Steady‐State, Scalable Production of Mesoporous Rutile and Brookite Particles and Their Use in Energy Conversion and Storage Cells
Source abstract
Abstract
Abstract Mesoporous TiO2 rutile particles with a cauliflower‐like morphology and an internal structure of self‐assembled nanoneedles were synthesized in a novel TiIV chloride aqueous‐solution hydrolysis process. In an effort to make nanostructured rutile synthesis cost‐effective and green, the process was conducted at steady‐state in a continuously stirred tank reactor (CSTR) below 100 °C. High TiCl4 concentration 0.5–1 m yielded rutile, while lowering the concentration to 0.1 m led to the crystallization of brookite nanoplatelets. Apart from phase control, specific surface area of rutile may be tuned via TiCl4 concentration regulation from 85 to 500 m2 g−1. Investigation revealed that low pH/high TiIV concentration conditions favored direct nucleation of rutile nuclei during steady state that grow radially outward into nanoneedle structured cauliflower particles with nanoscale edgy surface. The unique steady‐state produced mesoporous rutile particles were shown to have excellent light scattering properties in a bi‐layer photoanode structure resulting in 42.5 % increase in photovoltaic efficiency. Brookite nanoplatelets were shown, in addition to their scattering properties, to exhibit stable Li‐ion intercalation functionality.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: TiO2 Photocatalysis and Solar Cells · Advanced Photocatalysis Techniques · Iron oxide chemistry and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Materials Engineering McGill University 3610 University Street, M.H. Wong Building Montréal Canada
Funding
Strategic Projects Program of Canada's Natural Sciences & Engineering Research Council
References (41)
Show source-provided references
1. 10.1088/0953-8984/24/19/19550310.1088/0953-8984/24/19/195503 ↗
2. 10.1021/ie300510n10.1021/ie300510n ↗
3. 10.1016/j.mattod.2015.02.01510.1016/j.mattod.2015.02.015 ↗
4. 10.1557/jmr.2015.15010.1557/jmr.2015.150 ↗
5. 10.1039/c2ce26691a10.1039/c2ce26691a ↗
6. 10.1039/c3nr04462a10.1039/c3nr04462a ↗
7. 10.1016/j.snb.2014.08.09210.1016/j.snb.2014.08.092 ↗
8. 10.1016/S0040-6090(02)01105-710.1016/S0040-6090(02)01105-7 ↗
9. 10.1149/1.352923810.1149/1.3529238 ↗
10. 10.1557/jmr.2012.22610.1557/jmr.2012.226 ↗
11. 10.1016/j.matlet.2005.10.11410.1016/j.matlet.2005.10.114 ↗
12. 10.1016/j.msea.2007.02.09210.1016/j.msea.2007.02.092 ↗
13. 10.1021/cm902613h10.1021/cm902613h ↗
14. 10.1016/j.matchemphys.2008.04.01510.1016/j.matchemphys.2008.04.015 ↗
15. 10.1021/cg400858p10.1021/cg400858p ↗
16. 10.1039/b514632a10.1039/b514632a ↗
17. 10.1021/jp000499j10.1021/jp000499j ↗
18. 10.1016/j.hydromet.2008.10.00410.1016/j.hydromet.2008.10.004 ↗
19. 10.1016/j.cej.2015.11.04510.1016/j.cej.2015.11.045 ↗
20. 10.1039/b100435m10.1039/b100435m ↗
21. 10.1016/j.jcrysgro.2009.09.03310.1016/j.jcrysgro.2009.09.033 ↗
22. 10.1039/b009203g10.1039/b009203g ↗
23. 10.1088/0957-4484/19/14/14560510.1088/0957-4484/19/14/145605 ↗
24. 10.1016/S0277-5387(00)84215-110.1016/S0277-5387(00)84215-1 ↗
25. 10.1039/b001718n10.1039/b001718n ↗
26. 10.1021/cg301230w10.1021/cg301230w ↗
27. 10.1039/c0cc01394c10.1039/c0cc01394c ↗
28. 10.2109/jcersj2.117.81910.2109/jcersj2.117.819 ↗
29. 10.1016/S0040-6090(03)00539-X10.1016/S0040-6090(03)00539-X ↗
30. 10.1039/c0nr00561d10.1039/c0nr00561d ↗
31. 10.4067/S0717-9707201100030001610.4067/S0717-97072011000300016 ↗
32. 10.1016/j.electacta.2012.11.09110.1016/j.electacta.2012.11.091 ↗
33. 10.1016/j.jpowsour.2014.02.09210.1016/j.jpowsour.2014.02.092 ↗
34. 10.1002/cssc.20130113910.1002/cssc.201301139 ↗
35. 10.1557/jmr.2012.35910.1557/jmr.2012.359 ↗
36. 10.1016/j.electacta.2012.02.02810.1016/j.electacta.2012.02.028 ↗
37. 10.1039/C4RA01308E10.1039/C4RA01308E ↗
38. 10.1016/j.electacta.2008.09.02510.1016/j.electacta.2008.09.025 ↗
39. 10.1039/C4RA03723E10.1039/C4RA03723E ↗
40. 10.1016/j.electacta.2014.05.14810.1016/j.electacta.2014.05.148 ↗
41. 10.1002/pip.76810.1002/pip.768 ↗