On the problem of determining the parameter of a parabolic equation

We study the boundary-value problem of determining the parameter p of a parabolic equation $$v′(t)+Av(t)=f(t)+p,\;0⩽t⩽1,v(0)=φ,\;v(1)=ψ,$$ with strongly positive operator $A$ in an arbitrary Banach space $E$. The exact estimates are established for the solution of this problem in Hölder norms. In ap...

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Datum:2010
Hauptverfasser: Ashyralyev, A., Аширалієв, A.
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Veröffentlicht: Institute of Mathematics, NAS of Ukraine 2010
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Ukrains’kyi Matematychnyi Zhurnal
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author Ashyralyev, A.
Аширалієв, A.
author_facet Ashyralyev, A.
Аширалієв, A.
author_sort Ashyralyev, A.
baseUrl_str https://umj.imath.kiev.ua/index.php/umj/oai
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description We study the boundary-value problem of determining the parameter p of a parabolic equation $$v′(t)+Av(t)=f(t)+p,\;0⩽t⩽1,v(0)=φ,\;v(1)=ψ,$$ with strongly positive operator $A$ in an arbitrary Banach space $E$. The exact estimates are established for the solution of this problem in Hölder norms. In applications, the exact estimates are obtained for the solutions of the boundary-value problems for parabolic equations.
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fulltext UDC 517.5 A. Ashyralyev (Fatih Univ., Istanbul, Turkey) ON A PROBLEM OF DETERMINING THE PARAMETЕR OF A PARABOLIC EQUATION ПРО ЗАДАЧУ ВИЗНАЧЕННЯ ПАРАМЕТРА ПАРАБОЛIЧНОГО РIВНЯННЯ The boundary-value problem of determining the parameter p of a parabolic equation v′(t) +Av(t) = f(t) + p(0 ≤ t ≤ 1), v(0) = ϕ, v(1) = ψ in arbitrary Banach space E with the strongly positive operator A is considered. The exact estimates in Hölder norms for the solution of this problem are established. In applications, exact estimates for the solution of the boundary-value problems for parabolic equations are obtained. Розглянуто крайову задачу визначення параметра p параболiчного рiвняння v′(t) +Av(t) = f(t) + p(0 ≤ t ≤ 1), v(0) = ϕ, v(1) = ψ у довiльному банаховому просторi E iз сильно додатним оператором A. Встановлено точнi за норма- ми Гельдера оцiнки для розв’язку цiєї задачi. У застосуваннях одержано точнi оцiнки для розв’язкiв крайових задач для параболiчних рiвнянь. 