Investigation on the growth of snowflake-shaped Poly(l-Lactic acid) crystal by in-situ high-pressure microscope
Graphical abstract
Introduction
Crystallization of polymer molecules from melt film is a widely concerned condensed matter phenomenon [1] that can realize the closely packing of the long-chain molecular and functional group. The crystal morphology directly influences the chemical and physical characters of polymer film [1,2], and the morphology control plays a key role in functional film engineering [3]. So, understanding of the dependence of polymer film morphology on controlled variables and the crystal formation mechanism from melt film is of great significance.
The crystal of polymer film generally shows various morphologies including spherulite [4], seaweed-shape crystal [5], petal-like crystal [6] crystallographic dendritic crystal [7], polygonal single crystal [3,8] and so on. Among these crystal morphologies, the crystallographic dendritic crystal, believed as the transition morphology from non-crystallographic crystal to single crystal [[8], [9], [10], [11]], is receiving considerable attention. Snowflake-shape crystals were prepared by controlling thickness and temperature of isotactic Polystyrene (iPs) film [9] and Poly(l-Lactic Acid) (PLLA) film [15]. Wang et al. [[11], [12], [13], [14]] prepared Poly(ethylene oxide) (PEO) dendritic crystal with four growth directions through tune film thickness, temperature, and molecular weight. Based on the understanding on the interplay between crystallization and phase separation [16,17], crystallographic dendritic crystal was formed in the polymer blend system, like PEO/Poly(methyl meth acrylate) (PMMA) [18], PLLA/Poly(1,4-butylene adipate) [19,23], Tannin/Poly(ethylene succinate) [20], Poly(d-lactic acid)/Poly(1,4-butylene adipate) [21] and PLLA/PEO [22]. Furthermore, the crystallographic dendritic crystal of block copolymer was also induced by phase separation [[24], [25], [26]].
The formation process of these aesthetic structures also elicits a widespread interest. It is well known that the six main branches of snow originated from the six preferentially growing directions of hexagonal water single crystal [27]. Same with the growth mode of water molecule, the faceted structures assembled by PEO, Poly-2-vinylpyridineblock-polyethyleneoxid [28], iPS [29] and Polyoxymethylene [30] also developed from the preferentially growing directions of quadrangular crystal or hexagonal crystal. But there is an exception to this rule. Based on the previous research on PLLA crystal, at a relative low temperature of crystallization, the PLLA molecules will assemble a rhombic single crystal with two preferentially growing directions [[31], [32], [33]]. Interestingly, the rhombic crystals assemble a snowflake-shaped crystal with six main branches [19,21,22,34]. Through phase-separation-induced crystallization, Nurkhamidah and Woo [19] proposed a growth and packing mode of single crystals into snowflake-shaped dendritic crystal. Generally, the research method to speculate the growth process of polymer crystal according to the final crystal morphology is called as inversion method (sometimes called as archaeological method). The existing understanding of crystal morphology evolution of PLLA thin film is based on this inversion method, and the growth mode of snowflake-shaped PLLA crystal is still questionable.
In order to study the growth of snowflake-shaped PLLA crystal, it is needed to develop new methods and new tools. For many polymer materials, CO2 is a kind of poor solvent which can swell but not dissolve the most of polymer [35]. Previous researches indicated that CO2 can influence the glass transition temperature, melt temperature, supercooling degree [36,37], crystallization rate [38], crystallinity [39] and mesophase [40,41] of polymer bulk. For the polymer thin film, CO2 molecules can quickly embed into the film or escape from the film due to the feature of gas-like viscosities and liquid-like densities, especially in the supercritical state (temperature higher than 31 °C and pressure higher than 7.38 MPa) [35]. Based on the previous research, CO2 has been proved as a gentle tool to tune the crystallization behavior of polymer. Moreover, the pressurized CO2 can slow down the growth rate of polymer crystal [36] which provides a window to present more detail of the crystal growth process. However, the morphology and the crystal growth of polymer film are influenced by many factors including polymer molecular structure and environmental variants. In this way, to reveal the whole formation process of snowflake-shaped crystal, a reasonable crystallization condition should be firstly determined by considering PLLA degradation, observable crystal size, and recordable growth time.
In this paper, we developed an in-situ high-pressure observing system with special designed sample cell whose temperature and pressure can be close-loop controlled. The crystal growth process of Poly(l-Lactic Acid) (PLLA) film was recorded by this system in pressurized CO2 environment with different film thicknesses, different molecular weights, different temperatures and different CO2 pressures. With a reasonable selection of experimental parameters, the preliminary stage of formation process of snowflake-shaped crystal was recorded by the self-established system. With the help of atomic force microscope, we tentatively concluded the growth mode of the snowflake-shaped PLLA crystal.
