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Small‐angle X‐ray scattering study of the smart thermo‐optical behavior of zirconyl aqueous colloids
Author(s) -
Chiavacci L.A.,
Bourgaux C.,
Briois V.,
Pulcinelli S.H.,
Santilli C.V.
Publication year - 2000
Publication title -
journal of applied crystallography
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.429
H-Index - 162
ISSN - 1600-5767
DOI - 10.1107/s0021889899013151
Subject(s) - small angle x ray scattering , aqueous solution , dynamic light scattering , materials science , chloride , colloid , scattering , cluster (spacecraft) , chemical physics , light scattering , analytical chemistry (journal) , chemistry , nanoparticle , chromatography , nanotechnology , optics , physics , metallurgy , computer science , programming language
The smart thermo‐optical systems studied here are based on the unusual thermoreversible sol‐gel transition of zirconyl chloride aqueous solution modified by sulfuric acid in the molar ratio Zr/SO 4 :3/1. The transparency to the visible light changes during heating due to light scattering. This feature is related to the aggregates growth that occurs during gelation. These reversible changes can be controlled by the amount of chloride ions in solution. The thermoreversible sol‐gel transition temperature increases from 323 to 343 K by decreasing the molar ratio Cl/Zr from 7.0 to 1.3. In this work the effect of the concentration of chloride ions on the structural characteristics of the system has been analyzed by in situ SAXS measurements during the sol‐gel transition carried out at 323 and 333 K. The experimental SAXS curves of sols exhibit three regions at small, medium and high scattering vectors characteristics of Guinier, fractal and Porod regimes, respectively. The radius of primary particles, obtained from the crossover between the fractal and Porod regimes, remains almost invariable with the chloride concentration, and the value (4 Å) is consistent with the size of the molecular precursor. During the sol‐gel transition the aggregates grow with a fractal structure and the fractal dimensionality decreases from 2.4 to 1.8. This last value is characteristic of a cluster‐cluster aggregation controlled by a diffusion process. Furthermore, the time exponent of aggregate growth presents values of 0.33 and 1, typical of diffusional and hydrodynamic motions. A crossover between these two regimes is observed.