Abstract:The mechanical performance of semicrystalline polymers is strongly dependent on their underlying microstructure, consisting of crystallographic lamellae and amorphous layers. In line with that, semicrystalline polymers have previously been modeled as two and three‐phase composites, consisting of a crystalline and an amorphous phase and, in case of the three‐phase composite, a rigid‐amorphous phase between the other two, having a somewhat ordered structure and a constant thickness. In this work, the ability of … Show more
“…As obtaining fully amorphous PE samples at relevant temperatures is nearly impossible, the reported elastic values are either based on theoretical arguments or based on extrapolation to zero crystallinity of measurements made at nonzero crystallinities. Using the theoretical relationship for the plateau shear modulus and an amorphous bulk modulus of , Bédoui et al and Sedighiamiri et al estimated the amorphous Young's modulus and Poisson's ratio to be E am = 4.5 MPa and υ am = 0.49975, respectively. In eq , ρ is the amorphous phase density, T is the absolute temperature, R is the ideal gas constant, and M e is the molecular mass between entanglements.…”
Semi-crystalline polyethylene is composed of three domains: crystalline lamellae, the compliant amorphous phase, and the so-called "interphase" layer separating them. Among these three constituents, little is known about the mechanical properties of the interphase layer. This lack of knowledge is chiefly due to its mechanical instability as well as its nanometric thickness impeding any property measuring experiments. In this study, the Monte Carlo molecular simulation results for the interlamellar domain (i.e. amorphous+ interphases), reported in (in 't Veld et al. 2006) are employed. The amorphous elastic properties are adopted from the literature and then two distinct micromechanical homogenization approaches are utilized to dissociate the interphase stiffness from that of the interlamellar region. The results of the two approaches match perfectly, which validates the implemented dissociation methodology. Moreover, a hybrid numerical technique is proposed for one of the approaches when the recursive method poses numerical divergence problems. Interestingly, it is found that the dissociated interphase stiffness lacks the common feature of positive definiteness, which is attributed to its nature as a transitional domain between two coexisting phases. The sensitivity analyses carried out reveal that this property is insensitive to the non-orthotropic components of the interlamellar stiffness as well as the uncertainties existing in the interlamellar and amorphous stiffnesses. Finally, using the dissociated interphase stiffness, its effective Young's modulus is calculated. The evaluated Young's modulus compares well with the effective interlamellar Young's modulus for highly crystalline polyethylene, reported in an experimental study. This satisfactory agreement along with the identical results produced by the two micromechanical approaches confirms the validity of the new information about the interphase elastic properties in addition to making the proposed dissociation methodology quite reliable to be applied to similar problems.
“…As obtaining fully amorphous PE samples at relevant temperatures is nearly impossible, the reported elastic values are either based on theoretical arguments or based on extrapolation to zero crystallinity of measurements made at nonzero crystallinities. Using the theoretical relationship for the plateau shear modulus and an amorphous bulk modulus of , Bédoui et al and Sedighiamiri et al estimated the amorphous Young's modulus and Poisson's ratio to be E am = 4.5 MPa and υ am = 0.49975, respectively. In eq , ρ is the amorphous phase density, T is the absolute temperature, R is the ideal gas constant, and M e is the molecular mass between entanglements.…”
Semi-crystalline polyethylene is composed of three domains: crystalline lamellae, the compliant amorphous phase, and the so-called "interphase" layer separating them. Among these three constituents, little is known about the mechanical properties of the interphase layer. This lack of knowledge is chiefly due to its mechanical instability as well as its nanometric thickness impeding any property measuring experiments. In this study, the Monte Carlo molecular simulation results for the interlamellar domain (i.e. amorphous+ interphases), reported in (in 't Veld et al. 2006) are employed. The amorphous elastic properties are adopted from the literature and then two distinct micromechanical homogenization approaches are utilized to dissociate the interphase stiffness from that of the interlamellar region. The results of the two approaches match perfectly, which validates the implemented dissociation methodology. Moreover, a hybrid numerical technique is proposed for one of the approaches when the recursive method poses numerical divergence problems. Interestingly, it is found that the dissociated interphase stiffness lacks the common feature of positive definiteness, which is attributed to its nature as a transitional domain between two coexisting phases. The sensitivity analyses carried out reveal that this property is insensitive to the non-orthotropic components of the interlamellar stiffness as well as the uncertainties existing in the interlamellar and amorphous stiffnesses. Finally, using the dissociated interphase stiffness, its effective Young's modulus is calculated. The evaluated Young's modulus compares well with the effective interlamellar Young's modulus for highly crystalline polyethylene, reported in an experimental study. This satisfactory agreement along with the identical results produced by the two micromechanical approaches confirms the validity of the new information about the interphase elastic properties in addition to making the proposed dissociation methodology quite reliable to be applied to similar problems.