Section snippets
Materials
CO2 with a purity of 99.999% was supplied by Jinan Deyang special Gas Co., Ltd., China. Two pristine PLLA samples were purchased from Jinan Daigang Biomaterial Co., Ltd., China. The PLLA samples were firstly purified two times by reprecipitation method using chloroform as solvent and methanol as precipitant, and then purified two times by solution suction filtration using excess ethyl acetate as solvent. The polymer was dried 10 days at 50 °C in a vacuum drying oven to remove any moisture in
Morphology of PLLA film treated by pressurized CO2
PLLA is a kind of degradable polymer especially at the high temperature state. In order to study the dependence of crystal morphology on molecular weight in a single variable experiment, we control the holding time of PLLA film at the melt state to qualitatively tune the molecular weight. The different holding time at melt state will cause the different degrees of degradation of PLLA which correspond to the different molecular weights. Fig. 5 gives the morphology of the films with five
Conclusion
In summary, we developed an in-situ high-pressure observing system with special designed sample cell whose temperature and pressure can be close-loop controlled. The crystal morphology of PLLA film was recorded by this system in pressurized CO2 environment with different film thicknesses, different molecular weights, different temperatures and different CO2 pressures. The whole process of morphological evolution of snowflake-shaped crystal was firstly recorded which show a quite different
Acknowledgments
The authors are grateful to the financial support from the Climbing Program for Taishan Scholars of Shandong Province of China (No. 20110804) Research Award Fund for Shandong Province Excellent Innovation Team (No. 2012-136).
References (53)
- et al.
Comprehensive review on polymer single crystals from fundamental concepts to applications
Prog. Polym. Sci.
(2018) - et al.
Polymer spherulites: a critical review
Prog. Polym. Sci.
(2016) Crystallization and morphology of ultrathin films of homopolymers and polymer blends
Prog. Polym. Sci.
(2016)- et al.
Labyrinthine pattern of polymer crystals from supercooled ultrathin films
Polymer
(2010) - et al.
Crystal growth pattern changes in low molecular weight poly (ethylene oxide) ultrathin films
Polymer
(2011) - et al.
Dendritic crystallization in thin films of PEO/PMMA blends: a comparison to crystallization in small molecule liquids
Polymer
(2008) - et al.
Effects of surface wetting induced segregation on crystallization behaviors of melt-miscible poly (L-lactide)-block-poly (ethylene glycol) copolymer thin film
Polymer
(2013) - et al.
General crystallization behaviour of poly (L-lactic acid)
Polymer
(1980) - et al.
Fractal crystal growth of poly (ethylene oxide) crystals from its amorphous monolayers
Polymer
(2008) - et al.
On the origins of giant screw dislocations in polymer lamellae
Polymer
(2002)
The frustrated structure of poly (L-lactide)
Polymer
Structure in thin and ultrathin spin-cast polymer films
Science
Order in Thin Organic Films
Growth of 'dizzy dendrites' in a random field of foreign particles
Nat. Mater.
Morphological changes of isotactic polypropylene crystals grown in thin films
Macromolecules
A general mechanism of polycrystalline growth
Nat. Mater.
Crystal growth of isotactic polystyrene in ultrathin films: thickness and temperature dependence
J. Macromol. Sci., Part B: Physics
Crystal growth of isotactic polystyrene in ultrathin films: film thickness dependence
J. Macromol. Sci., Part B
Crystal pattern formation and transitions of PEO monolayers on solid substrates from nonequilibrium to near equilibrium
Macromolecules
Morphology diagram of single-layer crystal patterns in supercooled poly (ethylene oxide) ultrathin films: understanding macromolecular effect of crystal pattern formation and selection
ACS Macro Lett.
The crystallization of ultrathin films of polylactides Morphologies and transitions
Can. J. Chem.
Dynamic competition between crystallization and phase separation at the growth interface of a PMMA/PEO blend
Macromolecules
Lamellar orientation inversion under dynamic interplay between crystallization and phase separation
Macromolecules
Phase-separation-induced single-crystal morphology in poly (l-lactic acid) blended with poly (1, 4-butylene adipate) at specific composition
J. Phys. Chem. B
Tannin induced single crystalline morphology in poly (ethylene succinate)
Macromol. Chem. Phys.
Oppositely synchronized lamellar bending in poly (l-lactic acid) versus poly (d-lactic acid) blended with poly (1, 4-butylene adipate)
Macromol. Chem. Phys.
Cited by (11)
Crystallization behavior and secondary nucleation model of PP/GN nanocomposites under supercritical N<inf>2</inf>
2022, Composites CommunicationsBatch foaming of ultra-high molecular weight polyethylene with supercritical carbon dioxide: Influence of temperature and pressure
2021, Polymer TestingCitation Excerpt :As completely dissolved into a transparent gel, the gelatinous dissolutions are dripped onto a glass substrate. The glass substrate was cleaned by immersion in Piranha solution of H2SO4(98%)/H2O2(30%) with a volume ratio of 7:3 in glass ware at 100 °C for 5 h to remove any organic contamination and make the surface hydrophilic [18]. Another piece of glass substrate was covered on UHMWPE gel to form a thin film thickness of about 15 μm for observation.
Green fabrication method of layered and open-cell polylactide foams for oil-sorption via pre-crystallization and supercritical CO<inf>2</inf>-induced melting
2020, Journal of Supercritical FluidsCitation Excerpt :The coupling relationship among them and its intrinsic mechanism are complex scientific problems that need to be solved. First, at the CO2 saturation stage, the dissolved CO2 has the plasticization effect on the polymer, which can lower the glass transition temperature (Tg), crystallization temperature (Tc) and melting temperature (Tm) [25–27], and changes the crystallization kinetics [26–29] and crystal morphology [30,31]. In addition, the crystallization and melting of the polymer can conversely affect the CO2 dissolution behavior [32,33].
Crystal Structure and Thermal Properties of Polypropylene Prepared by Variable Speed Pressurization
2022, Gaoya Wuli Xuebao/Chinese Journal of High Pressure Physics