Attenuated Natural Convection in Molten Salt Electrochemical Systems with Minimal Heat Dissipation
Source abstract
Abstract
The accurate understanding of mass transfer in molten salt contributes to revealing the reaction mechanism and advancing the technologies. The existence of notable natural convection effects has been demonstrated in our previous studies, even though the driving forces for such a high natural convection are still not clear. Herein, we showed that the intense natural convection in molten salts resulted from severe heat dissipation through the electrodes (or the system). With an adiabatic design, natural convection effects were significantly suppressed in molten LiCl–KCl. The derived value of the natural convection layer (δ conv ) ranged from 190 to 250 μm in molten LiCl–KCl containing a redox couple (e.g., SmCl 3, EuCl 3, and CrCl 3 ), comparable to those in aqueous solutions. The values of δ conv in LiCl–KCl–173 mM CrCl 3 increased to ∼360 μm due to the change in salt viscosity. The density-driven convection became dominant under a high redox concentration, and the increasing working temperature had no apparent effect on the natural convection effects because of the adiabatic design.
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Research context
OpenAlex topics: Molten salt chemistry and electrochemical processes · Metallurgical Processes and Thermodynamics · Advancements in Solid Oxide Fuel Cells
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
State Key Laboratory of Advanced Metallurgy, University of Science and Technology Beijing, Beijing 100083, People’s Republic of China
State Key Laboratory of Advanced Processing and Recycling of Non-ferrous Metal, Lanzhou University of Technology, Lanzhou, Gansu 730050, People’s Republic of China
Funding
National Natural Science Foundation of China · China Baowu Low Carbon Metallurgy Innovation Foundation
References (18)
Show source-provided references
1. 10.1038/s41586-022-04748-410.1038/s41586-022-04748-4 ↗
2. 10.1038/s41467-021-26119-910.1038/s41467-021-26119-9 ↗
3. 10.1002/anie.20190599110.1002/anie.201905991 ↗
4. 10.1038/s41467-019-13065-w10.1038/s41467-019-13065-w ↗
5. 10.1021/acs.jpcb.3c0393810.1021/acs.jpcb.3c03938 ↗
6. 10.1016/S0022-0728(98)00431-810.1016/S0022-0728(98)00431-8 ↗
7. 10.1016/0022-0728(93)80180-P10.1016/0022-0728(93)80180-P ↗
8. 10.1016/j.coelec.2017.09.01010.1016/j.coelec.2017.09.010 ↗
9. 10.1021/acs.analchem.5b0129310.1021/acs.analchem.5b01293 ↗
10. 10.1016/j.elecom.2023.10757610.1016/j.elecom.2023.107576 ↗
11. 10.1016/j.jelechem.2023.11786510.1016/j.jelechem.2023.117865 ↗
12. 10.1016/j.jelechem.2023.11795010.1016/j.jelechem.2023.117950 ↗
13. 10.1021/je010092n10.1021/je010092n ↗
14. 10.1016/S0167-7322(02)00063-610.1016/S0167-7322(02)00063-6 ↗
15. 10.1016/j.jnucmat.2010.12.00410.1016/j.jnucmat.2010.12.004 ↗
16. 10.1149/1945-7111/ac436a10.1149/1945-7111/ac436a ↗
17. 10.1021/acs.jpcb.1c0374810.1021/acs.jpcb.1c03748 ↗
18. 10.1016/j.elecom.2024.10780810.1016/j.elecom.2024.107808 ↗