Solving the Axisymmetric Inverse Heat Conduction Problem by a Wavelet Dual Least Squares Method
© W. Cheng and C.-L. Fu. 2009
Received: 17 August 2008
Accepted: 10 March 2009
Published: 17 March 2009
We consider an axisymmetric inverse heat conduction problem of determining the surface temperature from a fixed location inside a cylinder. This problem is ill-posed; the solution (if it exists) does not depend continuously on the data. A special project method—dual least squares method generated by the family of Shannon wavelet is applied to formulate regularized solution. Meanwhile, an order optimal error estimate between the approximate solution and exact solution is proved.
Inverse heat conduction problems (IHCP) have become an interesting subject recently, and many regularization methods have been developed for the analysis of IHCP [1–13]. These methods include Tikhonov method [1, 2], mollification method [3, 4], optimal filtering method , lines method , wavelet and wavelet-Galerkin method [7–11], modified Tikhonov method  and "optimal approximations" , and so forth. However, most analytical and numerical methods were only used to dealing with IHCP in semiunbounded region. Some works of numerical methods were presented for IHCP in bounded domain [14–19].
Chen et al.  applied the hybrid numerical algorithm of Laplace transform technique to the IHCP in a rectangular plate. Busby and Trujillo  used the dynamic programming method to investigate the IHCP in a slab. Alifanov and Kerov  and Louahlia-Gualous et al.  researched IHCP in a cylinder. However to the authors' knowledge, most of them did not give any stability theory and convergence proofs.
where the functions and belong to for every fixed , is the radial coordinate, denotes the temperature history at one fixed radius of cylinder. We want to recover for . This problem is ill-posed problem; a small perturbation in the data may cause dramatically large errors in the solution (The details can be seen in Section 2).
To the authors' knowledge, up to now, there is no regularization theory with error estimate for problem (1.1) in the interval . The major objective of this paper is to do the theoretic stability and convergence estimates for problem (1.1).
Xiong and Fu  and Regińska  solved the sideways heat equation in semi-unbounded region by applying the wavelet dual least squares method, which is based on the family of Meyer wavelet. In this paper, we will apply a wavelet dual least squares method generated by the family of Shannon wavelet to problem (1.1) in bounded domain for determining surface temperature. According to the optimality results of general regularization theory, we conclude that our error estimate on surface temperature is order optimal.
2. Formulation of Solution of Problem (1.1)
Then we have the following lemma.
Substitution of in (2.16) into (2.12), we obtain (2.8).
In order to obtain ill-posedness of problem (1.1) for , we need the following lemma.
Finally, combining inequalities (2.22) with (2.23), we can see that there exist others constants and such that, for , inequalities (2.18) are valid. Similarly, we obtain inequalities (2.19).
From (2.26), we can prove the following lemma.
Hence the conclusion of Lemma 2.3 is proved.
This implies that , which is Fourier transform of exact data , must decay rapidly at high frequencies since . But such a decay is not likely to occur in the Fourier transform of the measured noisy data at . So, small perturbation of in high frequency components can blow up and completely destroy the solution given by (2.17) for .
3. Wavelet Dual Least Squares Method
3.1. Dual Least Squares Method
3.2. Shannon Wavelets
From (3.9), can be seen as a low-pass filter. The frequencies with greater than are filtered away.
Hence the conclusion of Theorem3.1 is proved.
4. Error Estimates via Dual Least Squares Method Approximation
Now we will devote to estimating the error .
Hence the conclusion of Theorem 4.1 is proved.
The following is the main result of this paper.
Hence the conclusion of Theorem 4.2 is proved.
- (i)When and , estimate (4.8) is a Hölder stability estimate given by(4.12)
When , estimate (4.8) is a logarithmical Hölder stability estimate.
- (iii)When , estimate (4.3) becomes(4.13)
This is a logarithmical stability estimate.
The work is supported by the National Natural Science Foundation of China (No. 10671085), the Hight-level Personnel fund of Henan University of Technology (2007BS028), and the Fundamental Research Fund for Natural Science of Education Department of Henan Province of China (No. 2009B110007).
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