K. Okada1, Y. Tanaka2, H. Masunaga3, and M. Hikosaka1
1Graduate school of integrated arts and sciences, Hiroshima University, Japan.
2Teijin Ltd., Japan.
3Japan synchrotron radiation research institute (JASRI), SPring-8, Japan.
We crystallized the supercooled melt of polyesters by the melt-elongation. We used three kinds of polyesters, such as poly(ethylene terephthalate); PET, poly(ethylene-2,6-naphthalene dicarboxylate); PEN and poly(butylene terephthalate); PBT. We found that the novel three-dimensional (3D) morphology of “nano-oriented crystals (NOCs)” was formed, while in the case of isotactic polypropylene, one-dimensional morphology of NOCs was formed [1,2]. We observed the structure and morphology of NOCs by means of polarizing optical microscope, small/wide angle X-ray scattering. The nano crystals of 10 nm in order showed single crystal like monoclinic arrangement. The molecular chains were mainly oriented along the elongational direction. We clarified the mechanism of formation of 3D-NOCs of polyesters and an important role of the Benzene plane. In the elongational flow, the Benzene planes will be arranged by the effect of hydrodynamics  and packed locally in parallel. The parallel-packed Benzene planes should become a precursor of a nucleus, which would result in homogeneous nucleation  and formation of 3D-NOCs.
 K. Okada et al., Polymer J. 42, 464 (2010). (link)
 K. Okada et al., Polymer J. 45, 70 (2013). (link)
 T. Tatsumi, Ryutairikigaku, p.171 (Baifukan Co. Ltd., Tokyo, Japan, 1982).
 F. P. Price, in Nucleation (ed. A. C. Zettlemoyer) Ch.8 (Marcel Dekker, Inc., New York, USA, 1969).
M. Hikosaka1, K. Okada1, K. Yasui2, M. Ishikawa3 and H. Masunaga4
1Graduate school of integrated arts and sciences, Hiroshima University, Japan.
2Bridgestone corp., Japan, 3ASAHI KASEI corp. , Japan.
4Japan synchrotron radiation research institute (JASRI), SPring-8, Japan.
We found that polyamide 66 (PA66) crystallizes into novel “bi-axial nano-oriented crystals (bi-NOCs)”, when the supercooled melt was elongated above a critical elongational strain rate.
We used PA66 (Mw=87×103, Mw/Mn=2.31). We used roll system to generate strain rate. We observed the structure and morphology of NOCs by means of polarizing optical microscope and small/wide angle X-ray scattering from three directions, through, edge and end. Polarizing optical micrographs suggested the formation of NOCs. SAXS patterns showed typical two-point pattern, which indicates the formation of NOCs. The two-point pattern showed orientation along machine direction (MD) for through and edge view, while along normal direction (ND) for end view. Size of a nano crystal (NC) was 11nm along MD and ND. WAXS patterns showed chain orientation along MD for through and edge views, while along ND for end view. From these observed facts, we concluded that the arrangement of NCs and chains showed bi-orientation along MD and ND.
The bi-orientation of NCs and chains suggests the important role of hydrogen bond planes (HBPs) in formation of NOCs. As the crystals of PA66 includes “rigid” HBPs, the HBPs should change into hydrogen bond clusters (HBCs) after melting. The HBCs should become nuclei. Under large strain rate, the HBCs would be parallelly oriented to the roll surface due to hydrodynamic effect, which should be the reason of the formation of bi-NOCs.