1. Introduction. Methods of solutions of the nonlocal boundary-value problems for evolution equations with a parameter have been studied extensively by many researchers (see, e.g., [1 – 21] and the references given therein). We consider the following local boundary-value problem for the differential equation v′(t) +Av(t) = f(t) + p(0 ≤ t ≤ 1), v(0) = ϕ, v(1) = ψ (1.1) in an arbitrary Banach space with linear (unbounded) operator A and an unknown pa- rameter p. In the paper [1] the solvability of the problem (1.1) in the space C(E) of the con- tinuous E-valued functions ϕ(t) defined on [0, 1], equipped with the norm ‖ϕ‖C(E) = max 0≤t≤1 ‖ϕ(t)‖E was studied under the necessary and sufficient conditions for the operator A. The solu- tion depends continuously on the initial and boundary data. Namely: Theorem 1.1. Assume that −A is the generator of the analytic semigroup exp{−tA}(t ≥ 0) and all points 2πik, k ∈ Z, k 6= 0 are not belongs to the spec- trum σ(A). Let v(0) ∈ E, v(1) ∈ D(A) and f(t) ∈ Cβ(E), 0 < β ≤ 1. Then for the solution (v(t), p) of problem (1.1) in C(E)× E the estimates ‖p‖E ≤M [ ‖v(0)‖E + ‖v(1)‖E + ‖Av(1)‖E + 1 β ‖f‖Cβ(E) ] , ‖v‖C(E) ≤M [‖v(0)‖E + ‖v(1)‖E + ‖f‖C(E)] hold, where M does not depend on β, v(0), v(1) and f(t). Here Cβ(E) is the space obtained by completion of the space of all smooth E-valued functions ϕ(t) on [0, 1] in c© A. ASHYRALYEV, 2010 1200 ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 ON A PROBLEM OF DETERMINING THE PARAMETR OF A PARABOLIC EQUATION 1201 the norm ‖ϕ‖Cβ(E) = max 0≤t≤1 ‖ϕ(t)‖E + sup 0≤t<t+τ≤1 ‖ϕ(t+ τ)− ϕ(t)‖E τβ . We say (v(t), p) is the solution of the problem (1.1) in Cβ,γ0 (E)×E1 if the following conditions are satisfied: i) v′(t), Av(t) ∈ Cβ,γ0 (E), p ∈ E1 ⊂ E, ii) (v(t), p) satisfies the equation and boundary conditions (1.1). Here Cβ,γ0 (E), (0 ≤ γ ≤ β, 0 < β < 1) is the Hölder space with weight obtained by completion of the space of all smooth E-valued functions ϕ(t) on [0, 1] in the norm ‖ϕ‖Cβ,γ0 (E) = max 0≤t≤1 ‖ϕ(t)‖E + sup 0≤t<t+τ≤1 (t+ τ)γ‖ϕ(t+ τ)− ϕ(t)‖E τβ . In the present paper the exact estimates in Hölder norms for the solution of problem (1.1) are proved. In applications, exact estimates for the solution of the boundary-value problems for parabolic equations are obtained. 2. Cβ,γ 0 (E)-estimates for the solution of problem (1.1). We study the problem (1.1) in the spaces Cβ,γ0 (E). To these spaces there correspond the spaces of traces Eβ,γ1 , which consist of the elements w ∈ E for which the following norm is finite: |w|β,γ1 = max 0≤z≤1 ‖A exp{−zA}w‖E+ + sup 0≤z<z+τ≤1 (z + τ)γ‖A (exp{− (z + τ)A} − exp{−zA})w‖E τβ . Assume that −A is the generator of the analytic semigroup exp{−tA}(t ≥ 0) with exponentially decreasing norm, when t→ +∞, i.e., the following estimates hold: ‖ exp{−tA}‖E→E ≤Me−δt, t‖A exp{−tA}‖E→E ≤M, t > 0, M > 0, δ > 0. (2.1) From (2.1) it follows that ‖T‖E→E ≤M(δ). (2.2) Here T = (I − exp{−A})−1. We have that v(t) = exp{−tA}v(0) + t∫ 0 exp{−(t− s)A}f(s)ds+ (I − exp{−tA})A−1p, p = T{Av(1)−A exp{−A}v(0)− 1∫ 0 A exp{−(1− s)A}f(s)ds} (2.3) for the solution of problem (1.1) in the space Cβ,γ0 (E) (see, for example, [1, 22]). ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 1202 A. ASHYRALYEV Theorem 2.1. Let v(0)−A−1f(0), v(1)−A−1f(1) ∈ Eβ,γ1 and f(t) ∈ Cβ,γ0 (E), 0 ≤ γ ≤ β, 0 < β < 1. Then for the solution (v(t), p) of problem (1.1) in Cβ,γ0 (E) × × Eβ,γ1 the estimates ‖v′‖Cβ,γ0 (E) + ‖Av − p‖Cβ,γ0 (E) + max 0≤t≤1 ∣∣v(t)−A−1f(t) ∣∣β,γ 1 ≤ ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣v(1)−A−1f(1) ∣∣β,γ 1 + β−1(1− β)−1‖f‖Cβ,γ0 (E) ] , (2.4) ∣∣A−1p ∣∣β,γ 1 ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1 + + ∣∣v(1)−A−1f(1) ∣∣β,γ 1 + β−1(1− β)−1‖f‖Cβ,γ0 (E) ] (2.5) hold, where M does not depend on γ, β, v(0), v(1) and f(t). Proof. Using formula (2.3), we can write Av(t)− f(t) = exp{−tA} (Av(0)− f(0)) + exp{−tA} (f(0)− f(t)) + + t∫ 0 A exp{−(t− s)A} (f(s)− f(t)) ds+ (I − exp{−tA}) p = = exp{−tA} (Av(0)− f(0)) + (I − exp{−tA}) p+ J(t), (2.6) p = T{Av(1)− f(1)− exp{−A} (Av(0)− f(0))− − 1∫ 0 A exp{−(1− s)A} (f(s)− f(1)) ds+ exp{−A} (f(1)− f(0))} = = T{Av(1)− f(1)− exp{−A} (Av(0)− f(0))− J(1)}, (2.7) where J(t) = exp{−tA} (f(0)− f(t)) + t∫ 0 A exp{−(t− s)A} (f(s)− f(t)) ds. By [22], Theorems 5.1 and 5.2 in Chapter 1, ‖J‖Cβ,γ0 (E) ≤Mβ−1(1− β)−1‖f‖Cβ,γ0 (E), (2.8) ∣∣A−1J(t) ∣∣β,γ 1 ≤Mβ−1(1− β)−1‖f‖Cβ,γ0 (E). (2.9) From the definition of the space Eβ,γ1 and the estimate (2.1) it follows that∣∣exp{−tA} ( v(0)−A−1f(0) ) + (I − exp{−tA})A−1p ∣∣β,γ 1 ≤ ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 ON A PROBLEM OF DETERMINING THE PARAMETR OF A PARABOLIC EQUATION 1203 ≤ ‖exp{−tA}‖E→E ∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ‖I − exp{−tA}‖E→E ∣∣A−1p ∣∣β,γ 1 ≤ ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣A−1p ∣∣β,γ 1 ] (2.10) for all t, t ∈ [0, 1]. By (2.2), (2.9), (2.10) and the triangle inequality max 0≤t≤1 ∣∣v(t)−A−1f(t) ∣∣β,γ 1 ≤ ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣A−1p ∣∣β,γ 1 + β−1(1− β)−1‖f‖Cβ,γ0 (E) ] , (2.11) ∣∣A−1p ∣∣β,γ 1 ≤ ‖T‖E→E [∣∣v(1)−A−1f(1) ∣∣β,γ 1 + + ‖exp{−A}‖E→E ∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣A−1J(1) ∣∣β,γ 1 ] ≤ ≤M [∣∣v(1)−A−1f(1) ∣∣β,γ 1 + ∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣A−1J(1) ∣∣β,γ 1 ] . (2.12) Estimate for max 0≤t≤1 ∣∣v(t)−A−1f(t) ∣∣β,γ 1 and estimate (2.5) are proved. Using formula (2.6) and equation (1.1), we can write v′(t) = exp{−tA} (Av(0)− f(0)− p) + J(t). (2.13) Applying the triangle inequality and the definition of the space Cβ,γ0 (E), we obtain ‖v′‖Cβ,γ0 (E) ≤ ∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣A−1p ∣∣β,γ 1 + ‖J‖Cβ,γ0 (E). From this estimate and (2.12), (2.12) it follows that ‖v′‖Cβ,γ0 (E) ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1 + + ∣∣v(1)−A−1f(1) ∣∣β,γ 1 + β−1(1− β)−1‖f‖Cβ,γ0 (E) ] . The estimate