CN1515892A - Micro-analysis chip for absorbance photometric detection and method of use thereof - Google Patents
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Abstract
Description
技术领域Technical field
本发明涉及的领域为微流控芯片分析,特别是涉及一种进行吸收光度检测的微分析芯片及其使用方法。The field of the invention relates to microfluidic chip analysis, in particular to a microanalysis chip for absorbing photometric detection and its use method.
背景技术 Background technique
微流控芯片分析以分析化学和分析生物化学为基础,以微机电加工技术为依托,以微管道网络为结构特征,把试样的采集、预处理、分离、反应、检测等部分集成在几平方厘米的面积内,从而高效、快速地完成试样的分离、分析及检测。自九十年代初提出微全分析系统以来,微流控芯片分析(Microfluidic Analysis)一直处于最活跃的发展前沿,代表着21世纪分析仪器走向微型化、集成化的发展方向。通常,微流控芯片由上下两层或多层芯片构成,芯片的材料为单晶硅、或石英、或玻璃、或高分子聚合物等。芯片的面积约为几平方厘米,微管道宽度和深度为微米级,一般为封闭式微通道网络,通过垂直于芯片与微通道相连的孔进出样品。Microfluidic chip analysis is based on analytical chemistry and analytical biochemistry, relying on micro-electromechanical processing technology, with micro-pipeline network as the structural feature, integrating sample collection, pretreatment, separation, reaction, detection and other parts in several Within an area of square centimeters, the separation, analysis and detection of samples can be completed efficiently and quickly. Since the micro-analysis system was proposed in the early 1990s, Microfluidic Analysis has been at the most active development frontier, representing the development direction of miniaturization and integration of analytical instruments in the 21st century. Usually, a microfluidic chip is composed of upper and lower layers or multi-layer chips, and the material of the chip is single crystal silicon, or quartz, or glass, or high molecular polymer. The area of the chip is about several square centimeters, and the width and depth of the microchannels are on the order of micrometers. Generally, it is a closed microchannel network, and samples enter and exit through holes perpendicular to the chip and connected to the microchannels.
本发明涉及的领域是有关微流控芯片上的检测系统的研究。检测系统是一个分析系统的重要组成部分。微流控芯片因其芯片体积小,进样量仅为皮、纳升级,检测处的反应通道一般为几十微米宽,因此对其检测手段和装置的要求有其特殊性。The field that the invention relates to is the research on the detection system on the microfluidic chip. The detection system is an important part of an analysis system. Due to the small size of the chip, the injection volume of the microfluidic chip is only picoliters or nanoliters, and the reaction channel at the detection site is generally tens of microns wide, so the requirements for its detection methods and devices have their own particularities.
吸收光谱分析法(亦称吸收光度检测法)是一种适用性广泛的检测方法,在分析化学中占有重要地位,也是最早用于微分析系统的检测方法之一。光度检测的波长范围约为185~1100纳米。但由于微流控芯片通道吸收池内的检测体积小,吸收光程短,导致采用吸光光度法检测灵敏度比常规宏观系统低2-4个数量级,因而目前在微流控芯片分析系统中的应用受到很大限制。近年有很多研究致力于增加微流控芯片上光度检测系统的吸收光程,以提高光度检测灵敏度。Absorption spectroscopy (also known as absorption photometry) is a widely applicable detection method, which occupies an important position in analytical chemistry and is also one of the earliest detection methods used in micro-analysis systems. The wavelength range of photometric detection is about 185-1100 nanometers. However, due to the small detection volume and short absorption path in the channel absorption cell of the microfluidic chip, the detection sensitivity of the absorptiometry is 2-4 orders of magnitude lower than that of the conventional macroscopic system, so the current application in the microfluidic chip analysis system is limited. Very restrictive. In recent years, many studies have been devoted to increasing the absorption path length of the photometric detection system on the microfluidic chip to improve the sensitivity of photometric detection.