 Bunn, C. W. & Garner, E. V. Proc. Royal Soc. London, A(189), 39 (1947). (link)
Jia-Ru Xu, Shuang Yang, and Er-Qiang Chen
Beijing National Laboratory for Molecular Sciences, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, College of Chemistry,
Peking University, Beijing 100871, China
Nylon 46 (PA46) is an important engineering plastic. Two crystal structures, monoclinic and triclinic, have been proposed for the α form of PA46. To distinguish which one is more suitable for the melt crystallized PA46, we prepared double oriented samples of PA46 by mechanical rolling at 180 °C followed by annealing at 260 °C. The samples showed the typical α phase diffractions. Combining the two-dimensional (2D) wide-angle X-ray diffraction (WAXD) patterns obtained with the X-ray beam perpendicular and parallel to the chain axis, we concluded that PA46 adopted the monoclinic structure that was determined by Atkins based on the electron diffraction of single crystals grown from solution . On heating, the room temperature α phase firstly transformed into high temperature α phase, and then changed into γ phase which is pseudo-hexagonal . We observed that directly cooling down the sample after high temperature rolling could result in the γ phase retained at room temperature, which was evidenced by 2D WAXD. This room temperature γ phase was a new observation. It was relatively stable and would transform to high temperature γ upon heating. For comparison, we also studied the thermal transition of the melt quenched samples. The obtained amorphous PA46 crystallized in γ phase during heating. The non-oriented γ phase would change into α phase during cooling, showing the typical Brill transition.
 Atkins, E.D.T., Hill, M., Hong, S.K., Keller, A. Organ, S. Macromolecules 25, 917 (1992). (link)
 Ramesh, C. Macromolecules 32, 3721 (1999). (link)
N. Hasan, T. M. H. Nguyen, A.-K. Flieger and J. Kressler
Faculty of Natural Sciences II, Martin Luther University Halle-Wittenberg, Von-Danckelmann-Platz 4, D-06120 Halle (Saale), Germany.
Perfect isotactic poly(methacrylic acid) (i-PMAA) was synthesized and characterized by NMR spectroscopy. Langmuir isotherms of i-PMAA were measured and compared with atactic PMAA. The crystallization of i-PMAA on the water surface strongly depends on the pH-value of the subphase. We found that i-PMAA solutions can immediately form crystalline nanoparticles upon spreading at the air-water interface at neutral pH value. They have diameters of approximately 14 nm to 40 nm and their size can be increased 60 nm to 100 nm without aggregation upon compression on the Langmuir trough. Helical structures are observed when i-PMAA is spread on water having pH value of 10. The morphology of i-PMAA was studied after transfer in LB films by AFM. i-PMAA can also be crystallized in thin films after treatment for several weeks with water. Wide-angle X-ray diffraction (WAXD) studies of these films show a new Bragg reflection at 2θ = 7° (d = 1.20 nm) indicating the crystallization of i-PMAA which might correspond to the helical pitch distance as known for isotactic poly(methyl methacrylate) (i-PMMA) [1-3]. The crystallization is also observed by polarized optical microscopy and AFM.
 E. van den Bosch, Q. Keil, G. Filipcsei, H. Berghmans and H. Reynaers, Macromolecules 37, 9673 (2004). (link)
 H. Ajiro, M. Akashi, Macromol. Rapid Commun 31, 714 (2010). (link)
 D. Kamei, H. Ajiro, C. Hongo and M. Akashi, Langmuir 25, 280 (2009) (link)
Xia Dong*, Lili Wang, Ping Zhu, Yunyun Gao, and Dujin Wang
Beijing National Laboratory for Molecular Sciences, CAS Key Laboratory of Engineering Plastics, Institute of Chemistry Chinese Academy of Sciences, Beijing, 100190, China
Deformation-induced microstructure evolution of a long chain aliphatic polyamide, with an emphasis on lamella development, polymorphism transition and molecular orientation, is investigated in this work. When the materials was deformed above Tg of polyamide1012, a series of complex SAXS patterns are continuously identified at intermediate strain including four points, a figure-eight and an X-shaped pattern, accompanied with two-bars pattern on the meridian, which corresponds to the transient microstructure. Such particular structure is resulted from the approach of tilted lamellae along the drawing direction, the insertion and the orientation of new lamellae. To investigate the temperature dependence, the microstructure developments at different temperature, which was below, above, or close to Tg, are compared. Based on the comprehensive results, the correlation between microstructure and mechanical response has been successfully established, which is featured by the synchronous occurrence of transient structure with slight strain hardening.
