2020
DOI: 10.1002/zamm.202000046
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Variational formulation and differential quadrature finite element for freely vibrating strain gradient Kirchhoff plates

Abstract: In this paper, we apply the energy variational principle to arrive at the differential equation of motion and all appropriate boundary conditions for strain gradient Kirchhoff micro‐plates. The resulting sixth‐order boundary value problem of free vibration is solved by a thirty‐six‐DOF four‐node differential quadrature plate finite element. The C2‐continuity condition of the deflection is guaranteed by devising a sixth‐order differential quadrature‐ based geometric mapping scheme that can transform the displac… Show more

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Cited by 10 publications
(7 citation statements)
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References 88 publications
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“…Rewriting the stress‐strain relation for the porous core and simplifying it yields [33]: σrrσθθσrzσθzσrθcbadbreak=A1(z)1emB1false(zfalse)1em01em01em0B1(z)1emA1false(zfalse)1em01em01em001em01emG(z)1em01em001em01em01emG(z)1em001em01em01em01emG(z)c{}εrrεθθγrzγθzγrθ$$\begin{equation}{\left\{ { \def\eqcellsep{&}\begin{array}{@{}*{1}{c}@{}} {{\sigma }_{rr}}\\[6pt] {{\sigma }_{\theta \theta }}\\[6pt] {{\sigma }_{rz}}\\[6pt] {{\sigma }_{\theta z}}\\[6pt] {{\sigma }_{r\theta }} \end{array} } \right\}}^c = {\left[ { \def\eqcellsep{&}\begin{array}{@{}*{5}{c}@{}} {{A}_1(z)}& \quad {{B}_1(z)}& \quad 0& \quad 0& \quad 0\\[6pt] {{B}_1(z)}& \quad {{A}_1(z)}& \quad 0& \quad 0& \quad 0\\[6pt] 0& \quad 0& \quad {G(z)}& \quad 0& \quad 0\\[6pt] 0& \quad 0& \quad 0& \quad {G(z)}& \quad 0\\[6pt] 0& \quad 0& \quad 0& \quad 0& \quad {G(z)} \end{array} } \right]}^c\left\{ { \def\eqcellsep{&}\begin{array}{@{}*{1}{c}@{}} {{\varepsilon }_{rr}}\\[6pt] {{\varepsilon }_{\theta \theta }}\\[6pt] {{\gamma...…”
Section: Mathematical Formulationsmentioning
confidence: 99%
“…Rewriting the stress‐strain relation for the porous core and simplifying it yields [33]: σrrσθθσrzσθzσrθcbadbreak=A1(z)1emB1false(zfalse)1em01em01em0B1(z)1emA1false(zfalse)1em01em01em001em01emG(z)1em01em001em01em01emG(z)1em001em01em01em01emG(z)c{}εrrεθθγrzγθzγrθ$$\begin{equation}{\left\{ { \def\eqcellsep{&}\begin{array}{@{}*{1}{c}@{}} {{\sigma }_{rr}}\\[6pt] {{\sigma }_{\theta \theta }}\\[6pt] {{\sigma }_{rz}}\\[6pt] {{\sigma }_{\theta z}}\\[6pt] {{\sigma }_{r\theta }} \end{array} } \right\}}^c = {\left[ { \def\eqcellsep{&}\begin{array}{@{}*{5}{c}@{}} {{A}_1(z)}& \quad {{B}_1(z)}& \quad 0& \quad 0& \quad 0\\[6pt] {{B}_1(z)}& \quad {{A}_1(z)}& \quad 0& \quad 0& \quad 0\\[6pt] 0& \quad 0& \quad {G(z)}& \quad 0& \quad 0\\[6pt] 0& \quad 0& \quad 0& \quad {G(z)}& \quad 0\\[6pt] 0& \quad 0& \quad 0& \quad 0& \quad {G(z)} \end{array} } \right]}^c\left\{ { \def\eqcellsep{&}\begin{array}{@{}*{1}{c}@{}} {{\varepsilon }_{rr}}\\[6pt] {{\varepsilon }_{\theta \theta }}\\[6pt] {{\gamma...…”
Section: Mathematical Formulationsmentioning
confidence: 99%
“…The displacement-based equations of motion and boundary conditions of gradient elastic thick microplates can be obtained using the variational formulations provided in [69].…”
Section: Governing Equations Of Gradient Elastic Thick Microplatesmentioning
confidence: 99%
“…Zhang et al [62] utilized the advantages of the DQM and FEM for the first time to construct weak-form DQFEs related to isotropic MSGT-based Euler-Bernoulli and Timoshenko beam models, respectively. Soon afterward, they proposed a series of weak-form DQFEs for size-dependent Reddy beams [63,64], Mindlin plates [65,66], and Kirchhoff plates [67][68][69] and showed the efficacy of their developed DQFEM in comparison with the standard FEM.…”
Section: Introductionmentioning
confidence: 99%
“…They studied the CNTs volume fraction, width-thickness ratio, CNTs distributions and boundary conditions on the natural frequencies of the composite plate. Zhang et al [12] applied the energy variational principle to arrive at the differential equation of motion and all appropriate boundary conditions for strain gradient Kirchhoff micro-plates. Civalek et al [13] investigated of the influences of volume fraction, length to width ratio, aspect ratio, layer number, and boundary conditions on the frequency and flexural loading of carbon nanotube reinforced composite plates.…”
Section: Introductionmentioning
confidence: 99%
“…Zhang et al. [12] applied the energy variational principle to arrive at the differential equation of motion and all appropriate boundary conditions for strain gradient Kirchhoff micro‐plates. Civalek et al.…”
Section: Introductionmentioning
confidence: 99%