Initiation of cavitation upon drawing of pre-oriented polypropylene film: In situ SAXS and WAXD studies
Graphical abstract
Introduction
Semi-crystalline polymers consisting of crystalline lamellae and amorphous phase generally display a complex structural hierarchy from meso-scale to macroscopic level [1], [2]. Generally, plastic deformation of semi-crystalline polymers involves crystal shear and cavitation. It seems that these processes can be activated concomitantly or competitively under tensile loads depending on material structures and experimental conditions [1], [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13], [14], [15], [16], [17].
Historically, cavitation during the tensile drawing of semi-crystalline polymers has been treated as a marginal effect, i.e. accompanying plastic deformation of polymer crystals. Butler et al. [3], [4], [5] studied plastic deformation of tensile drawn high density polyethylene and found the cavitation in polyethylene was formed at yield point when martensitic transformation and chain slips begins. Afterwards, Galeski et al. [7] proposed a competition mechanism between the cavitation in inter-lamellar amorphous layers and the crystal shear. This competition relation has been further confirmed in a recent paper [8] via comparing the onset strain of local crystal shear and cavitation during the tensile drawing of polyethylene by in-situ wide angle X-ray diffraction (WAXD) and small angle X-ray scattering (SAXS) experiments. Alternative understanding has been proposed by Men et al. [18], [19] where investigations on polybutene-1 revealed that cavities initiated first in the crystalline phase as a result of breakage of crystalline skeleton during tensile deformation.
Currently, cavitation in semi-crystalline polymers has been created for many functional applications. Polypropylene (PP) is a semi-crystalline polymer commonly used to produce porous membranes for battery separators [20], [21], [22]. The polypropylene resins are melt-extruded into a uniaxial oriented film which has a crystalline row structure with their long axis perpendicular to the machine direction (MD). Then the film is stretched in MD to create the pore structure at low temperature. So that understanding the ‘open’ mechanism for pre-oriented PP film is important to control the properties of the final products of micro-membranes.
In recent studies, Lin et al. [23] and Lei et al. [24] investigated the structural and processing parameters of pre-oriented film for the micro-pore formation. They found that the orientation degree and the thickness of crystalline and amorphous layers are crucial parameters for the formation of micro-pores. On the other hand, daughter lamellae were found to play important role on the formation and stabilization of pores upon drawing of pre-oriented polypropylene films. Chen and Lei et al. [25] reported that daughter lamellae were destroyed around yield point before parent crystals and then transferred to the connecting bridge between parent lamellae which can stabilize the cavities during deformation. Besides, annealing of the casted films benefits the formation of pores [26], [27], [28], [29]. It was interpreted as that the increase of the crystalline lamellar thickness promotes a better separation of crystalline lamellae. So that, it seems the thickness of the crystalline lamellae is crucial to the pore formation. However, little attention has been paid to the underlying physical mechanism and also the relationship between cavitation and crystal shear upon drawing of pre-oriented polypropylene films.
The initiation of cavitation has been investigated in this work in order to reveal the mechanism of pore formation in pre-oriented PP films. In-situ SAXS was performed to probe the variation of cavities upon tensile drawing. This technique has been largely used to study the strain induced cavitation in semi-crystalline polymers owing to its ability of capturing the very first events of cavitation [6], [19], [30]. It also allows correlating microscopic structure variation to the macroscopic stress and strain. The onset of crystal shear has been studied as well via in-situ WAXD. In-situ WAXD provides the variation of the crystalline structure upon drawing [8], [31]. The initiation of crystal shear and cavitation upon drawing of the pre-oriented PP films has been compared to disclose the relationship between them.
Section snippets
Materials and sample preparation
Three isotactic polypropylenes (PPA, PPB and PPC) with different molecular weight were offered by Lanzhou Petrochemical Company (China). Molecular weight information has been listed in Table 1.
The PP pellets were extruded using a single-screw extruder (Haake Polylab System) with a slit die. The temperature from the hopper to the die was 160, 190, 190 and 190 °C, respectively. The extrusion rate was set at 0.6 rpm. The extrudate was preliminarily elongated by three cooling rolls (diameter
Initiation of cavitation
Fig. 2 shows stress-strain curve of PPC-cast stretched in machine direction (MD). The insets give the corresponding SAXS patterns and optical images upon stretching. Clearly, strain hardening appeared after yielding without necking and softening. This is the so-called hard elastic behavior which has been observed in highly oriented semi-crystalline polymers stretched in MD [28]. Similar stress strain curves have been observed for other samples. The whitening caused by nano-sized cavitation
Discussion
In order to investigate the relationship between cavitation and crystal shear, εcav and εcs have been compared. Fig. 6 shows the critical strain for the initiation of cavitation εcav and crystal shear εcs as a function of crystalline thickness, Lc. Clearly, εcs is smaller than εcav indicating that the crystal shear occurred before the cavitation. So that the deformation of pre-oriented PP film can be summarized as: Elastic deformation occurs at the beginning of stretching followed by the
Conclusion
The initiation of cavitation during the drawing of pre-oriented polypropylene films has been investigated via in-situ SAXS and WAXD techniques. The macroscopic strains for the initiation of cavitation εcav and crystal shear εcs have been estimated for each film. Comparison between εcs and εcav confirms that crystal shear appears before cavitation upon drawing in machine direction. The initial size of cavities along machine direction is larger than crystalline lamellar long period while the size
Acknowledgements
This work was support by National Natural Science Foundation of China (21604088, 51525305, 51503134 and 51421061), China Postdoctoral Science Foundation (Grant No.2015LH0050) and International PostDoc Initiative project of State Key Laboratory of Polymer Physics and Chemistry (IPI SKLPPC) (Grant No: IPI2015). We thank Dr. Guang Mo and Prof. Zhonghua Wu for their helps on WAXD experiments at BSRF and Dr. Jingyou Lin and Pin Zhou for their help on SAXS experiments at SSRF (Z15sr0043).
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2023, PolymerCitation Excerpt :It is reported that cavitation can be controlled by intrinsic structures and tensile conditions. The crystalline structures, including crystalline morphology [17,18], crystalline orientation [19], crystallization condition [20], and modified amorphous region [15,21–23], significantly affect the cavitation behavior. Besides, the tensile temperature, which is related to the activation of molecular mobility, is an important condition for cavitation [20,24,25].