A DFT study on the interaction of small molecules with alkali metal ion-exchanged ETS-10

Abstract

In this paper, we present a systematic quantum-mechanical density functional theory (DFT) study of adsorption of small gas molecules in cation-exchanged Engelhard titanosilicate ETS-10 crystalline materials. Adsorbates with a range of polarities were considered, ranging from polar (H2O), quadrupolar (CO2 and N2), to apolar (CH4) atmospheric gases. Starting from the base-case of Na-ETS-10, other extra framework cations such as Li + , K + , Rb + and Cs + were considered. The DFT calculations were performed with the M06-L functional and were corrected for basis set superposition error with the counterpoise method in order to provide accurate and robust geometries and adsorption energies. For all adsorbates, the adsorption enthalpies decrease in the order Li + > Na + > K + > Rb + > Cs + , while adsorbate -cation interaction distances increase along the same order. For the two extreme cases, the enthalpies calculated at the M06-L/6-31++G** level of theory for CH4, N2, CO2, and H2O interaction with Li + (Cs + ) exchanged materials are -21.8 (-1.7) kJ•mol -1 , -19.0 (-10.7) kJ•mol -1 , -34.4 (-21.3) kJ•mol -1 , and -70.5 (-36.1) kJ•mol -1 , respectively. Additionally, the calculated vibrational frequencies are found to be in quite good agreement with the characteristic vibrational modes of alkali metal cation-exchanged ETS-10 and also with the available experimental frequencies for CH4, N2, CO2, and H2O interactions with alkali metal cations in the 12-membered channel of ETS-10.

Theoretical studies on carbon dioxide adsorption in cation-exchanged molecular sieves

“…44 The distances between O-Li, O-Na and O-K are 2.167, 2.515 and 2.888Å, respectively; thus, the distance between the O atom and metal cation is getting farther and farther. This is in line with the DFT study by Pillai et al that showed the adsorbate-cation distance increasing in the order of Li, Na and K. 45 Furthermore, the angle of the cation and CO 2 (M/O]C]O) is nonlinear as shown in Fig. 2, which is in good agreement with the GCMC simulations performed on the NaY system.…”