Jiayi Zhao1, Yingying Sun2, and Yongfeng Men1
1State Key Laboratory of Polymer Physics and Chemistry, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, University of Chinese Academy of Sciences, Renmin Street 5625, 130022 Changchun, P.R.China
2ExxonMobil Asia Pacific Research & Development Co., Ltd, 1099 Zixing Road, Minhang District, 200241 Shanghai, P.R.China
￼Isotactic polypropylene (iPP) is a widely used commercial polymer with various polymorphs. γ-form, which can only crystallize at high pressure for isotactic polypropylene, is a usual polymorph for propylene copolymers. The subsequent crystallization behavior during cooling for copolymer initially in pure α-form and γ-form processed at different melt temperature has been studied . Specifically, sample initially in α-form led to higher fraction of γ-form (fγ) and onset crystallization temperature (Tonset) than that of sample in γ-form under low melted temperature, which was caused by the difference between morphology of samples previously in α-form and γ-form.
Tensile deformation properties of the propylene/ethylene copolymers were also studied [2, 3]. The influence of stretching temperature and content of co-unit in transition behavior from γ-form to α-form during stretching was investigated. The critical stress for the polymorph transition was obtained which depends strongly on the stretching temperature and content of co-unit. The critical stress was higher for sample with lower co-unit content with less partitioning of ethylene co-unit in propylene crystalline lattices.
This work is supported by NSFC (21134006, 51525305) and ExxonMobil.
 Zhao, J.; Sun, Y.; Men, Y. Ind. Eng. Chem. Res. 56, 198 (2017). (link)
 Zhao, J.; Sun, Y.; Men, Y. Macromolecules 49, 609 (2016). (link)
 Zhao, J.; Sun, Y.; Men, Y. Submitted.
B. Zhang and J. B. Chen
School of Materials Science & Engineering, Zhengzhou University, Zhengzhou 450002, People’s Republic of China
Based on a control of the melt structure at temperatures near but below the equilibrium melting point we investigated the role of shear stress imposed by the wall of the capillary die on crystal morphology of isotactic polypropylene (iPP). Bundles of partially ordered nanoscale chain segments within the quiescent melt at temperatures between the nominal melting temperature and the equilibrium melting point allowed for the possibility of shear-induced or shear-assisted formation of crystalline cylindrites which were investigated by means of polarized optical microscopy and small/wide-angle X-ray scattering.1-4 The SAXS patterns of near melting point structured melt monitored at 180 °C can be fitted by using a form factor for polydisperse cylinders. It was found that the average radius and height of the bundles of partially ordered chain segments were about 17 nm and 40 nm, respectively. For a given structured melt, the number of cylindrites increased with shear stress. Concomitantly, the nucleation density of α-iPP within a single cylindrite structure increased with shear stress at the expense of β-iPP nucleation density.
 Zhang, B.; Chen, J.; Zhang, X.; Shen, C. Polymer 52, 2075 (2011). (link)
 Zhang, B.; Chen, J.; Ji, F.; Zhang, X.; Zheng, G.; Shen, C. Polymer 53, 1791 (2012). (link)
 Zhang, B.; Chen, J.; Cui, J.; Zhang, H.; Ji, F.; Zheng, G.; Heck, B.; Reiter, G.; Shen, C. Macromolecules 45, 8933 (2012). (link)
 Zhang, B.; Wang, B.; Chen, J.; Shen, C.; Reiter, R.; Chen, J.; Reiter, G. Macromolecules 49, 5145 (2016). (link)
Institute of Polymer Science & Engineering, Department of Chemical Engineering, Tsinghua University, Beijing 100084, China
￼Nucleation is a fundamental step of polymer crystallization and the mechanism is not fully understood yet . Classical nucleation theory based on the capillary approximation has achieved success in the field of polymer crystallization; however, there are still some open questions remained: (1) Which pathway is chosen for nuclei formation of polymer lamellar crystals, stem by stem or cluster by cluster? (2) How to describe the many intermediate states during nucleation? In this work, we propose a microscopic kinetics model without the prerequisite thermodynamics parameters. In our new model, crystal nucleation is considered as a series of elementary processes: attaching and detaching of units. Correlation factors were introduced to describe the variation of the rate constants to attach and detach a unit with the cluster size. Via the microscopic kinetics, we can determine the equivalent thermodynamics parameters and simulate the time evolution of cluster size distribution . Application of the new model to some polymers will be given. The critical size of nuclei in poly(butylene succinate) during crystallization and melting will be estimated. The model describes nucleation of small molecules and polymer chains in a unified view, which we believe can be applied to other kinetic processes far from equilibrium.
