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JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構

JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構

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1-34<br />

Nanoscale Structures of Radiation-Grafted<br />

Polymer Electrolyte Membranes Investigated<br />

by Dissipative Particle Dynamics Simulation<br />

S. Sawada a) , T. Yamaki a) , A. Suzuki b) , T. Terai b) and Y. Maekawa a)<br />

a) Environment and Industrial Materials Research Division, QuBS, <strong>JAEA</strong>,<br />

b) Graduate School of Engineering, The University of Tokyo<br />

A radiation-grafting method is one of the promising<br />

techniques for preparing polymer electrolyte membranes<br />

(PEMs) for fuel cell applications. In the research of the<br />

radiation-grafted PEMs, much effort has been devoted to<br />

improve their properties (proton conductivity, chemical<br />

stability, mechanical strength, etc.) by the best combination<br />

of base polymer films and graft monomers. As part of their<br />

basic science studies, we investigated the nanoscale<br />

structures of the PEMs by a dissipative particle dynamics<br />

(DPD) simulation. The simulation target was our original<br />

PEM synthesized by the radiation grafting of styrene into<br />

crosslinked-polytetrafluoroethylene (PTFE) and subsequent<br />

1-3)<br />

sulfonation .<br />

4)<br />

According to our recent report , we modeled the grafted<br />

electrolyte polymers with ion exchange capacities (IECs) of<br />

0.89 - 2.2 meq/g. Based on the molecular structures, the<br />

atom groups of (CF2) 6 –CH(C6H4SO3H)CH2, and 7<br />

water molecules were represented as particles A, B and W,<br />

respectively. The interaction parameters between the two<br />

particles of the A-B, A-W, or B-W pair were calculated by a<br />

full-atomistic simulation. The molecular architecture (e.g.,<br />

the length of PTFE main chains, the length of graft chains,<br />

and the number of graft chains per molecule) was<br />

determined based on the experimental data. As the initial<br />

state, the electrolyte polymers and a fixed number of<br />

particles W were randomly located in a cubic cell with the<br />

three-dimensional periodic boundaries. After 50,000 time<br />

steps, all the systems reached the equilibrated states. For<br />

comparison, a DPD simulation was also performed on<br />

5)<br />

Nafion .<br />

Figure 1 shows the snapshots of the simulation results in<br />

the equilibrated states. As in both (a) and (b), particles W<br />

appeared to be mixed with particles B while, in contrast,<br />

particles W in Nafion aggregated alone to grow larger.<br />

This finding indicates that, unlike Nafion, in which water<br />

clusters were excluded from any polymer parts, the<br />

water-filled regions were not clearly separated from the<br />

poly(styrene sulfonic acid) (PSSA) graft chains.<br />

In order to obtain quantitative information on nanoscale<br />

structures, we calculated the radial distribution function<br />

between particles W, GWW(r). The GWW(r) was defined as:<br />

n W<br />

GWW<br />

r <br />

, (1)<br />

2<br />

4π<br />

r r<br />

φW<br />

where nW is the average number of particles W existing<br />

in the distance between r and r +Δr from any particle W.<br />

Figure 2 shows the GWW(r) for the hydrated electrolyte<br />

<strong>JAEA</strong>-<strong>Review</strong> <strong>2010</strong>-065<br />

- 38 -<br />

polymers. In the case of Nafion, there were sharp peaks at<br />

r = 0.60, 1.0 and 1.5 nm. These three peaks are considered<br />

to originate from the first, second and third nearest W<br />

particles, respectively, in the same cluster. At r = 3.4 nm,<br />

the GWW(r) dropped to under 1, which suggests the edge of a<br />

5)<br />

water cluster . Accordingly, the diameter of the water<br />

cluster, dC, was twice as much as this value, i.e., 6.8 nm.<br />

For the grafted electrolyte polymers, the GWW(r) dropped to<br />

under 1 at r = 0.88 nm, corresponding to dC of 1.8 nm. This<br />

result is in good agreement with the diameter obtained<br />

previously by the small-angle X-ray scattering analysis<br />

6)<br />

(1.7 nm ). It was found that a low of these small clusters<br />

would exist surrounded by PSSA graft chains. Such unique<br />

nanoscale structures were possibly related to the high proton<br />

conductivity and low water diffusivity of the grafted PEMs.<br />

-(CF 2) 6-<br />

-CH-CH 2-<br />

SO 3 H<br />

A<br />

B<br />

7H2O W<br />

(a) (b)<br />

Fig. 1 Snapshots of the simulated polymer electrolyte in<br />

the IEC of (a) 0.89 and (b) 2.2 meq/g.<br />

G WW(r)<br />

3<br />

2<br />

1<br />

Grafted PEM (0.89 meq/g)<br />

Grafted PEM (2.2 meq/g)<br />

Nafion<br />

0<br />

0 1 2 3 4 5<br />

r (nm)<br />

Fig. 2 The GWW(r) as a function of r.<br />

References<br />

1) T. Yamaki et al., Polymer 45 (2004) 6569.<br />

2) S. Sawada et al., Trans. Mater. Res. Soc. Jpn. 30 (2005)<br />

943.<br />

3) S. Sawada et al., Solid State Inoics 179 (2008) 1611.<br />

4) S. Sawada et al., Kobunshi Ronbunshu 67 (<strong>2010</strong>) 224.<br />

5) S. Yamamoto et al., Polym. J. 35 (2003) 519.<br />

6) M. Elomaa et al., J. Mater. Chem. 10 (2000) 2678.

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