2009
DOI: 10.1007/s00466-009-0389-0
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A new family of time integration methods for heat conduction problems using numerical green’s functions

Abstract: This paper is concerned with the formulation and numerical implementation of a new class of time integration schemes applied to linear heat conduction problems. The temperature field at any time level is calculated in terms of the numerical Green's function matrix of the model problem by considering an analytical time integral equation. After spatial discretization by the finite element method, the Green's function matrix which transfers solution from t to t + t is explicitly computed in nodal coordinates usin… Show more

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Cited by 9 publications
(4 citation statements)
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“…We next consider a two‐dimensional rectangular slab with initial temperature of unity which is uniform over the entire domain 30. One the left boundary ( x = 0), the Dirichlet boundary condition for the temperature is set to zero (cooled side) while all other boundaries are insulated (null heat flux) as depicted in Figure 14(a).…”
Section: Numerical Examplesmentioning
confidence: 99%
“…We next consider a two‐dimensional rectangular slab with initial temperature of unity which is uniform over the entire domain 30. One the left boundary ( x = 0), the Dirichlet boundary condition for the temperature is set to zero (cooled side) while all other boundaries are insulated (null heat flux) as depicted in Figure 14(a).…”
Section: Numerical Examplesmentioning
confidence: 99%
“…Mancuso et al [42] apply continuous Galerkin formulation for time integration of linear heat conduction problems and obtain A-stable integration schemes of higher order. Loureiro and Mansur [40] use SDIRK method to compute a numerical Green's function matrix for the solution of linear heat conduction problems. In the recent study of [24] singly diagonally implicit Runge-Kutta (SDIRK) schemes are compared with backward difference formula of order two (BDF2).…”
Section: Introductionmentioning
confidence: 99%
“…This is indeed the so-called particular or steady-state solution studied by Loureiro and Mansur [15,16], for which the time shape function concerned with the heat load vector is represented exactly into the final solution. The key feature now is to replace the analytical Green's matrix by its numerical counterpart, i.e.,…”
Section: Appendix Amentioning
confidence: 99%
“…In fact, the optimal value is that for which the vertical line in Figure 3 , i.e. equal substeps [13,15], the stability constraint is 4 i t λ ∆ ≤ and iii) for the optimal 1 α , the stability constraint is increased to …”
Section: Time Stability Regionmentioning
confidence: 99%