Structures and Surface Wettability of Fluorinated Meth Acrylate Polymers
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- Περικλῆς Βαρνακιώτης
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1 PROGRESS IN CHEMISTRY Vol. 22 No. 6 Jun * O O A X Structures and Surface Wettability of Fluorinated Meth Acrylate Polymers Yang Hao Pi Pihui Wen Xiufang Zheng Dafeng Cheng Jiang Yang Zhuoru School of Chemistry and Chemical Engineering South China University of Technology Guangzhou China Abstract Fluorinated meth acrylate polymers are a class of novel low surface energy materials in which the fluorinated chains confer them hydrophobic and oleophobic properties and the non-fluorinated chains render them fine solubility and compatibility. The surface wettability can be changed by designing and controlling the structures of fluorinated meth acrylate polymers. In this article we review the influence factors of surface wettability for fluorinated meth acrylate homopolymers random block graft core-shell copolymers and crosslinked network copolymers etc. The relationships between the structures and surface wettability including wetting stability of the polymers are discussed by means of analyzing the crystallinity surface element content surface energy and contact angle of the polymers and the related models are also given which providing theoretical basis and guidance for design and synthesis of stable surface wettability of fluorinated meth acrylate polymers. Key words fluorinated meth acrylate polymer structures surface wettability wetting stability contact angle hysteresis Contents 1 Introduction 2 Contact angle hysteresis and wetting stability 3 The influence of fluorinated meth acrylate polymers structures on surface wettability and wetting stability 3. 1 Homopolymers 3. 2 Copolymers 4 Conclusion and outlook * No. 2008B Corresponding author zhryang@ scut. edu. cn
2 / 22 PTFE PVDF PTFE PTFE CF 3 Gibbs 6. 7mN / m 1 PTFE θ A advancing angle θ R receding angle θ A - θ R spacer group vinyl ester CF 2 n - θ A / θ R 3. 1 CH 2 m / 17 n 8
3 Fig. 1 Chemical structures of fluorinated meth acrylate homopolymers 23 2 < n 6 2 Fig. 2 Schematic illustration of structures and models for water repellency of homopolymers 23 γ p γ d n 8 n 6 27 n 2 Corpart 25 N- n = 6 n = 8 N- γ p γ d Caillier 26 n = 6 m m = α- m Saidi 24 n = m = / Hartmann 28
4 / / θ R θ A AIBN BPO θ R m 16 / γ d γ p Fig PFA-ran-PAA Models for water repellency of PFA-ran-PAA 22 CH 2 m Hartmann 17 m = 1 18 m = b 3 Fig. 3 Chemical structures of fluorinated meth acrylate copolymers 10mol% θ A mol% m Morita 22 FA m n = 9 AA m = m = m = 6 PFA-ran-PAA 3 a 11 m < 8 8 m < m = 18 m = 1 16 m 16 m θ A θ R 31 m < 8 θ R 45 m 8 θ R m 16 θ R 98 m < 8 Saidi F CF 2 8 CH 2 m OC O CH CH 2 F 8 A m 16 BA MMA m < 8 F 8 A / BA / γ d γ p / F 8 A / BA / MMA XPS
5 / m 25 5 F 8 A / BA / MMA m = 2 F 8 A / BA m = 8 Takahashi 34 MMA FOM FOSAM MPEGMA MMA / FOSAM MMA / MPEGMA / FOM MMA / FOSAM θ R N S / θ R MMA / MPEGMA / FOM θ R MMA / MPEGMA MMA PEG PEG θ R θ R Fujimori 35 5 a b 35 FF 10 EA Fig. 5 Models for layer structures a acrylate OA FF 10 EA / OA copolymers b methacrylate copolymers 35 FF 10 EMA / OMA X WAXD X SAXS X NEXAFS sub-cell ATRP RAFT FF 10 EA / OA = FF 10 EA / OA = 1 5
6 PSt-b-PFA PFA 18. 7mol% 120 Wang PSt-b- PFMA n m PFA n m miscible state n 6 A S A CF 3 S A 10. 8mN / m n > 6 B S B Valtola 38 CF 3 FMA EIMA 8mN / m PFMA-b-PEIMA PFMA-ran-PEIMA DSC 6 FMA Luo PDMS-b-PMMA-b-PFMA PDMS-b-PFMA PFMA 121 PFMA XPS F / Si PMMA 36 6 end-capped Ni ATRP Fig. 6 Schematic representation of the relationship between 2 3 the fluorinated side chain end structures and their critical surface tensions PMMA-ec- 36 FMA PMMA-ran- PFMA FMA Hikita mol% ATRP
7 mol% FMA wt% PMMA γ d γ p - push-me / pull-you 43 / / PTFE PTFE / PTFE 7 a PMMA-ec-FMA b PMMA-ran- 41 PFMA Fig. 7 a Self-assembly of the PMMA-ec-FMA. b Segregation of the fluorinated components in the PMMA-ran- PFMA Ameduri UV < 1wt% XPS Park 45 / / PFMA-g-PMMA / MMA PMMA FMA / / - Qu
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