2015
DOI: 10.1007/s12205-015-0252-0
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A new higher order shear deformation model for functionally graded beams

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Cited by 20 publications
(9 citation statements)
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“…The elasticity modulus of pure ferrite phases at bottom and top surface is E f = 178 GPa [36]; while that of martensite phases at core area is E m = 215 GPa [37]; The influence of Poisson's ratio on the deflection is much less than that of elasticity modulus [38]. Therefore, Poisson's ratio of the graded beams is assumed to be constant at 0.3.…”
Section: Methodsmentioning
confidence: 99%
“…The elasticity modulus of pure ferrite phases at bottom and top surface is E f = 178 GPa [36]; while that of martensite phases at core area is E m = 215 GPa [37]; The influence of Poisson's ratio on the deflection is much less than that of elasticity modulus [38]. Therefore, Poisson's ratio of the graded beams is assumed to be constant at 0.3.…”
Section: Methodsmentioning
confidence: 99%
“…This article assumes that material parameters change continuously along the width direction (y). The power-law (Hadji et al, 2015) is given by:where p(y) represents a typical material property such as elastic modulus E, mass density ρ, and Poisson’s ratio υ. pt and pb represent the material property values of the topmost and bottommost surfaces of the FG beam, respectively, and n is the non-negative power-law index.…”
Section: Physical Model and Methodsmentioning
confidence: 99%
“…Li formulated an analytical solution to analyze the static and dynamic behaviours of FGM Timoshenko and Euler-Bernoulli beams [25]. Higher order theories were investigated to introduce more complex characteristics such as shear deformation and warping, a sample of research papers [26][27][28][29][30][31][32][33][34][35][36][37][38] are quoted here which provide a good introduction on the subject.…”
Section: Literature Surveymentioning
confidence: 99%