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1.
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。  相似文献   

2.
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.  相似文献   

3.
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.  相似文献   

4.
正、负离子表面活性剂混合体系的负触变性   总被引:2,自引:0,他引:2  
报导正、负离子表面活性剂混合体系的负触变性(负触变性通常只存在于某些高分子溶液及极少数粗分散体系中).总结出负触变性的形成规律,提出了负触变性的形成机理,认为负触变性的产生是由于溶液中存在具有一定大小的层状胶团,当溶液流动时,层状胶团双层之间的平行排列方式被打乱,导致溶液粘度随时间而增加.  相似文献   

5.
稳态双曲流场中液/液混合的粘性液滴哑铃分散模型   总被引:1,自引:0,他引:1  
通过对稳态双曲流场中液/液混合体系分散相液滴所受分散作用力的分析,建立了粘性液滴的哑铃分散模型.趋于将两粘性液滴分开的分散作用力与粘度比、流场类型和强度、液滴半径、哑铃取向和尺寸有关.该模型解释了流场类型与分散作用的关系.流场类型对液滴的分散具有很大影响,在纯应变拉伸流场中分散作用力是简单剪切流场中的两倍,因而对于液滴的分散,拉伸流场较简单剪切流场更有效,这与以前的实验结论符合.当体系粘度比趋于无穷大时本模型转化为刚性哑铃分散模型  相似文献   

6.
微流控芯片液滴生成与检测技术研究进展   总被引:1,自引:0,他引:1  
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。  相似文献   

7.
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。  相似文献   

8.
耗散粒子动力学研究片状双层——囊泡转变   总被引:2,自引:1,他引:1       下载免费PDF全文
片状双层是囊泡自发形成过程中的重要中间态,由片状双层向囊泡的转变机理一直未被认清.本文以磷脂分子DMPC作为模拟对象,采用普适性的粗粒化模型和耗散粒子动力学模拟方法,以体系粒子无序分布和无应力片状双层作为初态,对水溶液中片状双层——囊泡的转变过程进行了深入研究.发现尾-水粒子间憎水作用能最小化是片状双层卷曲形成囊泡的微观本质.囊泡的双分子层为二维流体.此外还得到了囊泡上粒子的位置分布和化学键排列取向等方面的结构信息.  相似文献   

9.
以单分散液滴为模板,通过紫外光引发自由基聚合的方法,用微流控技术制备出单分散甲基丙烯酸甲酯/苯乙烯/四氧化三铁磁性聚合物微球,制备装置简易、操作简单.对样品的形貌结构、粒度分布、表面官能团、组成成分、有效磁含量及表面电势进行了表征分析.微球的粒径约为200μm,单分散性良好,且表面电势为-24 mV时能够迅速对水体中的阳离子染料孔雀石绿进行有效吸附分离.探究了pH、孔雀石绿溶液初始浓度、吸附时间和反应温度对吸附效率的影响,发现在孔雀石绿溶液体积为50 mL(50 mg·L-1),投加量为50 mg, pH为7,温度为30℃时吸附效率高达94.38%,重复利用9次的吸附效率仍可达到80%以上,具有较好的吸附能力.  相似文献   

10.
通过一个两步程序在膜片电极尖端形成自组装双层脂膜:(1)膜片电极尖端沾取成膜液;(2)将吸附成膜液的尖端浸入电解液中,排除尖端多余的成膜液,通过电学方法监测双层脂膜的形成。将短杆菌肽通道蛋白分散在成膜液和电解质溶液中,在制备膜片电极支撑双层脂膜过程中,短杆菌肽重组到双层脂膜中形成离子通道,对通道的一般特性进行了研究,并观察到通道开放和关闭的现象。  相似文献   

11.
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.  相似文献   

12.
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.  相似文献   

13.
Lee C  Lee J  Kim HH  Teh SY  Lee A  Chung IY  Park JY  Shung KK 《Lab on a chip》2012,12(15):2736-2742
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.  相似文献   

14.
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.  相似文献   

15.
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.  相似文献   

16.
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.  相似文献   

17.
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.  相似文献   

18.
Kim C  Chung S  Kim YE  Lee KS  Lee SH  Oh KW  Kang JY 《Lab on a chip》2011,11(2):246-252
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.  相似文献   

19.
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.  相似文献   

20.
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.  相似文献   

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