UTMS 2003 – 14 March 31 , 2003 On the determination of wave speed and potential in a hyperbolic equation by two measurements

نویسنده

  • M. Yamamoto
چکیده

We discuss a problem of finding a speed of sound c(x) and a potential q(x) in a second-order hyperbolic equation from two boundary observations. The coefficients are assumed to be unknown inside a disc in R. On a suitable bounded part of the cylindrical surface, we are given Cauchy data for solutions to a hyperbolic equation with zero initial data and sources located on the lines {(x, t) ∈ R3|x · ν = 0, t = 0} for two distinct unit vectors ν = ν, k = 1, 2. We obtain a conditional stability estimate under a priori assumptions on smallness of c(x)− 1 and q(x). §1. Statement of the inverse problem and main results In the papers [2], [6] [9], a new method for obtaining conditional stability estimates for problems related to determination of coefficients for linear hyperbolic equations has been proposed. This method uses a single observation for finding one unknown coefficient. By our method, we can prove the stability in determining coefficients by means of a finite number of measurements where initial data are zero and impulsive inputs are added. As other methodology for inverse problems with a finite number of measurements, we refer to [1], [4], [5] and the references therein. However in those papers, we have to assume some positivity or non-degeneracy of initial values, which is not practical. For our method, we need not such restrictions on initial data, which is very practical. On the other hand, we have to assume that unknown coefficients should be close to fixed reference coefficients which are constant. An analysis shows that the problem with several unknown coefficients under the derivatives of the first order can also be successfully studied by this method (see [7], [8]). However its application to determination of coefficients under derivatives of different orders meets some Sobolev Institute of Mathematics of Siberian Division of Russian Academy of Sciences, Acad. Koptyug prospekt 4, 630090 Novosibirsk Russia; e-mail: [email protected] Graduate School of Mathematical Sciences, The University of Tokyo, 3-8-1 Komaba, Meguro, Tokyo, 153 Japan; e-mail: [email protected] 1 difficulties. Recently the problems of finding a damping coefficient and a potential from two measurements, and the speed of sound and damping, were considered in papers [3] and [10], respectively. In this paper, by two measurements, we consider the inverse problem where coefficients of the leading term and the lowest term are unknown. The technique of this paper differs from [3] and [10], but keeps some common features with them. Let u = u(x, t), x ∈ R, satisfy the equation utt − c(∆u+ qu) = 2δ(t) δ(x · ν), (x, t) ∈ R, (1.1) and the zero initial condition u|t<0 = 0. (1.2) Here ν is a unit vector and the symbol x · ν means the scalar product of the vectors x and ν. The solution to problem (1.1) (1.2) depends on the parameter ν, i.e., u = u(x, t, ν). Assume that supports of the coefficients q(x) and c(x) − 1 are located strictly inside the disc B := {x ∈ R2| |x− x0| < r} and B belongs to the half-plane x · ν > 0. Suppose also that q(x) and c(x) > 0 are smooth functions in R (see below). Introduce the function τ(x, ν) as the solution to the following problem for the eikonal equation: |∇τ |2 = c−2(x), τ |x·ν=0 = 0. (1.3) Let G(ν) be the cylindrical domain G(ν) := {(x, t)| x ∈ B, τ(x, ν) < t < T + τ(x, ν)} where T is a positive number. Denote by S(ν) the lateral boundary of this domain and by Σ0(ν) and ΣT (ν) the lower and upper basements, respectively. That is, S(ν) := {(x, t)| x ∈ ∂B, τ(x, ν) ≤ t ≤ T + τ(x, ν)}, Σ0(ν) := {(x, t)| x ∈ B, t = τ(x, ν)}, ΣT (ν) := {(x, t)| x ∈ B, t = T + τ(x, ν)}, ∂B := {x ∈ R2| |x− x0| = r}. Consider the problem of determination of q(x) and c(x). Let the following information be known. We take distinct unit vectors ν and ν such that B belongs to the half plane x · ν > 0 for k = 1, 2. Then we are given the traces of the functions τ(x, ν) on ∂B, and 2 the traces on S(ν) := Sk of solutions and its normal derivatives to problem (1.1) (1.2) with ν = ν, that is, u(x, t, ν) = f (x, t), ∂ ∂n u(x, t, ν) = g(x, t), (x, t) ∈ Sk; τ(x, ν) = τ (x), x ∈ ∂B; k = 1, 2. (1.4) The problem is: find q(x) and c(x) from given data, i.e., from f , g, τ , k = 1, 2. For fixed constants q0 > 0 and d > 0, let Λ(q0, d) be the set of functions (q, c) satisfying the following two conditions: 1) supp q(x), supp (c(x)− 1) ⊂ Ω ⊂ B, dist(∂B,Ω) ≥ d, 2) ‖q‖C17(Rn) ≤ q0, ‖c− 1‖C19(Rn) ≤ q0. In particular, we note that ν and ν are linearly independent. We prove here the following stability and uniqueness theorems. Theorem 1.1. Let (qj, cj) ∈ Λ(q0, d), and let {f (k) j , g j , τ (k) j } be the data corresponding to the solution to (1.1) (1.2) with q = qj(x), c = cj(x) and ν = ν , k, j = 1, 2. Moreover let the condition 4r/T < 1 be satisfied. Then there exist positive numbers q∗ and C depending on T , r, d and |ν (1) − ν (2)| such that for all q0 ≤ q∗ the following inequality holds: ‖q1 − q2‖L2(B) + ‖c1 − c2‖H2(B) ≤ C 2 ∑ k=1 ( ‖f̂ (k) 1 − f̂ (k) 2 ‖H3(∂B×{0}) + ‖(f̂ (k) 1 − f̂ (k) 2 )t‖H2(∂B×(0,T )) (1.5) +‖(ĝ 1 − ĝ 2 )t‖H1(∂B×(0,T )) + ‖τ (k) 1 − τ (k) 2 ‖H5(∂B) ) , where f̂ (k) j (x, t) = f (k) j (x, t− τ (k) j (x)) and ĝ j (x, t) = g j (x, t− τ (k) j (x)). Theorem 1.2. Let the conditions the Theorem 1.1 be fulfilled. Then one can find a number q∗ > 0 such that if (qj , cj) ∈ Λ(q∗, d), j = 1, 2, and the corresponding data partly coincide, namely, f (k) 1 (x, t) = f (k) 2 (x, t), (x, t) ∈ Sk; τ (k) 1 (x) = τ (k) 2 (x), x ∈ ∂B; k = 1, 2, (1.6)

