Chinese Journal of Lasers, Volume. 52, Issue 4, 0402407(2025)
Aluminum‐Based Interfacial Evaporator for Solar Desalination Processed by Picosecond Laser
Fig. 3. Diameter and depth of point structure versus single pulse energy. (a) Diameter; (b) depth
Fig. 4. Surface microstructures of point structures under different single pulse energies
Fig. 5. Diameter and depth of point structure versus pulse number. (a) Diameter; (b) depth
Fig. 6. Surface microstructures of point structures under different pulse numbers
Fig. 7. Influence of laser process parameters on characteristic parameters of line structure. (a) Influence of single pulse energy on width and depth of line structure; (b) influence of laser scanning speed on width and depth of line structure; (c) influence of number of scans on width and depth of line structure
Fig. 8. Influence of process parameters on surface morphology of line structure. (a) Single pulse energy (v=100 mm/s, T=1);
Fig. 9. Surface morphologies of surface structures under different scanning intervals. (a) 20 μm; (b) 50 μm; (c) 80 μm; (d) 120 μm; (e) 150 μm
Fig. 10. Influence of number of scans on surface morphology of line array structure
Fig. 11. Simulated solar desalination of point array structured evaporators with different scan intervals. (a) Evaporating dish mass change; (b) evaporation rate of evaporator in certain time interval
Fig. 12. Simulated solar desalination of point array structured evaporators at different depths. (a) Evaporating dish mass change; (b) evaporation rate of evaporator in certain time interval
Fig. 13. Simulated solar desalination of line array structured evaporators with different scan intervals. (a) Evaporating dish mass change; (b) evaporation rate of evaporator in certain time interval
Fig. 14. Simulated solar desalination of line array structured evaporators at different depths. (a) Evaporating dish mass change; (b) evaporation rate of evaporator in certain time interval
Fig. 15. Simulated solar desalination of evaporators with different step widths. (a) Evaporating dish mass change; (b) evaporation rate of evaporator in certain time interval
Fig. 16. Simulated solar desalination of surface structured evaporators with different c values. (a) Evaporating dish mass change; (b) evaporation rate of evaporator in certain time interval
Fig. 17. Optical properties of stepped structured evaporator surface. (a) Reflectivity values of evaporators under different widths; (b) reflectivity values of evaporators under different c when a=b=720 μm
Fig. 18. Outdoor seawater desalination experiment and water quality testing. (a) Temperature and light intensity on day of outdoor experiment; (b) variation in outdoor mass of evaporating dish; (c) mass concentration changes of ions before and after seawater desalination
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Shuangshuang Hu, Zhiliang Tang, Weizhen Li, Dongkai Chu, Shuoshuo Qu, Peng Yao. Aluminum‐Based Interfacial Evaporator for Solar Desalination Processed by Picosecond Laser[J]. Chinese Journal of Lasers, 2025, 52(4): 0402407
Category: Laser Micro-Nano Manufacturing
Received: Jul. 18, 2024
Accepted: Sep. 19, 2024
Published Online: Jan. 20, 2025
The Author Email: Chu Dongkai (chudongkai@sdu.edu.cn), Yao Peng (yaopeng@sdu.edu.cn)
CSTR:32183.14.CJL241065