗‖L. (70) If (38) is fulfilled then the integration of (65) from t1 to t2, on account of (5), (6), and (7), yields Mβ(λ, h1)−mα(λ, h0) ≤ (M −m)(λ− h1(1))min { 1, 1 λ } ≤ ≤ M −m ≤ M‖`1(1)‖L + ‖q∗‖L. Therefore, in both cases (38) and (39), the inequality (70) holds. On the other hand, the integration of (65) from a to b implies |u(a)| − |u(b)| ≤ M‖`1(1)‖L −m‖`1(1)‖L + ‖q∗‖L. (71) Hence, using (36), (67), and (68) in (71) we get m ≤ M(1− β(λ, h1) + ‖`1(1)‖L) + ‖q∗‖L + c 1 + ‖`0(1)‖L − α(λ, h0) . From the last inequality and (70) we obtain M(β(λ, h1)− ‖`1(1)‖L) ≤ ≤ M(1− β(λ, h1) + ‖`1(1)‖L) + ‖q∗‖L + c 1 + ‖`0(1)‖L − α(λ, h0) α(λ, h0) + ‖q∗‖L + c. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 382 Z. OPLUŠTIL Thus, on account of (15) and the first inequality in (16), we have ‖u‖C = M ≤ r1 (c+ ‖q∗‖L)(1 + ‖`0(1)‖L), where r1 = [(β(λ, h1)− ‖`1(1)‖L)(1 + ‖`0(1)‖L)− α(λ, h0)] −1 > 0. Therefore, the estimate (27) holds, where r is defined by r = r1(1 + ‖`0(1)‖L). Now suppose that u changes its sign. Define numbersM andm by (49) and choose tM , tm ∈ ∈ [a, b] such that (50) is fulfilled. Obviously, M > 0, m > 0, and either (51) or (52) holds. First suppose that (51) is fulfilled. It is clear that there exists α1 ∈ ]tm, tM [ such that u(t) < 0 for tm ≤ t < α1, u(α1) = 0. (72) Let α2 = sup{t ∈ [a, b] : u(s) > 0 for tM ≤ s ≤ t}. Obviously, u(t) > 0 for tM ≤ t < α2 and u(α2) = 0 if α2 < b. (73) Put α3 = { a, if u(a) ≤ 0, sup{t ∈ [a, tm] : u(s) > 0 for a ≤ s ≤ t}, if u(a) > 0. It is clear that if α3 > a then u(t) > 0 for a ≤ t < α3, u(α3) = 0. (74) The integration of (32) from tm to α1, from tM to α2, and from a to α3, in view of (10), (49), (63) and (72) – (74), yields m ≤ M α1∫ tm `0(1)(s) ds+m α1∫ tm `1(1)(s) ds+ α1∫ tm q∗(s) ds, (75) M − u(α2) ≤ M α2∫ tM `1(1)(s) ds+m α2∫ tM `0(1)(s) ds+ α2∫ tM q∗(s) ds, (76) u(a)− u(α3) ≤ M α3∫ a `1(1)(s) ds+m α3∫ a `0(1)(s) ds+ α3∫ a q∗(s) ds. (77) ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 383 If u(b) ≤ 0 or u(a) ≤ 0 then, according to (49), (64), and (73), we obtain λu(α2) ≤ mh0(1) +Mh1(1) + c. (78) Multiplying both sides of (76) by λ and taking into account (10) and (78), we get λM − c−mh0(1)−Mh1(1) ≤ ≤ λ M α2∫ tM `1(1)(s) ds+m α2∫ tM `0(1)(s) ds+ α2∫ tM q∗(s) ds  , (79) and thus min { 1, 1 λ } (λM − c−mh0(1)−Mh1(1)) ≤ ≤ M ∫ I `1(1)(s) ds+m ∫ I `0(1)(s) ds+ ∫ I q∗(s) ds, (80) where I = [a, α3] ∪ [tM , α2]. If u(b) > 0 and u(a) > 0 then multiplying both sides of (76) by λ we get λM − λu(α2) ≤ λ M α2∫ tM `1(1)(s) ds+m α2∫ tM `0(1)(s) ds+ α2∫ tM q∗(s) ds  . Summing the last inequality and (77), according to (49), (64), (73), and (74), we obtain that the inequality (80) with I = [a, α3] ∪ [tM , α2] holds. From (75) and (80) we get m(1−A1) ≤ MC1 + ‖q∗‖L + c, (81) M(β(λ, h1)−B1) ≤ m ( min { 1, 1 λ } h0(1) +D1 ) + ‖q∗‖L + c, (82) where A1 = α1∫ tm `1(1)(s) ds, B1 = ∫ I `1(1)(s) ds, and C1 = α1∫ tm `0(1)(s) ds, D1 = ∫ I `0(1)(s) ds. