2017
DOI: 10.1002/nme.5604
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Element differential method and its application in thermal‐mechanical problems

Abstract: SummaryIn this paper, a new numerical method, element differential method (EDM), is proposed for solving general thermal-mechanical problems. The key point of the method is the direct differentiation of the shape functions of Lagrange isoparametric elements used to characterize the geometry and physical variables. A set of analytical expressions for computing the first-and second-order partial derivatives of the shape functions with respect to global coordinates are derived. Based on these expressions, a new c… Show more

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Cited by 47 publications
(27 citation statements)
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“…After solving the system, we can use eqns (25) and (24) to calculate T . Thus, all the unknowns of computational domain can be obtained.…”
Section: Boundary Element Methodsmentioning
confidence: 99%
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“…After solving the system, we can use eqns (25) and (24) to calculate T . Thus, all the unknowns of computational domain can be obtained.…”
Section: Boundary Element Methodsmentioning
confidence: 99%
“…Recently, a new numerical method called element differential method (EDM) is proposed by Gao et al [23]- [25] and Cui et al [26]. It is also a flexible method like FEM and can be used in most engineering problems.…”
Section: Introductionmentioning
confidence: 99%
“…The formula of shape functions and its first or second order can be obtained in the reference papers [11,12].…”
Section: Using Edm To Discretize the Governing Equationsmentioning
confidence: 99%
“…In recent years, Gao et al [11][12][13][14][15][16][17][18][19][20] proposed a new strong-form numerical method called element differential method (EDM). Like traditional FEM, EDM also uses isoparametric elements to discretize the computational domain and approximate physical variables.…”
Section: Introductionmentioning
confidence: 99%
“…Then, we transform the irregular element into a regular domain as done in FEM. The variables and Cartesian coordinates can be obtained by interpolation ϕtrue‾=Nifalse(boldξfalse)ϕi,x=Nifalse(boldξfalse)boldxi, where x=false(x1x2xNDfalse) and ξ=false(ξ1ξ2ξNDfalse) represent the Cartesian coordinates and Natural coordinates, respectively, N i represents interpolation functions or called the shape functions in FEM which can be found in References 36 in detail, and N D represent the spatial dimension of the problem. For 3D problem, ( x 1 , x 2 , x 3 ) = ( x , y , z ) and ( ξ 1 , ξ 2 , ξ 3 ) = ( ξ , η , ζ ).…”
Section: Momentum Equationmentioning
confidence: 99%