基于微流控液滴形成技术的聚乙烯醇微球制备

建立了一种新的基于微流控液滴形成技术的聚乙烯醇(Poly(vinyl alcohol),PVA)微球制备方法。在微流控芯片上利用液滴形成技术可以快速、连续产生尺度均一、单分散性好的PVA液滴。液滴制备速度可以达到7个/s。并且通过改变制备液中两相流体的注入流量和微流控通道宽度可对生成的PVA液滴的尺寸进行调节。将收集得到的PVA液滴进行物理交联固化处理,可以获得大量尺寸均一的聚乙烯醇微球。本方法制备效率高,所得到的微球单分散效果好,而且微球形成不需要化学交联剂的掺入,避免了对包载物质的干扰,非常适合药物载体等应用。     

微液滴微流控芯片:微液滴的形成、操纵和应用

微流控芯片中形成的微液滴粒径均一、可控,与传统的连续流体系相比,具有能实现试剂的快速混合、通量更高等优点.本文介绍了微流控芯片中由微通道控制的微液滴的形成、分裂、合并、混合、分选和捕获等微液滴操纵技术,以及微液滴技术在纳米粒子、聚合物微粒的合成、纳米粒子自组装、蛋白质结晶研究和DNA、细胞分析等领域的研究进展.     

基于微流体脉冲驱动控制技术的电化学微流控芯片制备方法

基于微流体脉冲驱动控制技术搭建了电化学微流控芯片的制备系统.首先将纳米银墨水和甘油溶液分别微喷射到玻璃基底表面形成微电极图形和微流道液体阳模图形;然后分别进行烧结和聚二甲基硅氧烷(PDMS)模塑工艺制得微电极和微流道;最后将微电极和微流道键合形成电化学微流控芯片.研究了系统参量对液滴产生的影响以及液滴直径和重叠率对液滴成线的影响,制得的微电极最小线宽为45 μm、厚度为2.2 μm、电阻率为5.2 μΩ·cm,制得的微流道最小线宽为35 μm,流道表面光滑.采用制得的电化学微流控芯片进行了葡萄糖浓度的电化学流动检测.结果表明,葡萄糖溶液的浓度与响应电流具有较高的线性关系,可对一定浓度范围内的葡萄糖溶液进行定量检测.基于微流体脉冲驱动控制技术的电化学微流控芯片制备方法具有微喷射精度高、重复性好,制备系统结构简单、成本低廉等优点,可用于生化分析、生物传感器等领域的芯片制备.     

DOPC/DPPC单层膜中分子间的相互作用及形态特征

利用Langmuir-Blodgett(LB)技术制备了不同表面压力下的1,2-二油酸-甘油-3-磷脂酰胆碱(DOPC)/1,2-二棕榈酸甘油-3-磷脂酰胆碱(DPPC)(摩尔比为1:1)和DOPC/DPPC/Chol(摩尔比为2:2:1)单层膜, 对单层膜内分子间的相互作用进行了热力学分析, 并用荧光显微镜和原子力显微镜对其形态进行了观测.热力学分析表明, DOPC与DPPC分子在单层膜结构中相互作用为排斥力, 诱导单层膜出现相变; DOPC, DPPC与胆固醇(Chol)间的相互作用均为吸引力, 当表面压力(π)大于18 mN/m时, DPPC与胆固醇的作用力大于DOPC.荧光显微镜观测表明, DOPC/DPPC单层膜出现明显相分离现象, 富含DPPC微区成“花形”结构, 且随着表面压力的升高微区逐渐增大, “花瓣”增多; 当胆固醇加入到DOPC/DPPC体系时, 单层膜相态由液相与凝胶相共存转变为液态无序相与液态有序相共存结构, 富含DPPC的微区形状从“花形”转变成“圆形”.原子力显微镜对单层膜的表征验证了荧光显微镜的观测结果, 表明胆固醇加入到DOPC/DPPC体系中对单层膜排列具有明显的影响, 压力和溶液状态等是影响脂膜结构的重要因素.     