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 384 Z. OPLUŠTIL Due to (15), it is clear that A1 < 1 and B1 < β(λ, h1). Consequently, (81) and (82) imply 0 < m(1−A1)(β(λ, h1)−B1) ≤ ≤ mC1 ( min { 1, 1 λ } h0(1) +D1 ) + (‖q∗‖L + c)(1 + ‖`0(1)‖L), (83) 0 < M(1−A1)(β(λ, h1)−B1) ≤ ≤ MC1 ( min { 1, 1 λ } h0(1) +D1 ) + (‖q∗‖L + c)(2 + ‖`0(1)‖L). Obviously, (1−A1)(β(λ, h1)−B1) ≥ β(λ, h1)−A1β(λ, h1)−B1 ≥ ≥ β(λ, h1)− (A1 +B1) ≥ β(λ, h1)− ‖`1(1)‖L > 0 and 4C1 ( min { 1, 1 λ } h0(1) +D1 ) ≤ ( min { 1, 1 λ } h0(1) + C1 +D1 )2 ≤ ≤ ( min { 1, 1 λ } h0(1) + ‖`0(1)‖L )2 . Hence, from the second inequality in (16) and (83) we obtain M ≤ r2(‖`0(1)‖L + 2)(c+ ‖q∗‖L), m ≤ r2(‖`0(1)‖L + 1)(c+ ‖q∗‖L), where r2 = [ β(λ, h1)− ‖`1(1)‖L − ( ‖`0(1)‖L + min { 1, 1 λ } h0(1) )2 4 ]−1 . Consequently, the estimate (27) holds, where r is defined by r = r2(‖`0(1)‖L + 2)(c+ ‖q∗‖L). If (52) holds, the validity of the estimate (27) can be proved analogously. The lemma is proved. 5. Proofs. Proof of Theorems 1 and 3. The validity of theorems follows from Lemmas 2, 3, and 4. Proof of Theorem 2 and 4. The assertion of theorems can be derived from Lemmas 2, 3, and 5. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 NEW SOLVABILITY CONDITIONS FOR A NONLOCAL BOUNDARY-VALUE PROBLEM FOR NONLINEAR . . . 385 Proof of Corollary 1. It is clear that (18), (19) is a particular case of (1), (2) in which a = 0, b = 1, and F, h, and ϕ are defined by the formulae F (z)(t) df= d cos(2πt) 1∫ 0 z(τ(s))√ s ds− g1(t)z(t)ez 2(ω(t)) + g2(t)|z(t)|ν for a.e. t ∈ [0, 1] and all z ∈ C([0, 1]; R) and h(z) df= z(0)− 1 2 z(1)− k 1∫ 0 sin(2πs)z(s) ds, ϕ(z) df= −z(0)ez(1/4) + arctan z(1/2) for z ∈ C([0, 1]; R), respectively. Moreover, the above-defined functional h admits the repre- sentation (4), where λ = 1/2 and h0(z) df= k 1∫ 0 max { sin(2πs), 0 } z(s) ds, h1(z) df= k 1∫ 0 max { − sin(2πs), 0 } z(s) ds for z ∈ C([0, 1]; R). Now we put `0(z)(t) df= d max { cos(2πt), 0 } 1∫ 0 z(τ(s))√ s ds, `1(z)(t) df= d max { − cos(2πt), 0 } 1∫ 0 z(τ(s))√ s ds for a.e. t ∈ [0, 1] and all z ∈ C([0, 1]; R). It is easy to verify that `0, `1 ∈ Pab, h0, h1 ∈ PFab, and ‖`0(1)‖L = ‖`1(1)‖L = 2d π , h0(1) = h1(1) = k π . Therefore, in view of the assumptions (20) and (21), the conditions (7), (8), (13), and (14) of Theorem 1 are fulfilled. On the other hand, operators F and ϕ satisfy the assumptions (H1) and (H2), the relation (9) with c = π/2 holds, and the inequality (11) is satisfied on the set C([0, 1]; R), where q(t, x) = |g2(t)|xν for a.e. t ∈ [0, 1] and all x ∈ R+. Applying Theorem 1, we establish solvability of the problem (18), (19). 1. Azbelev N. V., Maksimov V. P., Rakhmatullina L. F. Introduction to the theory of functional differential equa- tions (in Russian). — Moscow: Nauka, 1991. 2. Hakl R., Kiguradze I., Půža B. Upper and lower solutions of boundary-value problems for functional differ- ential equations and theorems on functional differential inequalities // Georg. Math. — 2000. — 7, №. 3. — P. 489 – 512. ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3 386 Z. OPLUŠTIL 3. Hakl R., Lomtatidze A., Šremr J. On a periodic type boundary-value problem for first order nonlinear func- tional differential equations // Nonlinear Anal. — 2002. — 51. — P. 425 – 447. 4. Hakl R., Lomtatidze A., Šremr J. Some boundary-value problems for first order scalar functional differential equations // Folia Fac. Sci. Natur. Univ. Masar. Brunensis, Brno. — 2002. 5. Hale J. Theory of functional differential equations. — New York etc.: Springer, 1977. 6. Kiguradze I., Půža B. On boundary-value problems for functional differential equations // Mem. Different. Equat. Math. Phys. — 1997. — 12. — P. 106 – 113. 