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Spontaneous polarization, n-type half-metallicity, low lattice thermal conductivity, and high structure stabilities in F@O-doped PbTiO<sub>3</sub>. [PDF]
RSC AdvHaider S, Felemban BF, Ali HT, Nazir S.
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Advanced analysis of nonlinear stability of two horizontal interfaces separating three-stratified non-Newtonian liquids. [PDF]
Sci RepMoatimid GM, Mohamed YM.
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Radial oscillation of an encapsulated bubble near a planar rigid wall under dual-frequency acoustic excitation in viscoelastic fluids. [PDF]
Ultrason SonochemZang YC, Chen DC, Zhu XF, Wu DJ, Lin WJ.
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Mechanical, structural, electronic, magnetic, and thermomagnetic properties of the full-Heusler Fe2MnAs1-xSix alloy using DFT and Monte Carlo simulation. [PDF]
Sci RepGharaibeh M +3 more
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NULL LAGRANGIANS IN LINEAR ELASTICITY
Mathematical Models and Methods in Applied Sciences, 1995The concept of null Lagrangian is exploited in the context of linear elasticity. In particular, it is shown that the stored energy functional can always be split into a null Lagrangian and a remainder; the null Lagrangian vanishes if and only if the elasticity tensor obeys the Cauchy relations, and is therefore determined by only 15 independent moduli
LANCIA, Maria Rosaria +2 more
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Linearized Elasticity as Γ-Limit of Finite Elasticity
Set-Valued Analysis, 2002Linearized elastic energies are derived from rescaled nonlinear energies by means of \(\Gamma\)-convergence. For Dirichlet and mixed boundary value problems in a Lipschitz domain \(\Omega\), the convergence of minimizers takes place in the weak topology of \(H^1(\Omega,\mathbb{R}^n)\) and in the strong topology of \(W^{1,q}(\Omega,\mathbb{R}^n)\) for \(
Dal Maso, Gianni, NEGRI M., PERCIVALE D.
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Journal of Applied Mechanics, 1968
Abstract The linear dipolar field equations for an initially flat surface are presented and applied to an elastic isotropic surface. The equations separate into extensional and bending equations, and the extensional equations are discussed in detail.
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Abstract The linear dipolar field equations for an initially flat surface are presented and applied to an elastic isotropic surface. The equations separate into extensional and bending equations, and the extensional equations are discussed in detail.
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