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Structural Studies of Proton-Conducting Fluorous Block Copolymer Membranes Barbara Frisken – SFU Physics Laurant Rubatat - University of Fribourg Ken Shi.

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Presentation on theme: "Structural Studies of Proton-Conducting Fluorous Block Copolymer Membranes Barbara Frisken – SFU Physics Laurant Rubatat - University of Fribourg Ken Shi."— Presentation transcript:

1 Structural Studies of Proton-Conducting Fluorous Block Copolymer Membranes Barbara Frisken – SFU Physics Laurant Rubatat - University of Fribourg Ken Shi – NRC IFCI Steven Holdcroft – SFU Chemistry and NRC IFCI Olivier Diat – CEA Grenoble

2 Two Series of Diblock Copolymers Series #1 – Variable Sulfonation 22% 32% 40% Sulfonation Rate 1B 1A 1C A B Poly(Vinylidene DiFluoride-co-Hexafluoropropylene) P(VDF-co-HFP) Sulfonated PolyStyrene sPS 17,900 g/mol 8,000 g/mol

3 9 12.5 18 2B 2A 2C 25,000 g/mol Degree of polymerization A B Poly(Vinylidene DiFluoride-co-Hexafluoropropylene) P(VDF-co-HFP) Sulfonated PolyStyrene sPS 1000-2000 g/mol Two Series of Diblock Copolymers Series #2 – Variable sPS Length

4 Conductivity and TEM Z. Ken Shi (2A) (2B) (1B) (1A) (2C) (1C) Nafion

5 Conductivity and TEM Z. Ken Shi (2A) (2B) (1B) (1A) (2C) (1C) Nafion 1A 1B 1C 2B 2C

6 SANS Studies The scattered intensity is proportional to the product of a structure factor S(q) and a form factor P(q): where P(q) describes the shape of the scattering objects and S(q) describes the spatial distribution of these objects. Neutron Beam Sample Detector 

7 Peak #1 Peak #2 Series #1 – Two Peaks Peak #1  400 Å Peak #2  40 Å Slight shift of the peaks to small angles  size increasing with IEC. Neutron Scattering Spectra – in D 2 O Series #2 – Two Peaks Peak #1  400 Å Peak #2  40 Å Peak #1 is less sharp  less ordered Peak #2 Peak #1 Series #1 – Partially SulfonatedSeries #2 – Variable Length

8 Contrast Variation Peak #1 Peak #2 Membrane 2B Peak #1 Membrane 1C Peak #2 Series #1 – Partially SulfonatedSeries #2 – Variable Length

9 Contrast Variation Series #1 Peak #1 Peak #2 Binary System Structure enhanced or diminished Ternary System Match core Match corona Membrane 1C

10 Spectra Divisions Membrane 1C t s r Core-shell disk form factor R >> t + 2s => Lamellar

11 Series #1 – Partially sulfonated PVDF PS Hydrated sPS 25 Å 165 Å 280 Å 180 Å 220 Å 30 Å170 Å 28 Å 180 Å Solvent pool 1B 1A 1C  p = 56 %  p = 30 %  p = 25 %

12 Series #2 – Fully sulfonated Contrast Variation Peak #1 Peak #2 Membrane 2B Binary System Structure enhanced or diminished

13 Small Length Scale Structure Modified hard-sphere model Yarusso and Cooper, Macromolecules 1983 Spherical ionic aggregates within PS matrix Hydrated sPS domain Increasing sulfonation from 22-100% leads to a decrease in the size of the barrier between ionic groups – consistent with improved conductivity.

14 Series #1 Series #2 40 Å 400 Å Fluorous domains and Hydrated sPS domains Solvent pools in a PS matrix

15 f  Volume fraction of A block (from data)  N  Interaction between blocks (not known) Series #1 Series #2 Series #1 shows lamellar structure Series #2 shows phase separation, but no long range order Compare to diblock copolymer theory Matsen and Bates, Macromolecules 1996 Q Im3m spheres H cylinders Q Ia3d bi-continuous L lamellar

16 Conductivity and SANS (2A) (2B) (1B) (1A) (2C) (1C) Nafion Large scale structure is more ordered in Series #1 sPS domains are similar Large scale structure affects the integrity of the membrane, but not the conductivity 1A 2C


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