1. 四川大学化学工程学院,四川 成都 610065
2. 中国工程物理研究院激光聚变研究中心,四川 绵阳 621900
3. 中国核动力研究设计院核反应堆系统设计技术重点实验室,四川 成都 610041
徐兰(1994—),女,硕士研究生,18428374312@163.com
黄卫星(1958—),男,博士,教授,hwx@scu.edu.cn
刘梅芳(1981—),女,博士,副研究员,sunset640@126.com
收稿:2019-04-18,
修回:2019-09-03,
网络首发:2020-06-09,
纸质出版:2019-12-05
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徐兰, 潘大伟, 邓朝俊, 黄卫星, 刘梅芳. “一步法”微流控制备大直径复合乳粒中几何尺寸调控规律研究[J]. 化工学报, 2019, 70(12): 4617-4624
XU Lan, PAN Dawei, DENG Chaojun, HUANG Weixing, LIU Meifang. Controlled size production of large double droplets in one-step microfluidic devices[J]. CIESC Journal, 2019, 70(12): 4617-4624
徐兰, 潘大伟, 邓朝俊, 黄卫星, 刘梅芳. “一步法”微流控制备大直径复合乳粒中几何尺寸调控规律研究[J]. 化工学报, 2019, 70(12): 4617-4624 DOI: 10.11949/0438-1157.20190413.
XU Lan, PAN Dawei, DENG Chaojun, HUANG Weixing, LIU Meifang. Controlled size production of large double droplets in one-step microfluidic devices[J]. CIESC Journal, 2019, 70(12): 4617-4624 DOI: 10.11949/0438-1157.20190413.
复合乳粒几何尺寸的精密调控对于实现特定规格参数要求的聚合物空心微球的可控制备具有重要意义。基于“一步法”微流控装置,通过大量的实验获得了以油相与内水相流量比
R
和连续相毛细管数
Ca
为变量的复合乳粒构建操作区域图,并在能稳定形成复合乳粒区域范围内探讨了
Ca
、
R
以及管道尺寸对大直径复合乳粒几何尺寸的影响规律。实验结果表明:随着连续相毛细管数增大,复合乳粒几何尺寸(内径、外径和壁厚)均减小;随着油相与内水相流量比增大,复合乳粒内径减小,壁厚增大,而外径则呈现先减小后增大的趋势。此外,复合乳粒几何尺寸随管道直径增大而增大,且存在极限尺寸。实验结果可为单分散大直径复合乳粒的定量可控制备提供实验设计依据。
The precise regulation of the composite latex geometry is important for the controllable preparation of polymer hollow microspheres to achieve specific specifications. Based on one-step microfluidic device
extensive experiments for double droplet preparation are conducted and the flow pattern diagram dependent on capillary number of continuous phase
Ca
W2
and the flow rate ratio of oil phase to inner phase
R
O/W1
is obtained
and further the effects of the
Ca
R
O/W1
and the diameter of external phase tube on the large double droplets size are discussed in this work. As
Ca
W2
increases
the droplet sizes
regarding inner diameter
shell thickness and outer diameter
decrease because of a large drag force generated by a continuous phase. With the
R
O/W1
increasing
the inner diameter decreases
while the shell thickness increases. However
as for the outer diameter of such double droplet
it initially decreases and then increases. In addition
the droplet sizes increase as the tube diameter increases under the same flow rate of all three phases
but it is always limited by the tube diameter. The present work could provide some guidelines for controllable and precise fabrication of double droplets with large diameter.
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