胶体晶体微球及其生物医学应用

光子晶体(PhCs)是由单分散纳米粒子周期性排列形成的材料,具有光子禁带,频率落在光子禁带内的光被禁止传播,这个特性激起了研究者对其制备和应用的研究热情。然而,一般的光子晶体材料都具有角度有偏性质,限制了其在宽视角光学材料和设备上的应用。近几年有一系列围绕球形胶体光子晶体材料的研究成果问世,由于球形的对称性,球形胶体晶体的衍射峰不会随着光的入射角变化而发生变化,从而拓宽了胶体晶体的应用范围。随着微流控技术被用于制备液滴模板,球形胶体晶体的制备取得了巨大的进步。微流控技术不仅保证了液滴模板的单分散性,还增加了胶体晶体微球的结构与功能的多样性。胶体晶体微球这些特有的性质,可以很好地将光子晶体材料与编码、非标记检测、细胞培养以及载药等生物医学领域连接起来,为其应用提供了广阔的前景。本文总结了球形光子晶体的研究进展,包括球形光子晶体的设计、制备及其生物医学应用,最后,对球形光子晶体未来的发展方向作了展望。     

微流控芯片液滴生成与检测技术研究进展

微流控芯片液滴技术是一种操控微小体积液体的新技术,既可实现高通量微观样本的生成及控制,也可进行独立液滴的操作。分散的微液滴单元可作为理想的微反应器,在生物医药中的药物筛选、材料筛选和高附加值微颗粒材料合成领域展现出巨大的应用潜力。液滴微流控芯片是利用流体剪切力的改变,使互不相溶的两相流体在其界面处生成稳定、有序的液滴,目前微液滴的生成方法主要有水动力法、气动法、光控法和电动法等。基于液滴的微流控系统越来越多地被应用于执行复杂的多重反应、测量和分析,可以进行超小体积和超高吞吐量的化学和生物实验。对液滴微流控系统而言,液滴的速度、大小和内容物含量会影响最终的检验结果,因此对液滴形成速率和液滴的内容物含量的实时检测至关重要,目前最常用的液滴检测方法有光学检测技术与电学传感检测技术。对两相流液滴生成机理以及现有液滴生成技术开展了讨论分析,同时对液滴检测技术进行了评述。     

微流控液滴软模板制备二氧化钛中空微球

应用微流控液滴技术合成功能材料已发展成为一个新兴领域。本文以夹流结构微流控芯片产生的微液滴作为软模板,以液滴模板界面处发生的水解反应生成二氧化钛球壳,并经后续脱核处理,制备二氧化钛中空微球。采用激光诱导荧光成像、扫描电镜等手段对微球形貌结构进行了分析表征。结果表明,通过控制微流控芯片液滴合成条件,可以得到壁厚约2 μm的二氧化钛中空微球。这种以微流控液滴为模板的合成方法简单灵活,若与其他材料改性方法相结合,有望实现对更多元、更复杂功能微球材料的制备,并进一步拓宽其在光电和催化剂材料领域的应用。     

多相微流控分析与毛细管电泳研究进展

简要介绍了近期在多相微流控分析和毛细管电泳领域的一些最新研究进展,包括实现高分辨纳流液相色谱-质谱分析的微流控液滴阵列技术,采用高灵敏生物传感检测的微流控液滴单细胞膜蛋白分析技术,以及用于毛细管电泳系统的通道表面改性技术及其相关应用。     

微流控液滴技术及其应用的研究进展

微液滴具有体积小、比表面积大,速度快、通量高,大小均匀、体系封闭,内部稳定等特性,在药物控释、病毒检测、颗粒材料合成、催化剂等领域中均有重要应用.微流控技术的发展为微液滴生成中实现尺寸规格、结构形貌和功能特性等的可控设计和精确操控提供了全新平台.本文概述了微流控液滴技术的基本原理、液滴生成方式及其基本操控,比较分析了微液滴的传统制备法与微流控合成法的异同,介绍了近年来微流控液滴技术在功能材料合成、生物医学和食品加工等领域中的研究新进展,探讨并展望了微流控液滴技术的潜在价值和未来发展方向.     

