流动聚焦型微流控体系中的液滴的图案化排列和转变模式

流体在微流通道中形成剪切流场(低雷诺数)．不同于宏观体系,由于剪切力和表面张力的竞争作用,产生的液滴在微尺度下的微流通道中形成特殊的排列现象---周期性类似“晶格”排列现象．设计了新型流动聚焦型微流控芯片,分析研究在微流体系中液滴周期性图案化排列和转变机理性,液滴排列模式受两方面因素影响：水油两相的流速比值和微通道尺寸．当微通道宽度为250或300 μm时,液滴形成单层分散,双层和单层挤压排列．当微通道宽度为350 μm 时,液滴会形成单层分散到三层排列到双层挤压最后到单层挤压排列．当出口通道宽度增加到400 μm时,甚至出现了液滴四层排列的现象．同时研究了各个液滴排列模式的“转变点”.     

液滴法制备高尺度比玻璃微球壳的研究

 定量给出了液滴法制备玻璃微球壳（HGM）的直径与壁厚之间的依存关系,确定了制备大直径薄壁HGM的液滴炉温度分布、抽气速率、溶液浓度和液滴发生器操作参数等工艺条件,制备出直径为300～450μm、壁厚为0.7～1.2μm、尺度比为300～700的HGM,表面粗糙度优于10nm,球形度和同心度均优于97%,耐外压能力大于0.91MPa,耐内压能力至少大于0.43MPa。     

液滴法制备高尺度比玻璃微球壳的研究

定量给出了液滴法制备玻璃微球壳（HGM）的直径与壁厚之间的依存关系,确定了制备大直径薄壁HGM的液滴炉温度分布、抽气速率、溶液浓度和液滴发生器操作参数等工艺条件,制备出直径为300～450μm、壁厚为0.7～1.2μm、尺度比为300～700的HGM,表面粗糙度优于10nm,球形度和同心度均优于97%,耐外压能力大于0.91MPa,耐内压能力至少大于0.43MPa。     

基于有限元计算的微流控聚焦装置液滴生成特性分析

研究微流控聚焦装置液滴生成特性是液滴微流控芯片结构优化设计的基础。利用水平集方法结合有限元技术建立了微流控聚焦装置内液滴生成过程的数值计算模型,并分析了分散相与连续相流速比、微流道几何结构对液滴生成机制和液滴生成特性的影响规律。在一定的流速比、微流道入口宽度比范围内,均生成了性态良好的液滴。当分散相与连续相入口宽度比大于1时,液滴尺寸随连续相入口宽度、连续相流速的增大而减小,液滴生成频率随连续相入口宽度、连续相流速的增大而增大;当分散相与连续相入口宽度比小于1时,液滴尺寸随分散相入口宽度增大而增大,随连续相流速的增大而减小,液滴生成频率随分散相入口宽度、连续相流速的增大而增大。数值计算结果表明：微流控聚焦装置液滴生成受几何结构、流速及两相流体物性参数的耦合作用,模拟计算的结果可为微流控聚焦装置结构优化设计提供指导。     

电润湿液滴微流控芯片液滴驱动的EHD数值模拟

利用液滴电水动力学方法,通过求解耦合的N-S方程,VOF方程以及电场方程,首次对电润湿非接地型单板式(开放式)液滴微流控芯片的液滴驱动过程进行了数值模拟研究.结果表明,在液滴向驱动电极运动的过程中,液滴形态呈现摇摆特性,前进和后退接触角呈现震荡特性,液滴运动速度逐渐下降,并最终停留在零电极和驱动电极的中间位置.     

用于微流控液滴检测的共焦激光诱导荧光检测系统

以发射波长为473nm的二极管泵浦激光器为激发光源,搭建适于微流控液滴检测的共聚焦激光诱导荧光检测系统.系统玻璃芯片采用简易加工技术加工而成.并用2%十八烷基三氯硅烷将微通道处理为具有强疏水性质.荧光素钠溶液在T形通道交叉处被十四烷剪切形成液滴,液滴流经检测点时被激光诱导荧光系统检测.荧光素钠的检出限为1.1×10<'...     

