2018
DOI: 10.1007/s00707-018-2180-9
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A research into bi-Helmholtz type of nonlocal elasticity and a direct approach to Eringen’s nonlocal integral model in a finite body

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Cited by 29 publications
(3 citation statements)
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“…It is noted that, in the current study, the constitutive law for the nonlocal theory will be assumed as a two‐phase material (local and nonlocal phases) [6] to resolve the issue of the ill‐posedness of the problem [55–57]. In other words, the nonlocal constitutive equation will be considered as follows: tve()boldx,tbadbreak=ζ1bold-italicσve()boldx,tgoodbreak+ζ2Vα()||xboldx,τbold-italicσve()x,tdV()boldx,boldxV\begin{equation}{{\bm{t}}^{ve}} \left( {{{\bf x}},t} \right) = {\zeta _1}\ {{\bm{\sigma }}^{ve}}\left( {{{\bf x}},t} \right) + {\zeta _2}\int_V \alpha \left( {\left| {{{\bf x^{\prime}}} - {{\bf x}}} \right|,\ \tau } \right){{\bm{\sigma }}^{ve}}\left( {{{\bf x^{\prime}}},t} \right)dV\left( {{{\bf x^{\prime}}}} \right),\quad \forall {{\bf x}} \in V\end{equation}…”
Section: Constitutive Equationsmentioning
confidence: 99%
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“…It is noted that, in the current study, the constitutive law for the nonlocal theory will be assumed as a two‐phase material (local and nonlocal phases) [6] to resolve the issue of the ill‐posedness of the problem [55–57]. In other words, the nonlocal constitutive equation will be considered as follows: tve()boldx,tbadbreak=ζ1bold-italicσve()boldx,tgoodbreak+ζ2Vα()||xboldx,τbold-italicσve()x,tdV()boldx,boldxV\begin{equation}{{\bm{t}}^{ve}} \left( {{{\bf x}},t} \right) = {\zeta _1}\ {{\bm{\sigma }}^{ve}}\left( {{{\bf x}},t} \right) + {\zeta _2}\int_V \alpha \left( {\left| {{{\bf x^{\prime}}} - {{\bf x}}} \right|,\ \tau } \right){{\bm{\sigma }}^{ve}}\left( {{{\bf x^{\prime}}},t} \right)dV\left( {{{\bf x^{\prime}}}} \right),\quad \forall {{\bf x}} \in V\end{equation}…”
Section: Constitutive Equationsmentioning
confidence: 99%
“…It is noted that, in the current study, the constitutive law for the nonlocal theory will be assumed as a two-phase material (local and nonlocal phases) [6] to resolve the issue of the ill-posedness of the problem [55][56][57]. In other words, the nonlocal constitutive equation will be considered as follows: In which, 𝜁 1 and 𝜁 2 are the positive constants referring to, respectively, the local and nonlocal fractions of the so-called two-phase material.…”
Section: Constitutive Equationsmentioning
confidence: 99%
“…Fakher et al (2018) studied the vibration of a mass nanosensor, consisting of a cantilevered carbon nanotube with a size-dependent nonlocal elastic foundation, by the finite element model of integral nonlocal elasticity. Also, Koutsoumaris and Eptaimeros (2018) explored the strain of the beams under bending via bi-Helmholtz operators and its kernel function in the integral nonlocal elasticity.…”
Section: Introductionmentioning
confidence: 99%