受限于两平行板间的对称星形共聚物Am Bm熔体相行为的格子自洽场理论研究

采用格子自洽场理论计算研究了受限于2个平行板间的对称星形共聚物AmBm(m=1,2,3,4,5)熔体形成的层状相结构.在给定的相互作用下(χNAB不变,χ为Flory-Huggins相互作用参数,NAB=(N?1)/m为单个聚合物分子中一对AB臂的总链节数目),针对平行板间距为体相周期的情况,系统考察了共聚物链长N和单个聚合物分子中A(或B)臂数目m对受限层结构细节及层取向的影响.由计算结果,当N或NAB不变时,受限层的归一化界面宽度随m的增大而减小.受限板为中性时,垂直层结构的单链自由能比平行层结构的低.随着板对共聚物中一种嵌段的选择作用Λ的增大,体系发生垂直层到平行层的转变,该转变为一阶相变.当m不变时,N越小,上述转变出现在越大的Λ值处,体系越容易保持垂直层结构.并且N越小,层状结构周期越小.当N或NAB不变时,m越大体系越容易保持垂直层结构.总之,星形共聚物的链长越短、臂数越多时,垂直层稳定的Λ区间越大、层状结构的界面宽度越小.这些结论可以指导刻蚀应用中对体系参数的选择.     

Deformation and breakup of micro- and nanoparticle stabilized droplets in microfluidic extensional flows

Using a microfluidic flow-focusing device, monodisperse water droplets in oil were generated and their interface populated by either 1 μm or 500 nm amine modified silica particles suspended in the water phase. The deformation and breakup of these Pickering droplets were studied in both pure extensional flow and combined extensional and shear flow at various capillary numbers using a microfluidic hyperbolic contraction. The shear resulted from droplet confinement and increased with droplet size and position along the hyperbolic contraction. Droplet deformation was found to increase with increasing confinement and capillary number. At low confinements and low capillary numbers, the droplet deformation followed the predictions of theory. For fully confined droplets, where the interface was populated by 1 μm silica particles, the droplet deformation increased precipitously and two tails were observed to form at the rear of the droplet. These tails were similar to those seen for surfactant covered droplets. At a critical capillary number, daughter droplets were observed to stream from these tails. Due to the elasticity of the particle-laden interface, these drops did not return to a spherical shape, but were observed to buckle. Although increases in droplet deformation were observed, no tail streaming occurred for the 500 nm silica particle covered droplets over the range of capillary numbers studied.     

Design of microfluidic channel geometries for the control of droplet volume, chemical concentration, and sorting

Passive microfluidic channel geometries for control of droplet fission, fusion and sorting are designed, fabricated, and tested. In droplet fission, the inlet width of the bifurcating junction is used to control the range of breakable droplet sizes and the relative resistances of the daughter channels were used to control the volume of the daughter droplets. Droplet fission is shown to produce concentration differences in the daughter droplets generated from a primary drop with an incompletely mixed chemical gradient, and for droplets in each of the bifurcated channels, droplets were found to be monodispersed with a less than 2% variation in size. Droplet fusion is demonstrated using a flow rectifying design that can fuse multiple droplets of same or different sizes generated at various frequencies. Droplet sorting is achieved using a bifurcating flow design that allows droplets to be separated base on their sizes by controlling the widths of the daughter channels. Using this sorting design, submicron satellite droplets are separated from the larger droplets.     

Microfluidic droplet sorting with a high frequency ultrasound beam

This paper presents experimental results demonstrating the feasibility of high frequency ultrasonic sensing and sorting for screening single oleic acid (lipid or oil) droplets under continuous flow in a microfluidic channel. In these experiments, hydrodynamically focused lipid droplets of two different diameters (50 μm and 100 μm) are centered along the middle of the channel, which is filled with deionized (DI) water. A 30 MHz lithium niobate (LiNbO(3)) transducer, placed outside the channel, first transmits short sensing pulses to non-invasively determine the acoustic scattering properties of the individual droplets passing through the beam's focus. Integrated backscatter (IB) coefficients, utilized as a sorting criterion, are measured by analyzing the received echo signals from each droplet. When the IB values corresponding to 100 μm droplets are obtained, a custom-built LabVIEW panel commands the transducer to emit sinusoidal burst signals to commence the sorting operation. The number of droplets tested for the sorting is 139 for 50 μm droplets and 95 for 100 μm droplets. The sensing efficiencies are estimated to be 98.6% and 99.0%, respectively. The sorting is carried out by applying acoustic radiation forces to 100 μm droplets to direct them towards the upper sheath flow, thus separating them from the centered droplet flow. The sorting efficiencies are 99.3% for 50 μm droplets and 85.3% for 100 μm droplets. The results suggest that this proposed technique has the potential to be further developed into a cost-effective and efficient cell/microparticle sorting instrument.     