T型微通道中液滴半阻塞不对称分裂行为研究

液滴不对称分裂是获得不同尺寸微液滴的优选方法,研究液滴不对称分裂行为对于生物医学、能源化工及食品工程等领域具有重要意义.本文研制T型微通道芯片并设计搭建T型微通道液滴半阻塞不对称分裂行为可视化实验平台,研究流量调控对微液滴分裂比的影响规律,并建立理论模型对分裂比进行预测,得到以下结论:液滴不对称挤压分裂过程分为挤压前期、挤压后期和快速夹断阶段,在挤压前期,液滴颈部宽度随时间呈线性变化,在挤压后期,颈部宽度随时间呈指数关系,而在快速夹断阶段,液滴颈部向心收缩的界面附加压力占主导,液滴颈部宽度剧烈收缩,呈断崖式减小;调控分支通道流量可对液滴不对称分裂比进行调控,且调控作用受毛细数影响较大;基于液液流动压降模型的液滴分裂比预测模型能够有效预测液滴分裂比.     

液滴法制备空心玻璃微球的模拟计算

通过对液滴法制备空心玻璃微球的成球过程进行分析,建立了成球过程数学模型,定量描述了液滴的形成、液滴的封装、凝胶球壳的形成与干燥,发泡剂的分解,球壳的预热与熔炼、冷却与收集等过程中,液滴/球壳的大小、速率、壁厚、气压等随操作条件的变化,计算了抽气速率、发泡剂浓度、玻璃溶液浓度和初始液滴大小等的改变对成球过程的影响,并进行了初步验证实验。     

液滴法制备空心玻璃微球的模拟计算

 通过对液滴法制备空心玻璃微球的成球过程进行分析,建立了成球过程数学模型,定量描述了液滴的形成、液滴的封装、凝胶球壳的形成与干燥,发泡剂的分解,球壳的预热与熔炼、冷却与收集等过程中,液滴/球壳的大小、速率、壁厚、气压等随操作条件的变化,计算了抽气速率、发泡剂浓度、玻璃溶液浓度和初始液滴大小等的改变对成球过程的影响,并进行了初步验证实验。     

T型微通道中微液滴被动破裂的可视化实验研究

本文搭建了微流体实验平台,对T型微通道内微液滴的对称被动破裂进行可视化实验研究,探索微液滴破裂的机理。采用横截面为200μm×100μm或100μm×100μm的微通道,用改性硅油和花生油作为连续相,去离子水作为离散相,在毛细数为0~0.1的范围下,捕捉到了T型微通道被动破裂的隧道破裂、不连续阻塞破裂、永久阻塞破裂和未破裂等四种流型,绘制了流型图并获得了临界毛细数与微液滴的无量纲轴向长度经验关联式,用来预测不同结构及尺寸微通道发生破裂等与未破裂的条件.     

Demonstration of Four Fundamental Operations of Liquid Droplets for Digital Microfluidic Systems Based on an Electrowetting-on-Dielectric Actuator

An electrowetting-on-dielectric actuator is developed, in which the liquid is sandwiched between top and bottom plates. For the bottom plate, silicon wafer is used as the substrate, the heavily phosphorus-doped polysilicon film is deposited by low pressure chemical vapour deposition as the microelectrode array, and thermally grown SiO2 film as the dielectric layer. The top p/ate is a glass plate covered with transparent and conductive indium tin oxide as the ground electrode. In addition, a Teflon AF1600 film is spun on the surface of both the plates as the hydrophobic layer. The experimental results show that when the gap height between two plates is 133μm, a prototype of the device is capable of creating, transporting, merging and dividing droplets of deionized water in an air environment with a 70V at lOHz voltage pulse. This is also established by simulations using the computational fluidic software of CFD-ACE＋.     

复方甲硝唑片含量测定方法的比较

文章经选择适当的测定波长,同时采用系数倍率法和联立方程组新解法不经提取分离直接测定复方甲硝唑片中甲硝唑和维生素B_6的含量。同时采用河北省药品标准法进行了对比测定。利用SPSS统计软件通过对各方法的测定结果做方差分析,结果表明:新建立的系数倍率法和联立方程组新解法的测定结果无显著性差异,而两法分别与河北省药品标准法的测定结果比较,均存在显著性差异。作者认为:河北省药品标准法经过烦琐的提取分离过程,引入的误差较大。而新建立的两法简便、快速、准确,优于河北省药品标准法。     

Droplets sliding on fibres

We present the results of a combined experimental and theoretical investigation of oil droplets sliding on fibres. First, both the axisymmetric shape and the motion of a droplet on a vertical fibre are described. The motion is shown to result from a balance between the droplet weight and the viscous stresses. On a long-term range, the droplet loses some mass through coating the fibre, which decreases its velocity. In a second time, we rationalize the behaviour of a droplet that encounters a junction between vertical and horizontal fibres. Depending on its size, the droplet may cross the junction or remain blocked. The transition is well described by an ordinary differential equation equivalent to a damped harmonic oscillator truncated to the neighbourhood of the horizontal fibre. This simple system is the basic element for more complex fiber networks that would be useful in microfluidic applications involving droplets.     

