Proton Conduction in Thickness-Controlled Ultrathin Polycation/Nafion Multilayers Prepared via Layer-by-Layer Assembly
Yusuke Daiko, Kiyofumi Katagiri, Atsunori Matsuda
Abstract
Yusuke Daiko, Kiyofumi Katagiri, Atsunori Matsuda
Abstract
Ultrathin layers of positively charged poly(allylamine hydrochloride) (PAH) and a negatively charged high-proton conductor of Nafion were alternately deposited via layer-by-layer assembly. The incremental film growth of PAH and Nafion multilayers was monitored using a quartz crystal microbalance (QCM). The results obtained using the QCM revealed that each PAH/Nafion multilayer was deposited regularly and homogeneously. The ζ-potential and thickness of the Nafion layer, which are related to the concentration of free −SO 3 − groups, were changed significantly by varying the pH of the PAH solution used. The thickness of one Nafion layer was controlled in the range from approximately 4 to 15 nm. The surface charge density of the PAH/Nafion multilayer was estimated using a Poisson−Boltzmann equation. A linear relationship between the proton conductivity and surface charge density of the outmost Nafion layer was observed. Furthermore, the proton mobility of the PAH/Nafion multilayer (15.2 cm 2 /(V s)) was about sevenfold higher than that of a bulk Nafion membrane (2.0 cm 2 /(V s)).
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Ultrathin layers of positively charged poly(allylamine hydrochloride) (PAH) and a negatively charged high-proton conductor of Nafion were alternately deposited via layer-by-layer assembly. The incremental film growth of PAH and Nafion multilayers was monitored using a quartz crystal microbalance (QCM). The results obtained using the QCM revealed that each PAH/Nafion multilayer was deposited regularly and homogeneously. The ζ-potential and thickness of the Nafion layer, which are related to the concentration of free −SO 3 − groups, were changed significantly by varying the pH of the PAH solution used. The thickness of one Nafion layer was controlled in the range from approximately 4 to 15 nm. The surface charge density of the PAH/Nafion multilayer was estimated using a Poisson−Boltzmann equation. A linear relationship between the proton conductivity and surface charge density of the outmost Nafion layer was observed. Furthermore, the proton mobility of the PAH/Nafion multilayer (15.2 cm 2 /(V s)) was about sevenfold higher than that of a bulk Nafion membrane (2.0 cm 2 /(V s)).
Key concepts: Nafion, Quartz crystal microbalance, Layer (electronics), Materials science, Layer by layer, Analytical Chemistry (journal), Conductivity, Ionomer