Microfluidic Formation of Membrane‐Free Aqueous Coacervate Droplets in Water

We report on the formation of coacervate droplets from poly(diallyldimethylammonium chloride) with either adenosine triphosphate or carboxymethyl‐dextran using a microfluidic flow‐focusing system. The formed droplets exhibit improved stability and narrower size distributions for both coacervate compositions when compared to the conventional vortex dispersion techniques. We also demonstrate the use of two parallel flow‐focusing channels for the simultaneous formation and co‐location of two distinct populations of coacervate droplets containing different DNA oligonucleotides, and that the populations can coexist in close proximity up to 48 h without detectable exchange of genetic information. Our results show that the observed improvements in droplet stability and size distribution may be scaled with ease. In addition, the ability to encapsulate different materials into coacervate droplets using a microfluidic channel structure allows for their use as cell‐mimicking compartments.     

Preparation of Poly(vinyl alcohol) Microspheres Based on Droplet Microfluidic Technology

A new method for preparing poly (vinyl alcohol) (PVA) microspheres was developed by using droplet microfluidic technology. In the microfluidic chip, a large number of uniform, monodispersed PVA droplets were prepared quickly and continuously by using droplet formation technology, and the droplet preparation speed reached 7 per second. The size of the PVA droplets could be controlled by changing the injection flow rate of the two-phase fluid and the width of microfluidic channel. Then the PVA microspheres were formed by physical crosslinking. This method has high preparation efficiency and good monodispersity of the obtained microspheres. Moreover, the process does not require the incorporation of chemical crosslinking agents, avoiding interference with the inclusion material, and is well suited for applications such as drug carrier.     

Digital droplet immunoassay based on a microfluidic chip with magnetic beads for the detection of prostate-specific antigen

Sensitive biomarker detection techniques are beneficial for both disease diagnosis and postoperative examinations. In this study, we report an integrated microfluidic chip designed for the immunodetection of prostate-specific antigens (PSAs). The microfluidic chip is based on the three-dimensional structure of quartz capillaries. The outlet channel extends to 1.8 cm, effectively facilitating the generation of uniform droplets ranging in size from 3 to 50 μm. Furthermore, we successfully immobilized the captured antibodies onto the surface of magnetic beads using an activator, and we constructed an immunosandwich complex by employing biotinylated antibodies. A key feature of this microfluidic chip is its integration of microfluidic droplet technology advantages, such as high-throughput parallelism, enzymatic signal amplification, and small droplet size. This integration results in an exceptionally sensitive PSA detection capability, with the detection limit reduced to 7.00 ± 0.62 pg/mL.     

Investigating the effects of precursor concentration and gelling parameters on droplet-based generation of Ca-Alginate microgels: identifying new stable modes of droplet formation

Droplet-based microfluidics is an attractive approach for producing microgels due to its high potential to control the size and shape of the particles and precisely entrap the substances within the hydrogel matrix. However, the microfluidic generation of monodisperse microgels with desired structures is still challenging. Indeed, the rheological and interfacial properties of the immiscible fluids, as well as the adopted gelling strategy, play important roles in microfluidic methods. Herein, sodium alginate droplets with different concentrations are generated via a microfluidic device with a flow-focusing unit. Besides, a combined in situ and ex situ strategy is optimized to crosslink sodium alginate droplets in the presence of calcium ions. The effects of alginate concentration and junction width in the flow focusing unit are investigated on droplet size and droplet formation regimes. It is observed that by increasing the alginate concentration, the dripping regime of droplet formation may be transformed to one of the binary dripping or quasijetting regimes. In the binary dripping regime, two successive different-sized droplets are generated in each period of droplet formation, which leads to low monodispersity in the collected droplets. However, the droplets produced in the quasijetting regime are interestingly monodisperse and also smaller than those of the dripping and binary dripping regimes. The breakup dynamics of the alginate thread is also analyzed with a computational fluid dynamics (CFD) code. This analysis discloses that the viscous stresses, as well as the viscous dissipation, have important roles in controlling the stable modes of droplet formation.     

