2014
DOI: 10.1007/s00707-014-1142-0
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Bending and vibration analysis of generalized gradient elastic plates

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Cited by 22 publications
(5 citation statements)
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“…Yaghoubi et al [154] developed a continuum model for medium-thick nanobeams based on this theory, and derived the governing equations, initial conditions, and boundary conditions using the variational principle. A mechanical model of static buckling and vibration in nano-Kirchhoff and Mindlin plates has been developed by Xu et al [155] using the Mindlin velocity gradient theory. It was found that the natural frequency ratio decreased with increasing gradient parameter, and when the dimensionless gradient parameter is small, the fundamental frequency ratio is close to 1, indicating that the gradient parameter has no significant effect on large-size plates.…”
Section: Velocity Gradientmentioning
confidence: 99%
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“…Yaghoubi et al [154] developed a continuum model for medium-thick nanobeams based on this theory, and derived the governing equations, initial conditions, and boundary conditions using the variational principle. A mechanical model of static buckling and vibration in nano-Kirchhoff and Mindlin plates has been developed by Xu et al [155] using the Mindlin velocity gradient theory. It was found that the natural frequency ratio decreased with increasing gradient parameter, and when the dimensionless gradient parameter is small, the fundamental frequency ratio is close to 1, indicating that the gradient parameter has no significant effect on large-size plates.…”
Section: Velocity Gradientmentioning
confidence: 99%
“…Based on the gradient theory with higher-order inertia effects proposed by Polizzotto [153], Xu et al [155] developed a nano-Euler beam model, which gives closed solutions for the free vibration frequencies of the beam under the conditions of clamped, simply-supported and cantilever boundary conditions.…”
Section: Velocity Gradientmentioning
confidence: 99%
“…For instance, the deflection of gradient elastic Kirchhoff plates [28,29] and Kirchhoff-Love cylindrical shells [33,34] requires C 2 -continuity. The deflection and rotations of gradient elastic Mindlin plates [31,49] require C 1 -continuity. Moreover, gradient elastic Reddy plates [32] require both the C 1 -continuity of rotation and the C 2 -continuity of deflection.…”
Section: Introductionmentioning
confidence: 99%
“…The existing two-dimensional non-local models for thin elastic plates are usually based on the above-mentioned differential constitutive relations (e.g. [20][21][22][23][24][25][26][27][28]). In these models, threedimensional → two-dimensional reduction is carried out using ad-hoc assumptions neglecting the variation of non-local properties across the thickness.…”
Section: Introductionmentioning
confidence: 99%
“…The existing 2D nonlocal models for thin elastic plates are usually based on the above mentioned differential constitutive relations, e.g., see Lu et al (2007), Duan and Wang (2007), Aghababaei and Reddy (2009), Pradhan and Phadikar (2009), Malekzadeh et al (2011), Xu et al (2014), Thai et al (2014), Jung and Han (2014), and Mousavi et al (2017). In these models, 3D → 2D reduction is carried out using ad-hoc assumptions neglecting the variation of nonlocal properties across the thickness.…”
Section: Introductionmentioning
confidence: 99%