for Av(t) − p in the norm Cβ,γ0 (E) follows from this estimate and the triangle inequality. Theorem 2.1 is proved. Remark 2.1. The spaces Cβ,γ0 (E) in which exact estimates has been established, depend on parameters β and γ. However, the constants in these inequalities depend only on β. Hence, we can be choose the parameter γ freely, which increases the number of spaces. With the help of A we introduce the fractional space Eα(E,A), 0 < α < 1, con- sisting of all v ∈ E for which the following norms are finite: ‖v‖α = sup λ>0 ∥∥λ1−αA exp{−λA}v ∥∥ E + ‖v‖E . 3. Cβ,γ 0 (Eα−β)-estimates for the solution of problem (1.1). We study the problem (1.1) in the spaces Cβ,γ0 (Eα−β). To these spaces there correspond the spaces of traces ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 1204 A. ASHYRALYEV Eβ,γ1+α−β , which consist of the elements w ∈ E for which the following norm is finite: |w|β,γ1+α−β = max 0≤z≤1 ‖A exp{−zA}w‖ α−β+ + sup 0≤z<z+τ≤1 (z + τ)γ‖A (exp{− (z + τ)A} − exp{−zA})w‖ α−β τβ . Theorem 3.1. Let v(0) − A−1f(0), v(1) − A−1f(1) ∈ Eβ,γ1+α−β and f(t) ∈ ∈ Cβ,γ0 (Eα−β), 0 ≤ γ ≤ β ≤ α, 0 < α < 1. Then for the solution (v(t), p) of problem (1.1) in Cβ,γ0 (Eα−β)× Eβ,γ1+α−β the estimates ‖v′‖Cβ,γ0 (Eα−β) + ‖Av − p‖Cβ,γ0 (Eα−β) + max 0≤t≤1 ∣∣v(t)−A−1f(t) ∣∣β,γ 1 ≤ ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + + ∣∣v(1)−A−1f(1) ∣∣β,γ 1+α−β + α−1(1− α)−1‖f‖Cβ,γ0 (Eα−β) ] , (3.1) ∣∣A−1p ∣∣β,γ 1+α−β ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + + ∣∣v(1)−A−1f(1) ∣∣β,γ 1+α−β + α−1(1− α)−1‖f‖Cβ,γ0 (Eα−β) ] (3.2) hold, where M does not depend on γ, β, α, v(0), v(1) and f(t). Proof. By [22], Theorem 5.3 in Chapter 1, ‖J‖Cβ,γ0 (Eα−β) ≤Mα−1(1− α)−1‖f‖Cβ,γ0 (Eα−β), (3.3) ∣∣A−1J(t) ∣∣β,γ 1+α−β ≤Mα−1(1− α)−1‖f‖Cβ,γ0 (Eα−β). (3.4) From the definition of the space Eβ,γ1+α−β and the estimate (2.1) it follows that ∣∣exp{−tA} ( v(0)−A−1f(0) ) + (I − exp{−tA})A−1p ∣∣β,γ 1+α−β ≤ ≤ ‖ exp{−tA}‖E→E ∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + +‖ − exp{−tA}‖E→E ∣∣A−1p ∣∣β,γ 1+α−β ≤ ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + ∣∣A−1p ∣∣β,γ 1+α−β ] (3.5) for all t, t ∈ [0, 1]. By (2.2), (3.4), (3.5) and the triangle inequality max 0≤t≤1 ∣∣v(t)−A−1f(t) ∣∣β,γ 1+α−β ≤ ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 ON A PROBLEM OF DETERMINING THE PARAMETR OF A PARABOLIC EQUATION 1205 ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + ∣∣A−1p ∣∣β,γ 1+α−β + α−1(1− α)−1‖f‖Cβ,γ0 (Eα−β) ] , (3.6) ∣∣A−1p ∣∣β,γ 1+α−β ≤ ‖T‖E→E [∣∣v(1)−A−1f(1) ∣∣β,γ 1+α−β + + ‖exp{−A}‖E→E ∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + ∣∣A−1J(1) ∣∣β,γ 1+α−β ] ≤ ≤M [∣∣v(1)−A−1f(1) ∣∣β,γ 1+α−β + ∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + ∣∣A−1J(1) ∣∣β,γ 1+α−β ] . (3.7) Estimate for max 0≤t≤1 ∣∣v(t)−A−1f(t) ∣∣β,γ 1+α−β and estimate (3.2) are proved. Applying (2.13), the triangle inequality and the definition of the space Cβ,γ0 (Eα−β), we obtain ‖v′‖Cβ,γ0 (Eα−β) ≤ ∣∣v(0)−A−1f(0) ∣∣β,γ 1 + ∣∣A−1p ∣∣β,γ 1 + ‖J‖Cβ,γ0 (Eα−β). From this estimate and (3.7), (3.7) it follows that ‖v′‖Cβ,γ0 (Eα−β) ≤M [∣∣v(0)−A−1f(0) ∣∣β,γ 1+α−β + + ∣∣v(1)−A−1f(1) ∣∣β,γ 1+α−β + α−1(1− α)−1‖f‖Cβ,γ0 (Eα−β) ] . The estimate for Av(t)− p in the norm Cβ,γ0 (Eα−β) follows from this estimate and the triangle inequality. Theorem 3.1 is proved. Note that applying the definition of the space Eβ,γ1+α−β , we can obtain |w|β,γ1+α−β ≤M‖Aw‖Eα−γ , Aw ∈ Eα−γ . We have not been able to establish the opposite inequality necessary for the equivalence of norms. Nevertheless, we have the following result. Theorem 3.2. Let v(0) − A−1f(0), v(1) − A−1f(1) ∈ Eα−γ and f(t) ∈ ∈ Cβ,γ0 (Eα−β), 0 ≤ γ ≤ β ≤ α, 0 < α < 1. Then for the solution (v(t), p) of problem (1.1) in Cβ,γ0 (Eα−β)× Eα−γ the estimates ‖v′‖Cβ,γ0 (Eα−β) + ‖Av − p‖Cβ,γ0 (Eα−β) + max 0≤t≤1 ‖Av(t)− f(t)‖α−γ ≤ ≤M [ ‖Av(0)− f(0)‖α−γ + ‖Av(1)− f(1)‖α−γ + α−1(1− α)−1‖f‖Cβ,γ0 (Eα−β) ] , (3.8) ‖p‖α−γ ≤M [ ‖Av(0)− f(0)‖α−γ + + ‖Av(1)− f(1)‖α−γ + α−1(1− α)−1‖f‖Cβ,γ0 (Eα−β) ] (3.9) hold, where M does not depend on γ, β, α, v(0), v(1) and f(t). ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 1206 A. ASHYRALYEV Remark 3.1. The spaces Cβ,γ0 (Eα−β) in which exact estimates has been estab- lished, depend on parameters α, β and γ. However, the constants in these inequalities depend only on α. Hence, we can be choose parameters β, γ freely, which increases the number of spaces. In particular, Theorems 3.1 and 3.2 imply the well-posedness theorem in C(Eα). Remark 3.2. Theorems 2.1 and 3.1, 3.2 hold for the following boundary-value problems: v′(t) +Av(t) = f(t) + p(0 ≤ t ≤ 1), v(0) = ϕ, v(λ) = ψ, 0 < λ ≤ 1, v′(t)−Av(t) = f(t) + p(0 ≤ t ≤ 1), v(1) = ϕ, v(λ) = ψ, 0 ≤ λ < 1 in an arbitrary Banach space with positive operator A and an unknown parameter p. Applications. First, the boundary-value problem on the range {0 ≤ t ≤ 1, x ∈ Rn} for the 2m-order multidimensional parabolic equation is considered: ∂v(t, x) ∂t + ∑ |r|=2m ar(x) ∂|r|v(t, x) ∂xr11 . . . ∂xrnn + σv(t, x) = f(t, x) + p(x), 0 < t < 1, ∑ |r|=2m ar(x) ∂|r|v(0, x) ∂xr11 . . . ∂xrnn + σv(0, x) = f(0, x), x ∈ Rn, ∑ |r|=2m ar(x) ∂|r|v(1, x) ∂xr11 . . . ∂xrnn + σv(1, x) = f(1, x), x ∈ Rn, |r| = r1 + . . .