Abstract

In this article, a novel meshless method using space–time radial polynomial basis function (SRPBF) for solving backward heat conduction problems is proposed. The SRPBF is constructed by incorporating time-dependent exponential function into the radial polynomial basis function. Different from the conventional radial basis function (RBF) collocation method that applies the RBF at each center point coinciding with the inner point, an innovative source collocation scheme using the sources instead of the centers is first developed for the proposed method. The randomly unstructured source, boundary, and inner points are collocated in the space–time domain, where both boundary as well as initial data may be regarded as space–time boundary conditions. The backward heat conduction problem is converted into an inverse boundary value problem such that the conventional time–marching scheme is not required. Because the SRPBF is infinitely differentiable and the corresponding derivative is a nonsingular and smooth function, solutions can be approximated by applying the SRPBF without the shape parameter. Numerical examples including the direct and backward heat conduction problems are conducted. Results show that more accurate numerical solutions than those of the conventional methods are obtained. Additionally, it is found that the error does not propagate with time such that absent temperature on the inaccessible boundaries can be recovered with high accuracy.

Highlights

  • Solving a heat conduction problem is to determine temperature histories within the heat–conducting material [1,2,3]

  • For the inner source collocation scheme, it seems that the maximum absolute error (MAE) of the order of 10−7 to 10−9 may be yielded when the terms of the space–time radial polynomial basis function (SRPBF) is in the range of 9 to 16

  • For the outer source collocation scheme, it is clear that the MAE of the order of 10−10 to 10−12 may be yielded when the terms of the SRPBF is in the range of 9 to 16

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Summary

Introduction

Solving a heat conduction problem is to determine temperature histories within the heat–conducting material [1,2,3]. The heat conduction problems are categorized into initial value problems, which have been extensively solved by meshless methods such as the method of fundamental solutions (MFS) [5], the radial basis function collocation method (RBFCM) [6,7,8], Appl. A collocation approach regarding space–time exponential basis functions for wave propagation problems, static and time harmonic elastic problems have been developed [23,24,25]. The pioneering work using the collocation scheme based on the space–time radial polynomial basis function (SRPBF) for modeling the transient heat conduction phenomena is first proposed. Result comparison between the proposed method and that from the RBFCM with the time–marching scheme is conducted.

The Space–time Radial Polynomial Basis Function Collocation Method
Accuracy and Convergence Analysis
A Matrix
Numerical Examples
The Benchmark BHCP
Conclusions
Methods
Full Text
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