“…Studies with a certain focus on processing parameter have been extended to morphology development and modification variation like β‐phase formation in molding, but also to investigations concerning shrinkage and dimensional stability, with holding pressure found as a dominant factor for the latter. A final target is the prediction of mechanic, for which mechanical concepts regarding the crystal structure and factors like lamellar thickness and the distribution between crystalline phase, rigid and mobile amorphous phase are required . Composite inclusion models have already been demonstrated to work for both HDPE and PP, but deformation involving high strains and strain rates up to the point of failure are still out of reach except for highly idealized cases.…”
Section: Processing‐based Modificationsmentioning
confidence: 99%
“…A logical next step should be to relate crystalline morphology to mechanics with realistic structural models. This implies progressing from continuum approaches to a more realistic image of the structure of semi‐crystalline solids while maintaining practically affordable calculation times . Multi‐phase systems either with particulate inclusions (like elastomer particles) or with more regular structure from co‐processing or phase separation will probably continue to present problems for coming years, even at least numerical work has been done already …”
Section: Introductionmentioning
confidence: 99%
“…This implies progressing from continuum approaches to a more realistic image of the structure of semi-crystalline solids while maintaining practically affordable calculation times. [22] Multi-phase systems either with particulate inclusions (like elastomer particles) or with more regular structure from coprocessing or phase separation will probably continue to present problems for coming years, even at least numerical work has been done already. [23,24] The present review will present three approaches to control crystal structure and resulting along the product design path: By modifying the polymer, by additivation and blending, and finally through the processing step.…”
More than 50% of the thermoplastic polymers applied globally are semi‐crystalline, making crystallization part of the material and component design process for these materials. The mechanical and optical performance, but also the long‐term stability of the final articles and applications will depend upon three major groups of influence factors: Polymer structure and monomer composition, additive addition (especially nucleation) and blending with secondary components, and processing parameters. In the present review, we try to establish a connection between these three areas, the resulting combination of crystallinity and morphology, and the final application properties. Examples are drawn from the two major polyolefins, polyethylene and polypropylene, technical polymers like polyamide and polyester, but also polymers from renewable sources like poly(lactic acid).
“…However, structural properties are treated implicitly in this approach. Another group of papers [108][109][110][111][112][113][114][115][116][117][118][119][120][121] uses conception of two-phase continuum containing rigid and soft components (crystalline and amorphous phases) with essentially different mechanical properties. The main distinction of semicrystalline polymers from the particulate composites is their peculiar self-organized structure containing stacks of crystal lamellae alternating with thin amorphous layers.…”
Section: Modeling Of Small-strain Deformation Behavior Of Semicrystalmentioning
The review focuses on the current studies of the deformation response and accompanying structural transformations of thermoplastic semicrystalline polymers subjected to uniaxial tension prior to the yield point. The mechanisms of strain-induced cavitation of amorphous layers and damages of crystalline lamellae are analyzed in line with novel results on the deformation behavior of solid polymers at temperatures exceeding the glass transition point. The coupling of viscoelastic and plastic deformation mechanisms with the small-strain structural transformations is critically discussed on the basis of the advanced theoretical modeling of mechanical properties of semicrystalline polymers.
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