+ rn, (4.1) where ar(x) and f(t, x) are given as sufficiently smooth functions. Here, σ is a suffi- ciently large positive constant. It is assumed that the symbol Bx(ξ) = ∑ |r|=2m ar(x) (iξ1) r1 . . . (iξn) rn , ξ = (ξ1, . . . , ξn) ∈ Rn of the differential operator of the form Bx = ∑ |r|=2m ar(x) ∂|r| ∂xr11 . . . ∂xrnn (4.2) acting on functions defined on the space Rn, satisfies the inequalities 0 < M1|ξ|2m ≤ (−1)mBx(ξ) ≤M2|ξ|2m <∞ for ξ 6= 0. The problem (4.1) has a unique smooth solution. This allows us to reduce the prob- lem (4.1) to the problem (1.1) in a Banach space E = Cµ(Rn) of all continuous bounded functions defined on Rn satisfying a Hölder condition with the indicator µ ∈ (0, 1) with a strongly positive operator A = Bx + σI defined by (4.2) (see [25] and [26]). ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 ON A PROBLEM OF DETERMINING THE PARAMETR OF A PARABOLIC EQUATION 1207 Theorem 4.1. For the solution of the boundary problem (4.1) the following esti- mates are satisfied: ‖v‖C1+β,γ 0 (Cµ(Rn)) ≤ M(µ) β(1− β) ‖f‖Cβ,γ0 (Cµ(Rn)), 0 ≤ γ ≤ β < 1, 0 < µ < 1, ‖v‖C1+β,γ 0 (C2m(α−β)(Rn)) ≤M(α, β)‖f‖Cβ,γ0 (C2m(α−β)(Rn)), ‖p‖C2m(α−γ)(Rn) ≤M(α, β, γ)‖f‖Cβ,γ0 (C2m(α−β)(Rn)), 0 ≤ γ ≤ β, 0 < 2m(α− β) < 1, where M(µ), M(α, β) and M(α, β, γ) does not depend on f(t, x). The proof of Theorem 4.1 is based on the abstract Theorems 2.1, 3.2 and on the following theorem on the structure of the fractional spaces Eα(A,Cµ(Rn)). Theorem 4.2. Eα(A,Cµ(Rn)) = C2mα+µ(Rn) for all 0 < α < 1 2m , 0 < µ < < 1 [22]. Second, let Ω be the unit open cube in the n-dimensional Euclidean space Rn, 0 < xk < 1, 1 ≤ k ≤ n, with boundary S,Ω = Ω ∪ S. In [0, 1] × Ω we consider the mixed boundary-value problem for the multidimensional parabolic equation ∂v(t, x) ∂t − n∑ r=1 αr(x) ∂2v(t, x) ∂x2 r + σv(t, x) = f(t, x) + p(x), x = (x1, . . . , xn) ∈ Ω, 0 < t < 1, − n∑ r=1 αr(x) ∂2v(0, x) ∂x2 r + σv(0, x) = f(0, x), x ∈ Ω, − n∑ r=1 αr(x) ∂2v(1, x) ∂x2 r + σv(1, x) = f(1, x), x ∈ Ω, v(t, x) = 0, x ∈ S, (4.3) where αr(x) (x ∈ Ω) and f(t, x) (t ∈ (0, 1), x ∈ Ω) are given smooth functions and αr(x) ≥ a > 0. Here, σ is a sufficiently large positive constant. We introduce the Banach spaces Cβ01(Ω), β = (β1, . . . , βn), 0 < xk < 1, k = = 1, . . . , n, of all continuous functions satisfying a Hölder condition with the indicator β = (β1, . . . , βn), βk ∈ (0, 1), 1 ≤ k ≤ n and with weight xβkk (1 − xk − hk)βk , 0 ≤ xk < xk + hk ≤ 1, 1 ≤ k ≤ n, which equipped with the norm ‖f‖Cβ01(Ω) = ‖f‖C(Ω) + sup 0≤xk<xk+hk≤1, 1≤k≤n ∣∣f(x1, . . . , xn)− −f(x1 + h1, . . . , xn + hn) ∣∣ n∏ k=1 h−βkk xβkk (1− xk − hk)βk , ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 1208 A. ASHYRALYEV where C(Ω)-is the space of the all continuous functions defined on Ω, equipped with the norm ‖f‖C(Ω) = max x∈Ω |f(x)| . It is known that the differential expression [24] Av = − n∑ r=1 αr(t, x) ∂2v(t, x) ∂x2 + δv(t, x) defines a positive operator A acting on Cβ01(Ω) with domain D(A) ⊂ C2+β 01 (Ω) and satisfying the condition v = 0 on S. Therefore, we can replace the mixed problem (4.3) by the abstract boundary