Ryszard Białecki

Prof. Ryszard Białecki

Department of Thermal Technology, Silesian University of Technology, PL-44-100 Gliwice, Poland

Research Focus & Metrics

Academic Career Length

46Years (1981-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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18 November 2004 in International Journal for Numerical Methods in Engineering
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Journal Article
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Ryszard BiałeckiRyszard Białecki
Ryszard Białecki
AKA. J. Kassab
A. J. Kassab
AFA. Fic
A. Fic

1 December 1981 in Applied Mathematical Modelling
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Journal Article
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Ryszard BiałeckiRyszard Białecki
Ryszard Białecki
Andrzej J. NowakAndrzej J. Nowak
Andrzej J. Nowak

1 August 2005 in Numerical Heat Transfer, Part B: Fundamentals
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Journal Article
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AFAdam Fic
Adam Fic
Ryszard BiałeckiRyszard Białecki
Ryszard Białecki
AKAlain J. Kassab
Alain J. Kassab
A method of reducing the number of degrees of freedom and the overall computing time by combining proper orthogonal decomposition (POD) with the finite-element method (FEM) has been devised. The POD-FEM technique can be applied both to linear and nonlinear problems. At the first stage of the method a standard FEM time-stepping procedure is invoked. The temperature fields obtained for the first few time steps undergo statistical analysis, yielding an optimal set of globally defined trial and weighting functions for the Galerkin solution of the problem at hand. The resulting set of ordinary differential equations (ODEs) is of greatly reduced dimensionality when compared with the original FEM formulation. For linear problems, the set can be solved either analytically, resorting to the modal analysis technique, or by time stepping. In the case of nonlinear problems, only time stepping can be applied. The focus of this article is on the time-stepping approach, in which the generation of the FEM-POD matrices, requiring some additional matrix manipulations, can be embedded in the assembly of standard FEM matrices. The gain in execution times comes from the significantly shorter time of solution of the set of algebraic equations at each time step. Numerical results are presented for both linear and nonlinear problems. In the case of linear problems, the derived time-stepping technique is compared with the standard FEM and the modal analysis. For nonlinear problems the proposed POD-FEM approach is compared with the standard FEM. Good accuracy of the POD-FEM solver has been observed. Controlling the error introduced by the reduction of the degrees of freedom in POD is also discussed.

1 October 2014 in Particuology
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Journal Article
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WAWojciech Adamczyk
Wojciech Adamczyk
GWGabriel Węcel
Gabriel Węcel
MKMarcin Klajny
Marcin Klajny
PKPaweł Kozołub
Paweł Kozołub
AKAdam Klimanek
Adam Klimanek
Ryszard BiałeckiRyszard Białecki
Ryszard Białecki

1 August 2014 in Particuology
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Journal Article
Closed access
WAWojciech Adamczyk
Wojciech Adamczyk
AKAdam Klimanek
Adam Klimanek
Ryszard BiałeckiRyszard Białecki
Ryszard Białecki
GWGabriel Węcel
Gabriel Węcel
PKPaweł Kozołub
Paweł Kozołub
Tomasz CzakiertTomasz Czakiert
Tomasz Czakiert

1 January 2008 in Inverse Problems in Science and Engineering
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Journal Article
Closed access
ZOZiemowit Ostrowski
Ziemowit Ostrowski
Ryszard BiałeckiRyszard Białecki
Ryszard Białecki
AKA. J. Kassab
A. J. Kassab
The article presents advances in the approach aiming to solve inverse problems of steady state and transient heat conduction. The regularization of ill-posed problem comes from the proper orthogonal decomposition (POD). The idea is to expand the direct problem solution into a sequence of orthonormal basis vectors, describing the most significant features of spatial and time variation of the temperature field. Due to the optimality of proposed expansion, the majority of the basis vectors can be discarded practically without accuracy loss. The amplitudes of this low-order expansion are expressed as a linear combination of radial basis functions (RBF) depending on both retrieved parameters and time. This approximation, further referred as trained POD-RBF network is then used to retrieve the sought-for parameters. This is done by resorting to least square fit of the network and measurements. Numerical examples show the robustness and numerical stability of the scheme.