2015
DOI: 10.1016/j.compstruct.2015.02.067
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An anisotropic in-plane and out-of-plane elasto-plastic continuum model for paperboard

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Cited by 62 publications
(64 citation statements)
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“…The potential governing the relationship between the stresses and the kinematical quantities is given by the free energy 0 D 0 ip C 0 op . A slightly different format of 0 compared with Borgqvist et al 7 is proposed, such that the Poisson's effect between the in-plane and out-of-plane directions initially is zero. This modification implies a zero initial Poisson's effect between the in-plane and out-of-plane directions, which provides a better experimental agreement.…”
Section: Materials Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…The potential governing the relationship between the stresses and the kinematical quantities is given by the free energy 0 D 0 ip C 0 op . A slightly different format of 0 compared with Borgqvist et al 7 is proposed, such that the Poisson's effect between the in-plane and out-of-plane directions initially is zero. This modification implies a zero initial Poisson's effect between the in-plane and out-of-plane directions, which provides a better experimental agreement.…”
Section: Materials Modelmentioning
confidence: 99%
“…The model has been implemented in the commercial software ABAQUS, 25 via the subroutine option UMAT. Details regarding the numerical implementation of the model is provided by Borgqvist et al 7 In the numerical model, the paperboard is homogeneous and therefore possess constant material parameters through the width and thickness. The geometry of the SCT is shown in Figure 8.…”
Section: Numerical Investigation Of Short-span Compression Testmentioning
confidence: 99%
“…The out‐of‐plane material behaviour in the thickness direction, ZD, is described by a director vector bold-italicn0false(3false), which is defined to be orthogonal to MD and CD, ie, bold-italicn0false(3false)=bold-italicv0false(1false)×bold-italicv0false(2false). This choice for the out‐of‐plane director vector follows from the assumption that paperboard can be considered as an idealized layered structure; details regarding this assumption are presented in Borgqvist et al The in‐plane director vectors are assumed to follow the elastic part of the deformation gradient, while the out‐of‐plane director vector is constructed to be orthogonal to the updated in‐plane directors, ie, vfalse(1false)=Febold-italicv0false(1false),1em1emvfalse(2false)=Febold-italicv0false(2false)1emand1emnfalse(3false)=JeFeTbold-italicn0false(3false), with J e being the determinant of the elastic deformation gradient. The Helmholtz free energy is assumed to be a function of the elastic Finger tensor b e = F e ( F e ) T and the structural tensors m (1) = v (1) ⊗ v (1) , m (2) = v (2) ⊗ v (2) , m (3) = n (3) ⊗ n (3) using the following invariants: rightleftI11=bold-italicm(1):I,I12=bold-italicm(2):I,I13=1Jebold-italicm(3):bold-italicbebold-italicbe,rightrightleftI23=…”
Section: Materials Model For Paperboardmentioning
confidence: 99%
“…The paperboard model has previously been used to study a number of industrial applications. In Borgqvist et al, a numerical study of the creasing process was considered using a simplified line‐creasing operation as well as a more realistic, 3D rotational setup. Furthermore, it was shown in Borgqvist et al that the paperboard model was able to capture the formation of wrinkles for both the line‐folding process of uncreased paperboard and for the short‐span compression test.…”
Section: Introductionmentioning
confidence: 99%
“…For paperboard and paperboard products, finite element simulations have previously successfully been used to study creasing and folding, brim forming, point loading of packages, delamination during printing, and 3D forming . Test methods such as the short compression test have been modelled.…”
Section: Introductionmentioning
confidence: 99%