problem (1.1). Using the results of Theorem 2.1, we can obtain that the following theorem. Theorem 4.3. For the solution of the mixed boundary-value problem (4.3) the following estimate is valid: ‖v‖C1+β,γ 0 (Cµ01(Ω))) ≤ M(µ) β(1− β) ‖f‖Cβ,γ0 (Cµ01(Ω))), 0 ≤ γ ≤ β < 1, µ = {µ1, . . . , µn}, 0 < µk < 1, 1 ≤ k ≤ n, where M(µ) is independent of β, γ and f(t, x). Third, we consider the mixed boundary-value problem for parabolic equation ∂v(t, x) ∂t − a(x) ∂2v(t, x) ∂x2 + σv(t, x) = f(t, x) + p(x), 0 < t < 1, 0 < x < 1, −a(x) ∂2v(0, x) ∂x2 + σv(0, x) = f(0, x), 0 ≤ x ≤ 1, −a(x) ∂2v(1, x) ∂x2 + σv(1, x) = f(1, x), 0 ≤ x ≤ 1, u(t, 0) = u(t, 1), ux(t, 0) = ux(t, 1), 0 ≤ t ≤ 1, (4.4) where a(t, x) and f(t, x) are given sufficiently smooth functions and a(t, x) ≥ a > 0. Here, σ is a sufficiently large positive constant. We introduce the Banach spaces Cβ [0, 1], 0 < β < 1 of all continuous functions ϕ(x) satisfying a Hölder condition for which the following norms are finite ‖ϕ‖Cβ [0,1] = ‖ϕ‖C[0,1] + sup 0≤x<x+τ≤1 |ϕ(x+ τ)− ϕ(x)| τβ , where C[0, 1] is the space of the all continuous functions ϕ(x) defined on [0,1] with the usual norm ‖ϕ‖C[0,1] = max 0≤x≤1 |ϕ(x)|. It is known that the differential expression [23] ISSN 1027-3190. Укр. мат. журн., 2010, т. 62, № 9 ON A PROBLEM OF DETERMINING THE PARAMETR OF A PARABOLIC EQUATION 1209 Av = −a(x)v′′(x) + δv(x) define a positive operator A acting in Cβ [0, 1] with domain Cβ+2[0, 1] and satisfying the conditions v(0) = v(1), vx(0) = vx(1). Therefore, we can replace the mixed problem (4.4) by the abstract boundary value problem (4.4). Using the results of Theorems 2.1, 3.2, we can obtain that Theorem 4.4. For the solution of the mixed problem (4.4) the following estimates are valid: ‖v‖C1+β,γ 0 (Cµ[0,1]) ≤ M(µ) β(1− β) ‖f‖Cβ,γ0 (Cµ[0,1]), 0 ≤ γ ≤ β < 1, 0 < µ < 1, ‖v‖C1+β,γ 0 (C2(α−β)[0,1]) ≤M(α, β)‖f‖Cβ,γ0 (C2(α−β)[0,1]), ‖p‖C2(α−γ)[0,1] ≤M(α, β, γ)‖f‖Cβ,γ0 (C2(α−β)[0,1]), 0 ≤ γ ≤ β, 0 < 2m(α− β) < 1, where M(µ), M(α, β) and M(α, β, γ) does not depend on f(t, x). The proof of Theorem 4.4 is based on the abstract Theorems 2.1, 3.2 and on the following theorem on the structure of the fractional spaces Eα(A,C[0, 1]). Theorem 4.5 [23]. Eα(A,C[0, 1]) = C2α[0, 1] for all 0 < α < 1 2 . Acknowledgement. The author would like to thank Prof. Pavel Sobolevskii (Jerusa- lem, Israel), for his helpful suggestions to the improvement of this paper. 1. Eidelman Yu. S. Boundary value problems for differential equations with parameters: PhD Thesis (in Russian). – Voronezh, 1984. 2. Eidelman Yu. S. The boundary value problem for differential equations with a parameter // Differents. Uravneniya. – 1978. – 14. – P. 1335–1337. 