目前已发表的技术可以分为以下两类:一是采用微加工的方法增加吸收池的光程,具体包括:制作高深宽比通道的芯片,垂直于通道直接检测,通道的深度一般小于100微米,通过这种方法提高光程,其效果有限(Laura Ceriotti,Jan Lichtenberg,et al.,Micro Total Analysis Systems 2001,339-340)在芯片上制作U形(Liang Z H,ChiemN,Ocvik G,Tong T,Fluri K,Harrison D J.Anal.Chem.1996,68:1040)或Z形结构的流通吸收池,沿通道方向引入光及检测,可以得到更长的光程,但是这种结构难以制造和调准,任何偏差都会造成分析信号的损耗和灵敏度的下降,受入射光的散射效应限制,检测光程不宜大于150微米(HS.Moosavi,Y.Jiang,et al.,Electrophoresis,vol.21,pp.1291-1299,2000);三层夹心式芯片,在中间层制作垂直通道吸收池,其检测光程达毫米级,但是这种芯片中间垂直通道制作困难,封接三层夹心式芯片比较困难,成本高(Jeffrey Wolk,MichaelSpaid,Morten Jensen,Richard MacReynolds,Knute Stevenson,and Ring-Ling Chien,Micro TotalAnalysis Systems 2001,367-368)。另一类采用平面波导技术,在芯片的上下面制作光全反射面,光以一定角度从上方入射口入射,在上下反射面之间反射,可多次经过通道,这种方法对入射光窗精度要求很高,需要非常精确入射光才能保证在微小的检测窗检测到信号,报道的检测光程为50-272微米(Moosav H S,Jiang Y,Lester L,McKinnon G,Harrison D J.Electrophoresis,2000,21:1291)。还有在吸收池内部集成镜面反射器件,采用硅MEMS刻蚀等制作高反射率镜面或反射通道(Verpoorte E,Manz A,Luedi H,Bruno A E,Maystre F,Krattiger B,Widmer H M,Van der Schoot B H,De Rooij N F.Sens.Actuators.B.1992,B6:66)(Tiggelaar R M,Veenstra T T,Sanders R G P,Gardeniers J G E,Elwenspoek M C,Van den Berg A.Talanta.2002,56:331)(Hidekuni Takao,Toshihiko Noda,MitsuakiAshiki,Kazuhiro Miyamura,Kazuaki Sawada,Makoto Ishida,Micro Total Analysis Systems 2001,363-364),基于多重平面反射结构,反射光程为毫米级,由于平面反射对光路要求苛刻,在芯片吸收池内集成反射镜面技术要求较高。The currently published technologies can be divided into the following two categories: one is to increase the optical path of the absorption cell by micromachining, which specifically includes: making a chip with a high aspect ratio channel and directly detecting it perpendicular to the channel. The depth of the channel is generally less than 100 microns , increasing the optical path length by this method has limited effect (Laura Ceriotti, Jan Lichtenberg, et al., Micro Total Analysis Systems 2001, 339-340) making U-shape on chip (Liang Z H, Chiem N, Ocvik G, Tong T, Fluri K, Harrison D J.Anal.Chem.1996, 68:1040) or a flow-through absorption cell with a Z-shaped structure, introducing light and detecting along the channel direction, can obtain a longer optical path, but this structure is difficult to manufacture And alignment, any deviation will cause the loss of analysis signal and the decline of sensitivity, limited by the scattering effect of incident light, the detection optical path should not be greater than 150 microns (HS.Moosavi, Y.Jiang, et al., Electrophoresis, vol.21, pp.1291-1299, 2000); three-layer sandwich chip, the vertical channel absorption cell is made in the middle layer, and its detection optical distance reaches millimeter level, but it is difficult to make the vertical channel in the middle of this chip, and the comparison of sealing the three-layer sandwich chip Difficult and costly (Jeffrey Wolk, MichaelSaid, Morten Jensen, Richard MacReynolds, Knute Stevenson, and Ring-Ling Chien, Micro Total Analysis Systems 2001, 367-368). The other type uses planar waveguide technology to make light total reflection surfaces on the upper and lower sides of the chip. The light is incident from the upper entrance at a certain angle, reflected between the upper and lower reflection surfaces, and can pass through the channel multiple times. The precision requirement is very high, and the incident light needs to be very precise to ensure that the signal is detected in the tiny detection window. The reported detection optical path is 50-272 microns (Moosav HS, Jiang Y, Lester L, McKinnon G, Harrison D J.Electrophoresis , 2000, 21: 1291). There are also integrated specular reflection devices inside the absorption pool, using silicon MEMS etching to make high reflectivity mirrors or reflection channels (Verpoorte E, Manz A, Luedi H, Bruno A E, Maystre F, Krattiger B, Widmer H M, Van der Schoot B H, De Rooij N F. Sens. Actuators. B. 1992, B6:66) (Tiggelaar R M, Veenstra T T, Sanders R G P, Gardeniers J G E, Elwenspoek M C, Van den Berg A. Talanta.2002, 56:331) (Hidekuni Takao, Toshihiko Noda, Mitsuaki Ashiki, Kazuhiro Miyamura, Kazuaki Sawada, Makoto Ishida, Micro Total Analysis Systems 2001, 363-364), based on the multi-plane reflective structure, the reflective optical path is millimeter-scale, Due to the strict requirements on the optical path due to plane reflection, the technical requirements for integrating reflective mirrors in the chip absorption pool are relatively high.
