Abstract

In this paper, we consider an inverse problem for a linear heat equation involving two time-fractional derivatives, subject to a nonlocal boundary condition. We determine a source term independent of the space variable, and the temperature distribution with an over- determining function of integral type.

Highlights

  • When the initial temperature φ(x) and the source term F (x, t) are given and continuous

  • A solution of the inverse problem is a pair of functions {u(x, t), a(t)} satisfying u(., t) ∈ C2[(0, 1), R], cD0α+ u(x, .),c D0β+ u(x, .) ∈ C ((0, T ], R) such that a ∈ C ((0, T ], R+), satisfying the initial data and the condition (1.4)

  • Our approach to the solvability of the inverse problem (1.1) − (1.4) is based on the expansion of the solution u(x, t) using a biorthogonal system of functions obtained from the eigenfunctions and associated eigenfunctions of the spectral problem (1.5) and its adjoint problem (1.6)

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Summary

Introduction

When the initial temperature φ(x) and the source term F (x, t) are given and continuous. A solution of the inverse problem is a pair of functions {u(x, t), a(t)} satisfying u(., t) ∈ C2[(0, 1), R], cD0α+ u(x, .),c D0β+ u(x, .) ∈ C ((0, T ], R) such that a ∈ C ((0, T ], R+), satisfying the initial data and the condition (1.4). 1-Existence of the solution of the inverse problem: We write the formal solution u(x, t) for the linear system (1.1) − (1.4) in the form u(x, t) = 2u0(t) + u2n−1(t)4 cos (2πnx) + u2n(t)4 (1 − x) sin (2πnx) , n=1 n=1 (3.2)

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