2011
DOI: 10.1016/j.compositesb.2011.05.030
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Electric-thermal link finite element made of a FGM with spatial variation of material properties

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Cited by 8 publications
(4 citation statements)
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“…However, pristine PCMs commonly exhibit low electrical conductivity and thermal conductivity, which restrict their applications. To overcome these deficiencies, various electrically and thermally conductive fillers including metal materials (Cu, Ag, Au, Al, Ni) and carbon materials (CNTs, graphene, expanded graphite) have been introduced into the PCM system. The electrons in the outer layer of metal atoms have strong delocalization and move under the action of an external electric field, thus generating an electric current. Electrons in the p orbital of parallel carbon atoms in one layer form large-scale delocalized π bonds, and the electrons can move freely in the lattice.…”
Section: Mechanismsmentioning
confidence: 99%
“…However, pristine PCMs commonly exhibit low electrical conductivity and thermal conductivity, which restrict their applications. To overcome these deficiencies, various electrically and thermally conductive fillers including metal materials (Cu, Ag, Au, Al, Ni) and carbon materials (CNTs, graphene, expanded graphite) have been introduced into the PCM system. The electrons in the outer layer of metal atoms have strong delocalization and move under the action of an external electric field, thus generating an electric current. Electrons in the p orbital of parallel carbon atoms in one layer form large-scale delocalized π bonds, and the electrons can move freely in the lattice.…”
Section: Mechanismsmentioning
confidence: 99%
“…Figure 2a presents simple link / beam FGM structure for which new FEM equations for coupled electro-thermo-mechanical analysis will be derived. Prior to the derivation process of the new FEM equations it is necessary to implement homogenization techniques (extended mixture rule [1] and multilayer method [2,3]) that convert spatial change of material properties (caused by chosen mixture of the constituents) into equivalent one-dimensional change of material properties for each link or beam of the FGM actuator structure. This 1D change of effective material properties is only in longitudinal direction (x axis) of the link / beam, Figure 2b.…”
Section: Fem Equations For Coupled Electro -Thermo -Mechanical Analysismentioning
confidence: 99%
“…Many studies have been devoted to the static and dynamic analysis of FGM beams [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18], FGM axial bars [19], FGM torsional bars [20], FGM plates [21], and FGM annular circular plates and disks [22,23]. In these studies, the material properties of one-dimensional (1-D) FGM structures were assumed to vary across the thickness (or radial) direction only [1][2][3][4][5][6][7][8][9]20], in the axial direction only [10][11][12]19], or in both the axial and thickness (or radial) directions [13,14].…”
Section: Introductionmentioning
confidence: 99%
“…In these studies, the material properties of one-dimensional (1-D) FGM structures were assumed to vary across the thickness (or radial) direction only [1][2][3][4][5][6][7][8][9]20], in the axial direction only [10][11][12]19], or in both the axial and thickness (or radial) directions [13,14]. In the literature, various solution methods have been applied to static and dynamic analyses of FGM structures; these include analytical methods [1][2][3][4]15,[20][21][22], the Rayleigh-Ritz method [16], the modal analysis method [10,14], power series expansion methods [11,19], the differential quadrature method [14], the dynamic stiffness method [23], the finite element method (FEM) [5][6][7][8][9]12,17,18], and the spectral element method [24].…”
Section: Introductionmentioning
confidence: 99%