目前,光度检测的各种增加光程的方法,都没有突破芯片及其通道微小尺寸带来的固有局限,因而无法真正突破检测限的瓶颈,其检测灵敏度无法达到常规分光光度计的水平。而且大都需要些要求很高的微加工手段,结构复杂,成本高,限制了光度法在芯片领域的应用。At present, the various methods of increasing the optical length of photometric detection have not broken through the inherent limitations brought about by the tiny size of the chip and its channel, so it cannot really break through the bottleneck of the detection limit, and its detection sensitivity cannot reach the level of conventional spectrophotometers. Moreover, most of them require some highly demanding micro-processing methods, with complex structures and high costs, which limit the application of photometry in the field of chips.
液芯波导管是一种以液体为内芯的光导纤维,在液芯波导管内,光发生全反射波导,可进行几乎无损的传播。该技术已被用于宏观的光度检测领域。现有研究表明用液芯波导管作为吸收池,其检测吸光度正比于浓度,符合朗伯比尔定律,其显著特点是可以极大的提高分光光度法的灵敏度及测量的线性范围。但在微分析芯片领域,尚未有液芯波导管应用于光度检测的报道。The liquid core waveguide is a kind of optical fiber with liquid as the inner core. In the liquid core waveguide, the light is totally reflected in the waveguide and can be transmitted almost losslessly. This technique has been used in the field of macroscopic photometric detection. Existing studies have shown that using a liquid core waveguide as an absorption cell, its detection absorbance is proportional to the concentration, which conforms to Lambert-Beer's law, and its notable feature is that it can greatly improve the sensitivity of the spectrophotometer and the linear range of measurement. However, in the field of micro-analysis chips, there is no report on the application of liquid-core waveguides in photometric detection.
发明内容Contents of Invention
本发明的目的在于突破芯片及其通道微小尺寸带来的固有局限,提供一种进行吸收光度检测的微分析芯片及其使用方法,将光度检测的有效光程提高2-3个数量级以上,大幅提高芯片上的分光光度检测灵敏度。The purpose of the present invention is to break through the inherent limitations brought about by the tiny size of the chip and its channel, provide a micro-analysis chip for absorbing photometric detection and its use method, increase the effective optical path of photometric detection by more than 2-3 orders of magnitude, greatly Increased sensitivity of on-chip spectrophotometric detection.
本发明提供的吸收光度检测的微分析芯片,是一种基于液芯波导原理的用于长光程吸收光度检测的微分析芯片,根据本发明,微分析芯片的吸收池,由微分析芯片通道与外接的液芯波导管耦合构成。The micro-analysis chip for absorbing photometric detection provided by the present invention is a micro-analyzing chip for long optical path absorbing photometric detection based on the liquid core waveguide principle. According to the present invention, the absorption pool of the micro-analyzing chip is composed of micro-analyzing chip It is formed by coupling with an external liquid core waveguide.