LED准直器设计中复合抛物面同步多曲面方法

利用非成像光学中流线法和同步多曲面(SMS)法,设计一种具有发散角小、均匀度好和光效高的LED准直器。设计中由复合抛物面(CPC)完成初级配光,将朗伯光源±90°的发散角缩小到±45°,再以SMS法设计的多重自由反射曲面实现准直均匀配光,并由光学扩展量给出准直器的理论光效,最后引入平顶宽度、平顶光效和平顶均匀度等的定义,以更好地反映准直光束质量。光学仿真结果表明,准直器的发散角小于±2.26°,整体光效达到0.79,理论与仿真光效的误差小于2.5%,在0.9平顶宽度范围内光斑均匀度大于等于0.9,平顶光效为0.56,效果良好。     

Droplets on inclined rough surfaces

The behaviour of liquid droplets on inclined heterogeneous surfaces was simulated by the lattice-Boltzmann method using the Shan-Chen multiphase model. The effect of topography of the surface on the contact angle hysteresis was investigated. It is shown in particular, by using anisotropic rough surfaces, how surface topography and thereby the continuity of the three-phase contact line, affect this hysteresis. Our results clearly indicate that the superhydrophobicity of a surface cannot be judged by the contact angle alone.     

微流控芯片系统中测温及控温装置的研制

报道了一种结构简单、成本低、操作方便、应用于微流控芯片系统中温度测量及温度控制的装置。该系统以CCD摄像机、荧光显微镜及图像采集卡构成的非接触荧光指示剂测温装置,实现了微流体空间温度分布测量以及随时间变化的温度测量。提出了以透明氧化铟锡薄膜玻璃作为加热元件,采用PID控制算法的温度控制平台,稳态时温度控制精度可达到±0.1 ℃。采用该测温和控温装置研究了玻璃微流控芯片微通道内溶液温度在空间上和随时间的变化情况,结果表明该方法简单、有效,可达到μm级的空间分辨率和ms级的时间分辨率。     

非对称布置液滴在波纹状基底上的聚并过程

基于润滑理论建立在波纹基底上两个含表面活性剂液滴聚并的演化模型，模拟液滴位于波纹基底波峰和波谷处的聚并过程，分析液滴初始间距和基底高度对聚并的影响，并与对称布置液滴进行比较.结果表明：液滴高度随时间呈现五个阶段变化；活性剂浓度在短时间内完成三个阶段变化；初始间距的增大将延长液滴及活性剂聚并时间；增大基底高度将缩短液滴及活性剂聚并时间；非对称液滴相较于对称液滴聚并时间短，聚并速度快.     

A Model for the Contact Angle of Liquid Droplets on Rough Surfaces

Up to now, measured results of the contact angle on rough surfaces have been explained usually based on the Wenzel equation （1936） and the Cassie-Baxter equation （1944）. However, these equations do not take into account considerations of liquid wetting behaviors on rough surfaces, and this leads to poor understanding of the mechanisms of contact between liquid droplets and rough surfaces （e.g. contact angle hysteresis）. We propose a new model for the contact angle of liquid droplets. By means of the present model, we can well understand the evperimental data which could not be well explained by the Wenzel equation and the Cassie-Baxter equation.     

Molecular-Dynamics Simulations of Droplets on a Solid Surface

By using a semi-empirical Lennard-Jones embedded-atom-method potential, we study the influence of many-body forces and atomic size mismatch on the wetting behavior of nano droplets on a solid surface. With molecular dynamics simulations, we find that the contact angle decreases with increasing many-body forces. The increase of atomic size mismatch between solid and liquid results in the decrease of contact angles. Our calculation also shows that the interface structure is strongly affected by the interaction between liquid and solid as well as the atomic size mismatch. For weak solid-liquid interaction, the interface layer of the droplet nearest to the solid exhibits a typical simple liquid structure regardless of the size mismatch. For strong solid-liquid interaction, evident ordering in the interface layer is observed for well matched cases.