2008
DOI: 10.1016/j.compstruct.2007.07.004
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Two-dimensional elasticity solutions for functionally graded beams resting on elastic foundations

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Cited by 238 publications
(94 citation statements)
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“…According to this technique, the M th term approximate solution of (2), (8) is sought in the form (9) where ( ) i Q t are coordinates in modal space and ( ) i P x are the normal modes of vibration written as (10) No difficulty arises at all to show that for a beam with simply supported end conditions, taking into account equation (10), equation (9) can be written as (11) Substituting equation (11) into the governing equation (8), one obtains (12 ) which after some simplifications and rearrangements yields (13) To determine the expression for ( ) i Q t , the expression on the LHS of equation (13) is required to be orthogonal to the function . Thus, multiplying equation (13) by and integrating with respect to x from x=0 to x=L, leads to (14) where , , (16) and considering only the i th particle of the system, equation (14) can then be written as (17) where , and (18) To obtain the solution of the equation (17), it is subjected to a Laplace transform defined as (19) where s is the Laplace parameter. Applying the initial conditions (3), one obtains the simple algebraic equation given as In what follows, we seek to find the Laplace inversion of equation (21).…”
Section: Solution Proceduresmentioning
confidence: 99%
See 1 more Smart Citation
“…According to this technique, the M th term approximate solution of (2), (8) is sought in the form (9) where ( ) i Q t are coordinates in modal space and ( ) i P x are the normal modes of vibration written as (10) No difficulty arises at all to show that for a beam with simply supported end conditions, taking into account equation (10), equation (9) can be written as (11) Substituting equation (11) into the governing equation (8), one obtains (12 ) which after some simplifications and rearrangements yields (13) To determine the expression for ( ) i Q t , the expression on the LHS of equation (13) is required to be orthogonal to the function . Thus, multiplying equation (13) by and integrating with respect to x from x=0 to x=L, leads to (14) where , , (16) and considering only the i th particle of the system, equation (14) can then be written as (17) where , and (18) To obtain the solution of the equation (17), it is subjected to a Laplace transform defined as (19) where s is the Laplace parameter. Applying the initial conditions (3), one obtains the simple algebraic equation given as In what follows, we seek to find the Laplace inversion of equation (21).…”
Section: Solution Proceduresmentioning
confidence: 99%
“…Beams on elastic foundation and under the actions of the moving loads have received a considerable attention in literature; see for example references [10][11][12][13][14][15][16][17][18]. However, most of these works employed the simplest mechanical model which was developed by Winkler and generally referred to as a one-parameter model.…”
mentioning
confidence: 99%
“…The first group used analytical and semi-analytical methods to study the bending and vibrations of FG beams resting on elastic foundations. Ying et al (2008) presented exact solutions for functionally graded simply supported beams resting on a Winkler-Pasternak elastic foundation based on the two-dimensional theory of elasticity. Fallah and Aghdam (2011) studied the free vibration and post-buckling of FG beams on nonlinear elastic foundations subject to axial loads.…”
Section: Introductionmentioning
confidence: 99%
“…The displacement of the beam is determined as the linear combination of a Fourier series and an auxiliary polynomial function. Ying et al investigated the precise solutions for free vibration and bending of functionally graded beams on a Winkler-Pasternak elastic foundation (Ying et al, 2008). The beam is considered as orthotropic at any point, while material properties varying exponentially along the thickness direction.…”
Section: Introductionmentioning
confidence: 99%