2008
DOI: 10.1007/s10659-008-9175-z
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Weak Local Minimizers in Finite Elasticity

Abstract: This paper deals with necessary conditions and sufficient conditions for a weak local minimum of the energy of a hyperelastic body. We consider anisotropic bodies of arbitrary shape, subject to prescribed displacements on a given portion of the boundary. As an example, we consider the uniaxial stretching of a cylinder, in the two cases of compressible and incompressible material. In both cases we find that there is a continuous path across the natural state, made of local energy minimizers. For the Blatz-Ko co… Show more

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Cited by 17 publications
(38 citation statements)
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“…Equivalently, one can derive estimates on the energy that ensure that the second variation of E is strictly positive at the deformation u h λ and, consequently, that u h λ is both linearization stable and a strict weak relative minimizer. For a compressible cylindrical solid in tension this technique was used by Spector [27] and, more recently, by Del Piero and Rizzoni [7] and Fosdick, Foti, Fraddosio, and Piccioni [10] (see, also, Del Piero [6]) to obtain estimates upon the values of λ where bifurcations cannot occur. Additionally, in [7] and [10] similar estimates are derived for compression (λ ≤ 1); incompressible materials are also considered in [7].…”
mentioning
confidence: 99%
“…Equivalently, one can derive estimates on the energy that ensure that the second variation of E is strictly positive at the deformation u h λ and, consequently, that u h λ is both linearization stable and a strict weak relative minimizer. For a compressible cylindrical solid in tension this technique was used by Spector [27] and, more recently, by Del Piero and Rizzoni [7] and Fosdick, Foti, Fraddosio, and Piccioni [10] (see, also, Del Piero [6]) to obtain estimates upon the values of λ where bifurcations cannot occur. Additionally, in [7] and [10] similar estimates are derived for compression (λ ≤ 1); incompressible materials are also considered in [7].…”
mentioning
confidence: 99%
“…In Fig. 1 we compare our estimates to that recently proposed in [4] for incompressible bodies: we see that our estimate is better for thick cylinders, whereas for slender cylinders the two estimates practically coincide. However, the effectiveness of an estimate from below depends on its "distance" from the actual critical load.…”
Section: Bound From Below Of the Hadamard Functionalmentioning
confidence: 51%
“…Indeed, by comparing our estimate λ LB to the upper bound estimate reported in [4], it is possible to conclude that for slender bodies, where the instability is mainly due to geometrical effects in presence of relatively small deformations, λ LB accurately approximates the critical load. Conversely, for small slenderness, when the instability is strongly related to the non-linearity of the constitutive equation, our lower bound estimate, although more efficient of that in [4], does not represent a good approximation of the critical load. Thus, there remains an open problem to enhance lower bound estimates when stable large deformations are anticipated.…”
Section: Bound From Below Of the Hadamard Functionalmentioning
confidence: 56%
“…In (Del Piero, 1979;Del Piero and Rizzoni, 2008) it is proved that if w 3 is frame-indifferent, then b 3 0 can be decomposed into…”
Section: Three-dimensional Energy Of a Mismatch Strained Interphasementioning
confidence: 99%