2017
DOI: 10.1007/s40995-017-0240-y
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Boundary Determination of the Inverse Heat Conduction Problem in One and Two Dimensions via the Collocation Method Based on the Satisfier Functions

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Cited by 7 publications
(5 citation statements)
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“…[17][18][19] In the present contribution, we use a spectral technique [53][54][55][56][57][58][59] which is a powerful tool to provide more accurate and at the same time stable numerical solution for the inverse problems (1.1)- (1.5). By applying the satisfier function 21,[60][61][62][63][64][65] which fulfills all the initial and boundary conditions and employing this function within a linear transformation, we get an equivalent problem with the homogeneous initial and boundary conditions. We expand the desired unknown function in terms of orthonormal Bernstein basis functions (OBBFs); the operational matrices 21,[66][67][68][69][70][71][72] of integration and differentiation of these polynomials are utilized to formulate the discrete version of the problem.…”
Section: Literature Reviewmentioning
confidence: 99%
“…[17][18][19] In the present contribution, we use a spectral technique [53][54][55][56][57][58][59] which is a powerful tool to provide more accurate and at the same time stable numerical solution for the inverse problems (1.1)- (1.5). By applying the satisfier function 21,[60][61][62][63][64][65] which fulfills all the initial and boundary conditions and employing this function within a linear transformation, we get an equivalent problem with the homogeneous initial and boundary conditions. We expand the desired unknown function in terms of orthonormal Bernstein basis functions (OBBFs); the operational matrices 21,[66][67][68][69][70][71][72] of integration and differentiation of these polynomials are utilized to formulate the discrete version of the problem.…”
Section: Literature Reviewmentioning
confidence: 99%
“…To contribute the boundary conditions () in computations, we define the satisfier function 54,55,59,66,79 as s ( x , t ) = g 1 ( t ) + x ( g 2 ( t ) − g 1 ( t ))and consider the approximate solution of u ( x , t )as uKKfalse(x,tfalse)xfalse(x1false)truei=0Ktruej=0Kcijϕifalse(xfalse)ψjfalse(tfalse)+sfalse(x,tfalse)=xfalse(x1false)ϕTfalse(xfalse)Cψfalse(tfalse)+ϕTfalse(xfalse)Sψfalse(tfalse), where ϕTfalse(xfalse)=[]ϕ0false(xfalse),ϕ1false(xfalse),,ϕKfalse(xfalse) and ψfalse(tfalse)=[]ψ0false(tfalse),ψ1false(tfalse),,ψKfalse(tfalse)T are the vectors including the orthonormal basis functions defined over the intervals [0, 1]and [0, t f ], respectively and C=()center center centerarrayc00arrayarrayc0KarrayarrayarrayarraycK0arrayarraycKK, is the coefficient matrix including the unknown parameter...…”
Section: Solution Proceduresmentioning
confidence: 99%
“…Operational matrices have been used as an efficient tool in the context of spectral methods such as Tau method and Ritz-Galerkin method. 36,37,[44][45][46][47][48][49][50][51][52][53][54][55][56][57][58][59][60][61][62] These techniques provide a general approach based on expanding the approximate solution of the unknown functions in terms of the basis functions with unknown coefficients. Then, the operational matrices of the integration, differentiation, and product regarding the considered basis functions are utilized to tackle integral, differential, and nonlinear terms included in the problem.…”
Section: Literature Reviewmentioning
confidence: 99%
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