CIESC Journal ›› 2024, Vol. 75 ›› Issue (11): 4095-4119.DOI: 10.11949/0438-1157.20240598
• Reviews and monographs • Previous Articles Next Articles
Zhengya DONG1,2,3(), Xiaojing ZHU1,3, Jingfu JIA1,3, Jie ZHANG1,3, Zhuotao ZHENG1,3, Xiaolin LIU3, Zhilin WU1,2
Received:
2024-05-31
Revised:
2024-07-29
Online:
2024-12-26
Published:
2024-11-25
Contact:
Zhengya DONG
董正亚1,2,3(), 朱晓晶1,3, 贾竞夫1,3, 张杰1,3, 郑卓韬1,3, 刘晓霖3, 武志林1,2
通讯作者:
董正亚
作者简介:
董正亚(1987—),男,博士,教授,zhydong@stu.edu.cn
基金资助:
CLC Number:
Zhengya DONG, Xiaojing ZHU, Jingfu JIA, Jie ZHANG, Zhuotao ZHENG, Xiaolin LIU, Zhilin WU. Scale-up of ultrasonic microreactor systems and their applications in the preparation of nanomaterials[J]. CIESC Journal, 2024, 75(11): 4095-4119.
董正亚, 朱晓晶, 贾竞夫, 张杰, 郑卓韬, 刘晓霖, 武志林. 超声微反应器系统的放大及其在纳米材料制备中的应用[J]. 化工学报, 2024, 75(11): 4095-4119.
Fig.2 (a) Schematic diagram of the structure of the sandwich piezoelectric ceramic ultrasonic transducer; (b) Physical diagram of the ultrasonic transducer of various structures[27]
Fig.4 (a) Schematic of the ultrasonic cavitation-based micromixer design; (b) Geometric information of the glass capillary-based microchannel; (c) Schematic of the ultrasonic setup using co-flow and impinge flow microchannel
Fig.6 (a) Vibration system consisting of a capillary microreactor; (b) Vibration system consisting of a cylindrical luffing rod and a sandwich transducer
Fig.7 (a) Acoustic cavitation under ultrasound[41]; Cavitation behavior of free bubbles at the microscale: (b) vibrational behavior,(c) confinement effect[38]; (d) Acoustic flow from vibration[42]; Two important cavitation bubble oscillation phenomena observed in ultrasonic microreactor: (e) bubble arrays (or bubble cluster arrays) in straight channels and (f) strongly oscillating bubble clouds in curved channels[43]
Fig.8 (a) The number of cavitation bubbles and mixing behavior under different solvent systems[22]; The effect of ultrasonic power on cavitation bubble formation rate (b) and mixing performance under different solvent systems (c); (d) Cavitation behavior and bubble distribution in the ultrasonic reactor with different channel sizes[57]; (e) Mixing time as a function of ultrasonic power for 0.5—2.0 mm channel sizes[22]
Fig.9 Typical cavitation modes: (a) cavitation modes at different channel sizes and frequencies: array mode, elastic cluster mode and cluster mode; (b) Under different ultrasonic powers and flows: cavitation modes and microscopic cavitation behaviors; (c) Cavitation modes under different relative positions of coaxial casings and channels: bubble tailing, satellite, surround and cluster; (d) Cavitation pattern diagram in the ultrasonic microreactor[57]
Fig.11 Schematic diagram of the reaction nucleation growth process in the microchannel: (a) Nucleation growth in diffusion mixed mode; (b) Nucleation growth in ultrasound-enhanced mass transfer mode
Fig.12 Scanning electron microscopy of silica microspheres: (a) An average particle size of 155 nm and a CV value of 6.77%; (b) An average particle size of 300 nm and a CV value of 4.33%; (c) An average particle size of 409 nm and a CV value of 6.90%; (d) An average particle size of 550 nm and a CV value of 5.87%; (e) An average particle size of 730 nm and a CV value of 4.17%; (f) An average particle size of 840 nm and a CV value of 4.05%
Fig.15 (a) Schematic illustration of USMR approach for synthesis biomedical organic NPs; (b) Size distribution and (c) mRNA encapsulation efficiency of mRNA-LNPs synthesized by different approaches; (d) Cryo-TEM micrographs of mRNA-LNP synthesized via this approach[22]
Fig.16 (a) Preparation of liposomes by USMR with different flow patterns; (b),(c) Effect of ultrasonic power on DS and PDI of liposomes prepared with USMR-IF; (d) Comparison of liposomes prepared by different methods; (e) Cryo-TEM image of liposomes prepared with USMR-IF under the optimal condition[25]
Fig.17 Emulsification observed in ultrasonic microreactor: (a) bubble shuttle emulsification[110], (b) two-phase emulsification[41],(c) bubble oscillation-induced interface deformation and emulsification, (d) shockwave-induced emulsification[112]; (e) Effect of different cavitation behaviors on emulsion size distribution[114]
Fig.18 The influence of the main factors on the particle size and PDI of the emulsions: (a) the ratio of aqueous phase to soybean oil, (b) the residence time of the feedstocks, (c) ultrasonic power; (d) Photographs of emulsion samples[26]
USMR | Residence time/min | Ultrasonic power/W | Total flow rate/(ml/min) | DS/nm | PDI |
---|---|---|---|---|---|
umFlow-D×1 | 1 | 40 | 0.66 | 119.8 | 0.211 |
![]() | 1 | 40 | 1.32 | 121.3 | 0.239 |
![]() | 1 | 40 | 2.64 | 119.7 | 0.225 |
![]() | 0.7 | 160 | 20 | 120.5 | 0.219 |
Table 1 DS and PDI of nanoemulsions prepared with different USMR(A∶O ratio:9∶1)[26]
USMR | Residence time/min | Ultrasonic power/W | Total flow rate/(ml/min) | DS/nm | PDI |
---|---|---|---|---|---|
umFlow-D×1 | 1 | 40 | 0.66 | 119.8 | 0.211 |
![]() | 1 | 40 | 1.32 | 121.3 | 0.239 |
![]() | 1 | 40 | 2.64 | 119.7 | 0.225 |
![]() | 0.7 | 160 | 20 | 120.5 | 0.219 |
Fig.19 Photographs of magnetic polymer nanosphere: (a) photographs of scanning electron microscope; (b) photographs of transmission electron microscope and EDS
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