2017
DOI: 10.1016/j.icheatmasstransfer.2017.04.003
|View full text |Cite
|
Sign up to set email alerts
|

Transient heat transfer analysis of anisotropic material by using Element-Free Galerkin method

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
7
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 32 publications
(7 citation statements)
references
References 15 publications
0
7
0
Order By: Relevance
“…We assume that Ω s is a 3D space domain bounded by a surface 𝜕Ω s = Γ, where Γ = Γ D ∪ Γ N and Γ D ∩ Γ N = ∅. Considering the transient heat conduction problem in anisotropic media in Ω s , the function T(x, t) describing the transient temperature distribution satisfies the following governing equation, 18,39 𝜌c 𝜕T(x, t)…”
Section: Problem Statementmentioning
confidence: 99%
See 1 more Smart Citation
“…We assume that Ω s is a 3D space domain bounded by a surface 𝜕Ω s = Γ, where Γ = Γ D ∪ Γ N and Γ D ∩ Γ N = ∅. Considering the transient heat conduction problem in anisotropic media in Ω s , the function T(x, t) describing the transient temperature distribution satisfies the following governing equation, 18,39 𝜌c 𝜕T(x, t)…”
Section: Problem Statementmentioning
confidence: 99%
“…We assume that Ωs$$ {\Omega}_s $$ is a 3D space domain bounded by a surface Ωs=normalΓ$$ \partial {\Omega}_s=\Gamma $$, where normalΓ=ΓDΓN$$ \Gamma ={\Gamma}_D\cup {\Gamma}_N $$ and ΓDΓN=$$ {\Gamma}_D\cap {\Gamma}_N=\varnothing $$. Considering the transient heat conduction problem in anisotropic media in Ωs$$ {\Omega}_s $$, the function T(boldx,t)$$ T\left(\mathbf{x},t\right) $$ describing the transient temperature distribution satisfies the following governing equation, 18,39 ρcT(boldx,t)tgoodbreak=Dij2T(boldx,t)xixjgoodbreak+Q(boldx,t),1.5emboldxΩs,1emt[]t0,tf,$$ \rho c\frac{\partial T\left(\mathbf{x},t\right)}{\partial t}={D}_{ij}\frac{\partial^2T\left(\mathbf{x},t\right)}{\partial {x}_i\partial {x}_j}+Q\left(\mathbf{x},t\right),\kern1.5em \mathbf{x}\in {\Omega}_s,\kern1em t\in \left[{t}_0,{t}_f\right], $$ where boldx=()x1,x2,x3$$ \m...…”
Section: Problem Statementmentioning
confidence: 99%
“…, C M over the main boundary ∂ and we assume that M ≥ N. By satisfying Eqs. (8) and ( 9) at all collocation points on the boundary, the following system of linear equations are obtained:…”
Section: The Mfs Formulation For Two-dimensional Anisotropic Elasticitymentioning
confidence: 99%
“…Meshfree methods can be classified into two major categories [4]. The first category includes meshfree methods based on strong forms of differential equations [5][6][7], while the meshfree methods based on weak forms of governing equations [8,9] fall into the second category. The weak-form meshfree methods need suitable techniques for the computation of domain integrals [10][11][12]; however, the MFS is a strong-form and truly meshfree method without any need for evaluating any domain or boundary integral.…”
Section: Introductionmentioning
confidence: 99%
“…Studies dealing with thermal properties of wood materials focused mostly on determining the effect of density, temperature, and MC on thermal conductivity, thermal diffusivity, and specific heat capacity [24][25][26].…”
Section: Introductionmentioning
confidence: 99%