2018
DOI: 10.1016/j.compstruct.2017.10.083
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Flexoelectric effect on the bending and vibration responses of functionally graded piezoelectric nanobeams based on general modified strain gradient theory

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Cited by 75 publications
(30 citation statements)
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“…The boundary condition in Equation 21indicates that nonlocal and flexoelectric effects act as a concentrated bending moment at the free end, which would change the shape of the deflection curve, especially near the free end. Hence, Figure 3 is presented to investigate the normalized deflection The boundary condition in Equation (21) indicates that nonlocal and flexoelectric effects act as a concentrated bending moment at the free end, which would change the shape of the deflection curve, especially near the free end. Hence, Figure 3 is presented to investigate the normalized deflection w(L)/w 0 (L) at the free end of sensors versus the normalized thickness h/h 0 for the different nonlocal parameters, in which h 0 = 12µ 2 13 / c 11 κ 33 + e 2 311 denotes an intrinsic thickness for the maximum induced electric potential of flexoelectric beams [15].…”
Section: Subjected To Uniformly Distributed Loads and A Concentrated mentioning
confidence: 99%
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“…The boundary condition in Equation 21indicates that nonlocal and flexoelectric effects act as a concentrated bending moment at the free end, which would change the shape of the deflection curve, especially near the free end. Hence, Figure 3 is presented to investigate the normalized deflection The boundary condition in Equation (21) indicates that nonlocal and flexoelectric effects act as a concentrated bending moment at the free end, which would change the shape of the deflection curve, especially near the free end. Hence, Figure 3 is presented to investigate the normalized deflection w(L)/w 0 (L) at the free end of sensors versus the normalized thickness h/h 0 for the different nonlocal parameters, in which h 0 = 12µ 2 13 / c 11 κ 33 + e 2 311 denotes an intrinsic thickness for the maximum induced electric potential of flexoelectric beams [15].…”
Section: Subjected To Uniformly Distributed Loads and A Concentrated mentioning
confidence: 99%
“…When the uniformly distributed load 0 has been considered, the expression of d 2 ( 1 )/d 1 2 = 0 should be satisfied in Equation (21). Here, a concentrated force at the free end and transverse From Equation 23, it can be clearly found that neglecting the nonlocal effect causes the induced electric potential to disappear as /( 0 ) = −1/3.…”
Section: Subjected To Sinusoidal Distributed Loads and A Concentratedmentioning
confidence: 99%
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“…Therefore, multiscale modeling of microstructures [27][28][29] and higher-order continuum elasticity theories including the non-local [30][31][32], couple stress [33][34][35] and strain gradient theories [36][37][38][39], which contain additional material length scale parameters for capturing the effect of size in small-scale structures, have been proposed. Many studies have been conducted on the basis of the SGT and non-local Eringen's theory to examine the size-dependent response of micro-and nanostructures with the consideration of surface and flexoelectric effects [40][41][42][43][44][45][46][47][48][49]. Lazopoulos and Lazopoulos [50] proposed another form of strain energy density function with surface energy to develop a new microscale Bernoulli-Euler beam model.…”
Section: Introductionmentioning
confidence: 99%