TY - JOUR
T1 - TiO2 stability landscape
T2 - Polymorphism, surface energy, and bound water energetics
AU - Levchenko, Andrey A.
AU - Li, Guangshe
AU - Boerio-Goates, Juliana
AU - Woodfield, Brian F.
AU - Navrotsky, Alexandra
N1 - Copyright:
Copyright 2011 Elsevier B.V., All rights reserved.
PY - 2006/12/26
Y1 - 2006/12/26
N2 - The energetics of pure-phase rutile nanorods and spherical anatase nanoparticles have been studied by high-temperature drop solution calorimetry in 3Na2O-4MoO3 solvent at 975 K and water adsorption calorimetry in a wide range of particle sixes (surface area) from 6 to 40 nm (5-270 m2/g). The calorimetric surface enthalpies for rutile and anatase. calculated as 2.22 ± 0.07 and 0.74 ± 0.04 J/m 2, respectively, are in general agreement with Ranade et al.'s results (Proc. Natl. Acad, Sci. U.S.A., 2002, 99, 6476), although their numerical values are somewhat different because of impurities and unaccounted bound water in the previous work. This study supports the energy crossovers previously proposed for the TiO2 polymorphs. The energetics of water adsorption were measured using a commercial Calvet microcalorimeter coupled with a gas dosing system. This permitted the calculation of differential and integral enthalpies of water adsorption that characterize how tightly water binds to rutile and anatase surfaces and the calculation of adsorption entropies, which reflect the surface mobility of adsorbed water. The integral enthalpy of tightly bound water (relative to liquid H2O standard state) is -18 kJ/mol for anatase and -40 kJ/mol for rutile. As seen previously for Al2O2, the TiO2 polymorphs with higher surface energy bind water more tightly. The calculated entropy changes for the adsorption of water on TiO2 are more negative than the entropy changes for the condensation of gaseous water to hexagonal ice. This finding suggests highly restricted mobility of molecules adsorbed at initial stages of adsorption (low coverage) and, possibly, dissociative adsorption on both rutile and anatase surfaces. However, nanoparticles contain both tightly bound water and loosely bound water. The latter is characterized by energetics of bulk water. The stabilizing water contribution to the overall energy of the system makes the hydrated nanophase samples more stable. The recommended transformation enthalpy for bulk anatase to bulk rutile is -1.7 ± 0.9 kJ/mol.
AB - The energetics of pure-phase rutile nanorods and spherical anatase nanoparticles have been studied by high-temperature drop solution calorimetry in 3Na2O-4MoO3 solvent at 975 K and water adsorption calorimetry in a wide range of particle sixes (surface area) from 6 to 40 nm (5-270 m2/g). The calorimetric surface enthalpies for rutile and anatase. calculated as 2.22 ± 0.07 and 0.74 ± 0.04 J/m 2, respectively, are in general agreement with Ranade et al.'s results (Proc. Natl. Acad, Sci. U.S.A., 2002, 99, 6476), although their numerical values are somewhat different because of impurities and unaccounted bound water in the previous work. This study supports the energy crossovers previously proposed for the TiO2 polymorphs. The energetics of water adsorption were measured using a commercial Calvet microcalorimeter coupled with a gas dosing system. This permitted the calculation of differential and integral enthalpies of water adsorption that characterize how tightly water binds to rutile and anatase surfaces and the calculation of adsorption entropies, which reflect the surface mobility of adsorbed water. The integral enthalpy of tightly bound water (relative to liquid H2O standard state) is -18 kJ/mol for anatase and -40 kJ/mol for rutile. As seen previously for Al2O2, the TiO2 polymorphs with higher surface energy bind water more tightly. The calculated entropy changes for the adsorption of water on TiO2 are more negative than the entropy changes for the condensation of gaseous water to hexagonal ice. This finding suggests highly restricted mobility of molecules adsorbed at initial stages of adsorption (low coverage) and, possibly, dissociative adsorption on both rutile and anatase surfaces. However, nanoparticles contain both tightly bound water and loosely bound water. The latter is characterized by energetics of bulk water. The stabilizing water contribution to the overall energy of the system makes the hydrated nanophase samples more stable. The recommended transformation enthalpy for bulk anatase to bulk rutile is -1.7 ± 0.9 kJ/mol.
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U2 - 10.1021/cm061183c
DO - 10.1021/cm061183c
M3 - Article
AN - SCOPUS:33846356643
SN - 0897-4756
VL - 18
SP - 6324
EP - 6332
JO - Chemistry of Materials
JF - Chemistry of Materials
IS - 26
ER -