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Thermoelastic Interaction in a Three-Dimensional Layered Sandwich Structure

The present article investigates the thermoelastic interaction in a three-dimensional homogeneous and isotropic sandwich structure using the dual-phase-lag (DPL) model of generalized thermoelasticity. The incorporated resulting non-dimensional coupled equations are applied to a specific problem in which a sandwich layer of unidentical homogeneous and isotropic substances is subjected to time-de...

متن کامل

Wave Equations in Transversely Isotropic Media in Terms of Potential Functions (RESEARCH NOTE)

A complete series of potential functions for solving the wave equations in an almost transversely isotropic media is presented. The potential functions are reduced to only one potential function particularly for axisymmetric wave propagation problems. The potential functions presented in this paper can be reduced to Lekhnitskii-Hu-Nowacki solution for elastostatics problems.

متن کامل

Numerical studies of non-local hyperbolic partial differential equations using collocation methods

The non-local hyperbolic partial differential equations have many applications in sciences and engineering. A collocation finite element approach based on exponential cubic B-spline and quintic B-spline are presented for the numerical solution of the wave equation subject to nonlocal boundary condition. Von Neumann stability analysis is used to analyze the proposed methods. The efficiency, accu...

متن کامل

Large Scale Experiments Data Analysis for Estimation of Hydrodynamic Force Coefficients

This paper describes the various frequency domain methods which may be used to analyze experiments data on the force experienced by a circular cylinder in wave and current to estimate drag and inertia coefficients for use in Morison’s equation. An additional approach, system identification techniques (SIT) is also introduced. A set of data obtained from experiments on heavily roughened circular...

متن کامل

Comparison of the hyperbolic range of two-fluid models on two-phase gas -liquid flows

In this paper, a numerical study is conducted in order to compare hyperbolic range of equations of isotherm two-fluid model governing on two-phase flow inside of pipe using conservative Shock capturing method. Differential equations of the two-fluid model are presented in two forms (i.e. form I and form II). In forms I and II, pressure correction terms are hydrodynamic and hydrostatic, respecti...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2003