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Strain localization in polyurethane foams. Experiments and theoretical model.
Giampiero Pampolini, Gianpietro del Piero
To cite this version:
Giampiero Pampolini, Gianpietro del Piero. Strain localization in polyurethane foams. Experiments
and theoretical model.. 11th EUROMECH-MECAMAT Conference, Mar 2008, Torino, Italy. pp.29-
38. �hal-00462212�
(will be inserted by the editor)
Strain localization in polyurethane foams. Experiments and theoretical model.
Giampiero Pampolini · Gianpietro Del Piero
Received: date / Accepted: date
Abstract Strain localization has been observed in polyurethane foams subjected to confined compression up to 70% of deformation. This phenomenon is described by a one-dimensional model, in which the foam is represented as a chain of non-linear elastic springs with non-convex strain energy density, and localization is attributed to progressive phase transition.
Keywords polyurethane foams · strain localization · non-convex strain energy, solid-solid phase transition.
1 Introduction
In the uniaxial compression of foam polymers, and of cellular materials in general, three regimes can be identified. The first regime is an almost linear response, the sec- ond is a stress plateau with large displacements occurring at almost constant load, and the last is a branch characterized by large stress increase under relatively moder- ate deformations. In the literature, two main approaches for modeling the mechan- ical response of foam polymers are used: a microstructural approach, reproducing directly the microstructure with a complex structure of beams, and a macroscopic approach, based on a full three-dimensional representation of the material as a con- tinuum. There has been a wide spread of models based on the first approach (e.g., [Gent and Thomas (1963)], [Gibson and Ashby (1997)], [Warren and Kraynik (1997)], [Gong et al. (2005)]). In particular, Gong et al. studied the response curves of open- cell foams, and [Gong and Kyriakides (2005)] proposed a model with a periodic struc- Giampiero Pampolini
Laboratoire de M´ ecanique et d’Acoustique, CNRS, 31 chemin Joseph Aiguier, 13402 Marseille, France.
Universit` a di Ferrara, Via Saragat 1, 44100 Ferrara, Italy.
E-mail: pampolini@lma.cnrs-mrs.fr; giampiero.pampolini@unife.it
Gianpietro Del Piero
Universit` a di Ferrara, Via Saragat 1, 44100 Ferrara, Italy.
E-mail: dlpgpt@unife.it
2
ture given by a 14-sided polyhedron, called the Kelvin cell. The ligaments are mod- eled as shear-deformable extensional beams, and the basic material is assumed to be linearly elastic. In this approach, the numerical simulation is demanding from the computational point of view, due to the complexity of the assumed microstructure and to the difficulty of modeling the contact between beams in the post-buckling regime, see [Bardenhagen et al. (2005)]. In the continuum approach, the material is considered as homogeneous and hyperelastic, and subject to non-homogeneous defor- mations. Indeed, there is experimental evidence of strain localization, see for exam- ple [Lakes et al. (1993)], [Wang and Cuitinho (2002)]. In particular, strain localization along bands orthogonal to the loading direction was observed by Wang and Cuitio, and confirmed by experiments performed by the present authors on polyurethane foam specimens, subjected to axial compression up to 70%. The same three stages in the evolution of deformation have been observed by [Bastawros et al. (2000)] and [Bart-Smith et al. (1998)] in both open- and closed-cell aluminium alloy foams. In these cases, the deformation localizes in narrow bands, whose width is of the order of a cell diameter. These results support the interpretation, suggested in previous works [Wang and Cuitinho (2002)], [Gioia et al. (2001)], of the non-homogeneous deforma- tion as a phase transition. Here we present a model in which the foam is represented as a chain of non-linear elastic springs with non-convex strain energy, and the local- ization is interpreted as a progressive phase change. The first part of the paper deals with the test procedure and the experimental results, and the second contains an out- line of the theoretical model. A complete description of the model can be found in [Pampolini and Del Piero (2008)].
2 EXPERIMENTAL TESTS
For the compression tests we used the load frame INSTRON 4467 located at the Lab- oratorio di Materiali Polimerici of the University of Ferrara, with a load cell of 500 N.
The tests were made on commercial polyurethane foams in confined compression. For confinement we used a polystyrene box, clamped to the load frame. The polystyrene box is more rigid than the tested material and, being transparent, allowed us to control optically the evolution of the deformation. At the upper basis, the specimen was in con- tact with a steel plate fixed to the moving crosshead. Five specimens of dimensions 100
× 100 × 50 mm were tested. The crosshead speed was chosen to be 1 mm/min, which we believe small enough to neglect all rate-dependent effects. The test was stopped at a relative elongation of 70%. As we will see later, this value is sufficiently large to include the significant portions of the response curves.
The stress-strain curves shown in Figure 1 reveal the characteristic behavior of polyurethane foams, and of cellular materials in general. From the figure, we notice that the plateau begins at a relative elongation of about 10% and ends at about 63%, and that the stress is close to 6,5 kPa. The slope of the second branch is approximatively 25 kPa. These values are close to those obtained by [Gioia et al. (2001)].
During the tests, the deformation was initially homogeneous (Figure 2a). Then a
severe deformation occurred at the upper layer of the specimen (Figure 2b), and prop-
agated to the underlying layers (Figures 2c, 2d). When all layers had reached the same
deformation the specimen began again to deform homogeneously (Figure 2e). That the
large deformation regime starts at one of the ends of the specimen can be attributed
to a local boundary effect due to contact between steel plate and specimen. The same
Deformation
S tr es s (k P a)
Fig. 1 Experimental curves of polyurethane foams in confined compression tests.
evolution mechanism was observed by [Wang and Cuitinho (2002)] in polyurethane low-density foams, and by [Bastawros et al. (2000)] and [Bart-Smith et al. (1998)] in aluminium alloy foams. In Wang and Cuitio’s experiments, localization does not initiate at the upper part of the specimen as it does in our tests.
(a) (b) (c)
(d) (e)