Generation of core-shell microcapsules with three-dimensional focusing device for efficient formation of cell spheroid

We present a microfluidic device generating three-dimensional (3D) coaxial flow by the addition of a simple hillock to produce an alginate core-shell microcapsule for the efficient formation of a cell spheroid. A hillock tapered at downstream of the two-dimensional focusing channel enables outside flow to enclose the core flow. The aqueous solution in the core flow was focused and surrounded by 1.8% alginate solution to be solidified as a shell. The double-layered coaxial flow (aqueous phase) was broken up into a droplet by the shear flow of oleic acid (oil phase) containing calcium chloride for the polymerization of the alginate shell. The droplet generated from the laminar coaxial flow maintained a double-layer structure and gelation of the alginate solution made a core-shell microcapsule. The shell-thickness of the microcapsule was adjusted from 8-21 μm by the variation of two aqueous flow rates. The inner shape of the shell was almost spherical when the ratio of the water-glycol mixture in the core flow exceeded 20%. The microcapsule was used to form a spheroid of embryonic carcinoma cells (embryoid body; EB) by injecting a cell suspension into the core flow. The cells inside the microcapsule aggregated into an EB within 2 days and the EB formation rate was more than 80% with strong compaction. The microcapsule formed single spherical EBs without small satellite clusters or a bumpy shape as observed in solid microbeads. The microfluidic chip for encapsulation of cells could generate a number of EBs with high rate of EB formation when compared with the conventional hanging drop method. The core-shell microcapsule generated by 3D focusing in the microchannel was effective in forming large number of spherical cell clusters and the encapsulation of cells in the microcapsule is expected to be useful in the transplantation of islet cells or cancer stem cell enrichment.     

Optimisation of a microfluidic analysis chamber for the placement of microelectrodes

The behaviour of droplets entering a microfluidic chamber designed to house microelectrode detectors for real time analysis of clinical microdialysate is described. We have designed an analysis chamber to collect the droplets produced by multiphase flows of oil and artificial cerebral spinal fluid. The coalescence chamber creates a constant aqueous environment ideal for the placement of microelectrodes avoiding the contamination of the microelectrode surface by oil. A stream of alternating light and dark coloured droplets were filmed as they passed through the chamber using a high speed camera. Image analysis of these videos shows the colour change evolution at each point along the chamber length. The flow in the chamber was simulated using the general solution for Poiseuille flow in a rectangular chamber. It is shown that on the centre line the velocity profile is very close to parabolic, and an expression is presented for the ratio between this centre line velocity and the mean flow velocity as a function of channel aspect ratio. If this aspect ratio of width/height is 2, the ratio of flow velocities closely matches that of Poiseuille flow in a circular tube, with implications for connections between microfluidic channels and connection tubing. The droplets are well mixed as the surface tension at the interface with the oil dominates the viscous forces. However once the droplet coalesces with the solution held in the chamber, the no-slip condition at the walls allows Poiseuille flow to take over. The meniscus at the back of the droplet continues to mix the droplet and acts as a piston until the meniscus stops moving. We have found that the no-slip conditions at the walls of the chamber, create a banding effect which records the history of previous drops. The optimal position for sensors is to be placed at the plane of droplet coalescence ideally at the centre of the channel, where there is an abrupt concentration change leading to a response time ?16 ms, the compressed frame rate of the video. Further away from this point the response time and sensitivity decrease due to convective dispersion.     

Formation of droplets and bubbles in a microfluidic T-junction-scaling and mechanism of break-up

This article describes the process of formation of droplets and bubbles in microfluidic T-junction geometries. At low capillary numbers break-up is not dominated by shear stresses: experimental results support the assertion that the dominant contribution to the dynamics of break-up arises from the pressure drop across the emerging droplet or bubble. This pressure drop results from the high resistance to flow of the continuous (carrier) fluid in the thin films that separate the droplet from the walls of the microchannel when the droplet fills almost the entire cross-section of the channel. A simple scaling relation, based on this assertion, predicts the size of droplets and bubbles produced in the T-junctions over a range of rates of flow of the two immiscible phases, the viscosity of the continuous phase, the interfacial tension, and the geometrical dimensions of the device.