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Model structures of molten salt-promoted MgO to probe the mechanism of MgCO3 formation during CO2 capture at a solid-liquid interface.
Bork, Alexander H; Ackerl, Norbert; Reuteler, Joakim; Jog, Sachin; Gut, David; Zboray, Robert; Müller, Christoph R.
Affiliation
  • Bork AH; Laboratory of Energy Science and Engineering, Department of Mechanical and Process Engineering, ETH Zurich CH-8092 Zürich Switzerland muelchri@ethz.ch.
  • Ackerl N; Laboratory of Energy Science and Engineering, Department of Mechanical and Process Engineering, ETH Zurich CH-8092 Zürich Switzerland muelchri@ethz.ch.
  • Reuteler J; NAPho - Norbert Ackerl Photonics CH-8049 Zürich Switzerland.
  • Jog S; Scientific Center for Optical and Electron Microscopy, ETH Zurich CH-8093 Zurich Switzerland.
  • Gut D; Laboratory of Energy Science and Engineering, Department of Mechanical and Process Engineering, ETH Zurich CH-8092 Zürich Switzerland muelchri@ethz.ch.
  • Zboray R; Laboratory of Energy Science and Engineering, Department of Mechanical and Process Engineering, ETH Zurich CH-8092 Zürich Switzerland muelchri@ethz.ch.
  • Müller CR; Center for X-ray Analytics, Empa, Swiss Federal Laboratories for Materials Science and Technology CH-8600 Dübendorf Switzerland.
J Mater Chem A Mater ; 10(32): 16803-16812, 2022 Aug 17.
Article in En | MEDLINE | ID: mdl-36092378
ABSTRACT
MgO is a promising solid oxide-based sorbent to capture anthropogenic CO2 emissions due to its high theoretical gravimetric CO2 uptake and its abundance. When MgO is coated with alkali metal salts such as LiNO3, NaNO3, KNO3, or their mixtures, the kinetics of the CO2 uptake reaction is significantly faster resulting in a 15 times higher CO2 uptake compared to bare MgO. However, the underlying mechanism that leads to this dramatic increase in the carbonation rate is still unclear. This study aims to determine the most favourable location for the nucleation and growth of MgCO3 and more specifically, whether the carbonation occurs preferentially at the buried interface, the triple phase boundary (TPB), and/or inside the molten salt of the NaNO3-MgO system. For this purpose, a model system consisting of a MgO single crystal that is structured by ultra-short pulse laser ablation and coated with NaNO3 as the promoter is used. To identify the location of nucleation and growth of MgCO3, micro X-ray computed tomography, scanning electron microscopy, Raman microspectroscopy and optical profilometry were applied. We found that MgCO3 forms at the NaNO3/MgO interface and not inside the melt. Moreover, there was no preferential nucleation of MgCO3 at the TPB when compared to the buried interface. Furthermore, it is found that there is no observable CO2 diffusion limitation in the nucleation step. However, it was observed that CO2 diffusion limits MgCO3 crystal growth, i.e. the growth rate of MgCO3 is approximately an order of magnitude faster in shallow grooves compared to that in deep grooves.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: J Mater Chem A Mater Year: 2022 Document type: Article

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: J Mater Chem A Mater Year: 2022 Document type: Article