 M. C. Zhang, Y. Gao, B. H. Guo, J. Xu, Crystals 7(1), 4 (2017). (link)
 K. L. Xu, B. H. Guo, R. Reiter, G. Reiter, J. Xu, Chinese Chemical Letters
26, 1105 (2015). (link)
B. Wang,1 T. Wen,2 X. Zhang,3 D. Wang,4 D. Cavallo1
1 Department of Chemistry and Industrial Chemistry, Genova (Italy)
2 Department of Chemical Engineering, Hsinchu (Taiwan)
3 Beijing Institute of Fashion Technology, Beijing (China)
4 Institute of Chemistry Chinese Academy of Sciences, Beijing (China)
￼Fiber-reinforced semicrystalline polymer composites are largely employed for their improved strength with respect to the pure polymer matrix. The adhesion between the polymer and the fiber is known to play a key role in determining the overall mechanical behavior. When semicrystalline polymers are employed, the heterogeneous nucleation on the surface of the solid fiber is an efficient way to improve the adhesion and speeding up the composite production rate. However, fiber induced nucleation studies are still scarce and mainly limited to polyolefins, despite the increasing importance of bio-based polymers and composites.
In the work, the nucleation process of polylactide (PLA) on several fibers was studied in-situ by means of hot-stage polarized optical microscope. Several commercially available fibers (i.e., PET, Kevlar and glass fibers) are employed and compared to stereocomplex enantiomeric PLA blend and annealed homochiral PLA fibers. The nucleating efficiency of the various heterogeneous substrates is quantitatively compared on the basis of the derived free energy barrier for critical nucleus formation, ΔG*.
It results clear that the PLA stereocomplex fibers has higher nucleating ability, due to the identical surface chemistry between the substrate and PLA homocrystal, although the crystalline structure of stereocomplex and homochiral crystals is not the same. On the other hand, the nucleation kinetics of PLA homocrystal on fibers of the very same crystal is even more efficient, and simply follows the secondary nucleation process: the induction times for the birth of the nucleus display the same temperature dependence of crystal growth.
Xiaoliang Tang, Junsheng Yang, Tingyu Xu, Fucheng Tian, Chun Xie, Liangbin Li
National Synchrotron Radiation Lab and CAS Key Laboratory of Soft Matter Chemistry, University of Science and Technology of China, Hefei, China
Flexibility and connectivity are the most prominent characteristics of polymer, how does flexible chain transform into rigid conformational ordered segments may be the key step for crystallization . We investigate the nucleation process of polyethylene with full-atom molecular dynamic simulation, during which the structural evolution is analyzed with three order parameters, including conformational order, modified bond-orientational order  and density. Coupling between conformational and bond-orientational orderings results in the formation of hexagonal clusters first, which is dynamic in nature and absence of density order. Whilst nucleation of orthorhombic clusters occurs inside hexagonal clusters later, which involves all three order parameters and proceeds via the coalescence of neighboring hexagonal clusters rather than standard stepwise growth process. This demonstrates that nucleation of PE crystal is a two-step process with the assistance of bond-orientational order, which is different from early models for polymer crystallization but in line with that proposed for spherical “atoms” like colloid and metal.
 Su F, Ji Y, Meng L, et al. Coupling of Multiscale Orderings during Flow- Induced Crystallization of Isotactic Polypropylene. Macromolecules, 2017, 50(5): 1991-1997. (link)
 Yang J, Tang X, et al. Coupling between intra-and inter-chain orderings in flow-induced crystallization of polyethylene: A non-equilibrium molecular dynamics simulation study. The Journal of Chemical Physics, 2017, 146(1): 014901. (link)