7. Kiguradze I., Sokhadze Z. On the global solvability of the Cauchy problem for singular functional differential equations // Georg. Math. J. — 1997. — 4, № 4. — P. 355 – 373. 8. Kiguradze I., Sokhadze Z. On the uniqueness of a solution to the Cauchy problem for functional differential equations // Different. Equat. — 1995. — 31, № 12. — P. 1947 – 1958. 9. Kiguradze I. T., Půža B. Theorems of Conti – Opial type for nonlinear functional-differential equations // Ibid. — 1997. — 33, №. 2. — P. 184 – 193. 10. Kolmanovskii V., Myshkis A. Introduction to the theory and applications of functional differential equations. — Dordrecht etc.: Kluwer Acad. Publ., 1999. 11. Schwabik Š., Tvrdý M., Vejvoda O. Differential and integral equations: boundary-value problems and ad- joints. — Praha: Academia, 1979. 12. Lomtatidze A., Opluštil Z., Šremr J. On a nonlocal boundary-value problem for first order linear functional differential equations // Mem. Different. Equat. Math. Phys. — 2007. — 41. — P. 69 – 85. Received 19.11.07 ISSN 1562-3076. Нелiнiйнi коливання, 2008, т . 11, N◦ 3
id nasplib_isofts_kiev_ua-123456789-178203
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
issn 1562-3076
language English
last_indexed 2025-11-28T11:17:51Z
publishDate 2008
publisher Інститут математики НАН України
record_format dspace
spelling Oplustil, Z.
2021-02-18T08:15:55Z
2021-02-18T08:15:55Z
2008
New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations / Z. Oplustil // Нелінійні коливання. — 2008. — Т. 11, № 3. — С. 365-386. — Бібліогр.: 12 назв. — англ.
1562-3076
https://nasplib.isofts.kiev.ua/handle/123456789/178203
517.9
New efficient conditions are obtained sufficient for the solvability as well as unique solvability of a nonlocal boundary-value problem for nonlinear functional differential equations.
Отримано новi ефективнi умови розв’язностi, а також єдиної розв’язностi нелокальних граничних задач для нелiнiйних функцiонально-диференцiальних рiвнянь.
Published results were acquired using the subsidization of the Ministry of Education, Youth and Sports of the Czech Republic, research plan MSM 0021630518 “Simulation modelling of mechatronic systems”.
en
Інститут математики НАН України
Нелінійні коливання
New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
Новi умови розв’язностi нелокальних граничних задач для нелiнiйних функцiонально-диференцiальних рiвнянь
Article
published earlier
spellingShingle New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
Oplustil, Z.
title New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
title_alt Новi умови розв’язностi нелокальних граничних задач для нелiнiйних функцiонально-диференцiальних рiвнянь
title_full New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
title_fullStr New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
title_full_unstemmed New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
title_short New solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
title_sort new solvability conditions for a non-local boundary value problem for nonlinear functional differential equations
url https://nasplib.isofts.kiev.ua/handle/123456789/178203
work_keys_str_mv AT oplustilz newsolvabilityconditionsforanonlocalboundaryvalueproblemfornonlinearfunctionaldifferentialequations
AT oplustilz noviumovirozvâznostinelokalʹnihgraničnihzadačdlâneliniinihfunkcionalʹnodiferencialʹnihrivnânʹ