The scientific goal of this study is in depth understanding of the fundamental properties of the carbon materials and their functionality at the molecular and atomic level under non-polarized conditions. For this purpose the nanoporous carbon RP-20 [7] as a main electrode component has been used and correlation between morphology (i.e., pore shape, size of the pores) and instance wetting (filling density) of the carbon material matrix with the solvent was determined. Keeping in mind real application requirements, the primarily used 1M NaClO4 solution in dimethyl carbonate (DMC) and ethylene carbonate (EC) (1:1 wt%) solvent mixture as an electrolyte [3] has been studied. Several independent methods – x-ray microcomputed tomography (µCT) [8], small-angle neutron scattering (SANS) [9], and small-angle x-ray scattering (SAXS) [10-12] were applied for characterization of the following systems: RP-20 1MNaClO4 in EC:DMC; RP-20 in EC:DMC or RP-20 1MNaClO4 in D2O. It is rather difficult to simultaneously determine/distinguish the structure or dynamic effects on the efficiency and durability of the electrochemical devices (i.e., inhomogeniously/randomly distributed pores filled with electrolyte contributing during the charge and discharge cycling processes), therefore the above listed methods have contributed to an improved awareness of the nature of complex systems in steady state (non-polarized) conditions. Based on the µCT measurements, the linear attenuation coefficient values and filling densities were obtained and calculated. To determine the shape and size of the pores for nanoporous RP-20 electrode and to observe the influence/interaction of the electrolyte ions dissolved in aqueous and non-aqueous solvent (i.e., differences in filling of the pores) SANS method was applied. SAXS measurements were performed in order to collect quantitative morphological and structural information for nanoporous RP-20 powder and RP-20 electrode material (e.g., surface area, pore size, pore structure, binder effect).
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Acknowledgments
The Authors would like to thank HZB for the allocation of neutron radiation beamtime on instrument V4. This project has received funding from the European Union's Seventh Framework Programme for research, technological development and demonstration under the NMI3-II Grant number 283883, The Estonian Ministry of Education and Research (institutional research project IUT20-13, personal research grant PUT55) and European Regional Development Fund (The Centres of Excellence TK117 and, TK141).