2010
DOI: 10.1016/j.compstruct.2009.12.016
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Vibration analysis of radially FGM sectorial plates of variable thickness on elastic foundations

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Cited by 71 publications
(23 citation statements)
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“…To calculate basic displacement functions, the differential equations governing higher-order shear deformable beam must be solved with respect to transverse displacement of the beam, i.e., w. Since closed-form solution for governing differential equation of higher-order shear deformable beams is not attainable, it is necessary to resort application of numerical methods such as Rayleigh-Ritz method [28], differential quadrature method (DQM) [29], differential quadrature element method (DQEM) [30], least-square-based finite difference (LSFD) [31], methods based on the green functions [32] and differential transform method (DTM) [33].…”
Section: Introductionmentioning
confidence: 99%
“…To calculate basic displacement functions, the differential equations governing higher-order shear deformable beam must be solved with respect to transverse displacement of the beam, i.e., w. Since closed-form solution for governing differential equation of higher-order shear deformable beams is not attainable, it is necessary to resort application of numerical methods such as Rayleigh-Ritz method [28], differential quadrature method (DQM) [29], differential quadrature element method (DQEM) [30], least-square-based finite difference (LSFD) [31], methods based on the green functions [32] and differential transform method (DTM) [33].…”
Section: Introductionmentioning
confidence: 99%
“…This has been addressed by in [7][8][9] for axially graded Euler-Bernoulli and Timoshenko beams. It has also been fully discussed for radially FGM circular plates by Sahraee [10], Shariyat and Alipour [11] and Hosseini-Hashemi et al [12], [13]. However, information about rectangular plates with in-plane inhomogeneity is very limited.…”
Section: Introductionmentioning
confidence: 99%
“…The plate middle surface is described by the following position vector r(x, ϑ) = (R i + x) cos ϑ e 1 − (R i + x) sin ϑ e 2 (91) where x, ϑ are the principal coordinate of the surface, assuming x ∈ [0, L] and ϑ ∈ [0, 2π]. The inner radius is denoted by R i , whereas the outer one can be computed as R out = R i + L. A linear variation is applied along the radial direction to define the thickness profile…”
Section: Comparison With the Literaturementioning
confidence: 99%
“…Several thickness profiles, as well as volume fraction distributions, were considered. The same kind of FGM structures resting on the Pasternak elastic foundation were investigated also by Hosseini-Hashemi et al [91] and by Tajeddini et al [92]. In the first paper, the differential quadrature method was used to solve numerically the governing equations based on the classical plate theory, whereas the free vibration problem was solved by means of the polynomial-Ritz method in the second paper.…”
Section: Introductionmentioning
confidence: 99%