2003
DOI: 10.1080/1068276031000114884
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Multidimensional inverse heat conduction problems solution via lagrange theory and model size reduction techniques

Abstract: This article is concerned with inverse heat conduction problems (IHCP) involving large-scale linear systems (i.e. multidimensional systems) with unknown sources or boundary conditions. The inverse problem is stated as an optimisation problem with a regularised quadratic objective functional, and it is solved using Lagrange theory. We demonstrate that the IHCP solution is obtained by simple time integration of a state-variable model: the inverse model, which is analytically derived from the so called direct and… Show more

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Cited by 16 publications
(9 citation statements)
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References 22 publications
(38 reference statements)
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“…[26]) that the minimum of J is achieved when the following three problems are satisfied simultaneously: ðaÞ Direct problem : dTðtÞ=dt ¼ ATðtÞ þ BWðtÞ; ð12Þ ðbÞ Adjoint problem : ÀdkðtÞ=dt ¼ A 0 kðtÞ þ C 0 CTðtÞ À C 0 y m ðtÞ; ð13Þ ðcÞ Stationarity condition : WðtÞ ¼ ÀR À1 B 0 kðtÞ ð 14Þ with T(0) = T o and k(t f ) = 0. T(t) (n  1) and k(t) (n  1) are respectively the PCM thermal state vector and the so called co-state vector (as previously, n is the number of nodes in the discretisation mesh).…”
Section: Problem Solutionmentioning
confidence: 99%
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“…[26]) that the minimum of J is achieved when the following three problems are satisfied simultaneously: ðaÞ Direct problem : dTðtÞ=dt ¼ ATðtÞ þ BWðtÞ; ð12Þ ðbÞ Adjoint problem : ÀdkðtÞ=dt ¼ A 0 kðtÞ þ C 0 CTðtÞ À C 0 y m ðtÞ; ð13Þ ðcÞ Stationarity condition : WðtÞ ¼ ÀR À1 B 0 kðtÞ ð 14Þ with T(0) = T o and k(t f ) = 0. T(t) (n  1) and k(t) (n  1) are respectively the PCM thermal state vector and the so called co-state vector (as previously, n is the number of nodes in the discretisation mesh).…”
Section: Problem Solutionmentioning
confidence: 99%
“…This problem can be easily solved using the ''sweep method'' [26,27], which assumes that kðtÞ and T(t) satisfy an affine relation like k(t) = S 1 T(t) + v(t) for some as yet unknown matrix function S 1 and vector function v(t). The solution of the inverse problem is then given by (cf.…”
Section: Problem Solutionmentioning
confidence: 99%
“…Zmywaczyk [4] applied the modified Newton-Raphson method to determine temperature-dependent thermophysical properties (k r , k z , ρc p ) of an orthotropic material. Del Barrio [5] identified heat sources in a 2D diffusion problem by the Lagrange theory. Pohanka et al [6] applied the simplex method to determine the temperature-dependent thermal properties (k, ρc p ) of a fused silica shell.…”
Section: Introductionmentioning
confidence: 99%
“…Powerful model reduction techniques based on PCA/KLD/SVD have been also proposed for lowdimensional description of problems described by partial differential equations, mostly in the field of turbulent flows [12,13]. In thermal analysis, SVD-based methods have been developed for efficient reduction of linear and non-linear heat transfer problems [14][15][16][17][18], as well as for solving heat transfer inverse problems dealing with unknown heat sources [19][20][21]. For a fairly comprehensive introduction to PCA/KLD/SVD, we recommend the books by Jolliffe [22] and Deprettere [8].…”
Section: Introductionmentioning
confidence: 99%