3. Eidelman Yu. S. Two-point boundary value problem for differential equations with a parameter // Dop. Akad. Nauk Ukr. RSR. Ser. A. – 1983, № 4. – S. 15 – 18. 4. Prilepko A. I. Inverse problems of potential theory // Mat. Zametki. – 1973. – 14. – S. 755 – 767. 5. Iskenderov A. D., Tagiev R. G. The inverse problem of determining the right-hand sides of evolution equations in Banach space // Nauchn. Trudy Azerbaidzhan. Gos. Univ. – 1979. – 1. – S. 51 – 56. 6. Rundell W. 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Укр. мат. журн., 2010, т. 62, № 9
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spelling umjimathkievua-article-29482020-03-18T19:41:02Z On the problem of determining the parameter of a parabolic equation Про задачу визначення параметра параболічного рівняння Ashyralyev, A. Аширалієв, A. We study the boundary-value problem of determining the parameter p of a parabolic equation $$v′(t)+Av(t)=f(t)+p,\;0⩽t⩽1,v(0)=φ,\;v(1)=ψ,$$ with strongly positive operator $A$ in an arbitrary Banach space $E$. The exact estimates are established for the solution of this problem in Hölder norms. In applications, the exact estimates are obtained for the solutions of the boundary-value problems for parabolic equations. Розглянуто крайову задачу визначення параметра р параболічного рівняння $$v′(t)+Av(t)=f(t)+p,\;0⩽t⩽1,v(0)=φ,\;v(1)=ψ,$$ у довільному банаховому просторі е із сильно додатним оператором а. Встановлено точні за нормами Гельдера оцінки для розв&#039;язку цієї задачі. У застосуваннях одержано точні оцінки для розв&#039;язків крайових задач для параболічних рівнянь. Institute of Mathematics, NAS of Ukraine 2010-09-25 Article Article application/pdf https://umj.imath.kiev.ua/index.php/umj/article/view/2948 Ukrains’kyi Matematychnyi Zhurnal; Vol. 62 No. 9 (2010); 1200–1210 Український математичний журнал; Том 62 № 9 (2010); 1200–1210 1027-3190 en https://umj.imath.kiev.ua/index.php/umj/article/view/2948/2646 https://umj.imath.kiev.ua/index.php/umj/article/view/2948/2647 Copyright (c) 2010 Ashyralyev A.
spellingShingle Ashyralyev, A.
Аширалієв, A.
On the problem of determining the parameter of a parabolic equation
title On the problem of determining the parameter of a parabolic equation
title_alt Про задачу визначення параметра параболічного рівняння
title_full On the problem of determining the parameter of a parabolic equation
title_fullStr On the problem of determining the parameter of a parabolic equation
title_full_unstemmed On the problem of determining the parameter of a parabolic equation
title_short On the problem of determining the parameter of a parabolic equation
title_sort on the problem of determining the parameter of a parabolic equation
url https://umj.imath.kiev.ua/index.php/umj/article/view/2948
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