根据本发明,所述的液芯波导管是一种管内有待检测流体流过,利用管壁的性质实现光线在管内部流体中连续全反射或反射传递的毛细管。液芯波导管内通道的横截面构型为圆形或椭圆形。液芯波导管内通道的内径在0.1微米-5毫米范围内,管壁厚度在1微米-1厘米范围内。液芯波导管的管长在5毫米-50米范围内。According to the present invention, the liquid core waveguide is a capillary through which the fluid to be detected flows through the tube, and the properties of the tube wall are used to realize continuous total reflection or reflective transmission of light in the fluid inside the tube. The cross-sectional configuration of the channel in the liquid core waveguide is circular or elliptical. The inner diameter of the inner channel of the liquid core waveguide is in the range of 0.1 micron to 5 mm, and the thickness of the tube wall is in the range of 1 micron to 1 cm. The tube length of the liquid core waveguide is in the range of 5mm-50m.
根据本发明,为实现光在波导管内的波导,所使用的波导管的内壁、外壁、管壁本身三部分之中,至少有一部分具有对光线的反射或全反射功能。According to the present invention, in order to realize the waveguide of light in the waveguide, at least one part of the inner wall, outer wall, and tube wall of the waveguide used has the function of reflection or total reflection of light.
根据本发明,所使用的一类波导管是利用折射率的差异实现的光的波导,其特征是,在波导管的内壁、外壁、管壁本身三者之中,至少一个采用折射率低于管内流体的材料制作。According to the present invention, a type of waveguide used is a waveguide for light realized by using a difference in refractive index, and it is characterized in that at least one of the inner wall, outer wall, and tube wall of the waveguide uses a material with a refractive index lower than that of the waveguide. The material of the fluid in the tube is made.
根据本发明,所使用的另一类波导管是利用光反射的原理实现光的波导,其特征是,所述波导管的内壁、外壁、管壁本身三者之中,至少一个采用具有高效光反射性能的材料制作。According to the present invention, another type of waveguide used is a waveguide that utilizes the principle of light reflection to realize light. Made of reflective material.
根据本发明的另一个特点,微分析芯片内通道与液芯波导管通道耦合接口采用小死体积的接口,有利于降低试样带在接口处的分散,同时,在接口处不易留存气泡,以免干扰正常的测定操作。According to another feature of the present invention, the coupling interface between the channel in the micro-analysis chip and the channel of the liquid core waveguide adopts an interface with a small dead volume, which is conducive to reducing the dispersion of the sample strip at the interface, and at the same time, it is not easy to retain air bubbles at the interface to avoid Interfere with normal assay operation.
本发明的吸收光度检测的微分析芯片使用方法,实际测定时,检测系统光源发射的入射光线由波导管入口进入液芯波导管,通过管内流体,由波导管出口导出,被光检测器检测。光源发出的光被液芯波导管中流体吸收,从而发生吸光度的变化。更为有利的是,光源的入射光与波导管圆心同轴对准,以提高入射光能量,即提高测定的信噪比。由波导管出口导出的光,采用与波导管同轴对准的光纤收集,再导入光检测器,以提高收集光的效率。In the method of using the micro-analysis chip for absorbing photometric detection of the present invention, during actual measurement, the incident light emitted by the light source of the detection system enters the liquid core waveguide from the entrance of the waveguide, passes through the fluid in the tube, is exported from the outlet of the waveguide, and is detected by the photodetector. The light emitted by the light source is absorbed by the fluid in the liquid core waveguide, resulting in a change in absorbance. More advantageously, the incident light of the light source is coaxially aligned with the center of the waveguide, so as to increase the energy of the incident light, that is, improve the signal-to-noise ratio of the measurement. The light exported from the exit of the waveguide is collected by an optical fiber coaxially aligned with the waveguide, and then introduced into a photodetector to improve the efficiency of light collection.
根据本发明的使用方法,采用较长的波导管有利于提高光吸收的有效光程。According to the use method of the present invention, the use of a longer waveguide is beneficial to increase the effective optical path of light absorption.
根据本发明的使用方法,相对波导管内流体,利用管外壁实现波导,因存在光线在管壁内的传输而损失光度检测的有效光程;对于相同长度的波导管,利用管内壁实现波导比利用管外壁实现波导具有更长的有效光程。According to the use method of the present invention, relative to the fluid in the waveguide, the outer wall of the tube is used to realize the waveguide, and the effective optical path of photometric detection is lost due to the transmission of light in the tube wall; The outer wall of the tube realizes a waveguide with a longer effective optical path.
根据本发明的使用方法,利用管外壁实现波导时,采用较薄的液芯波导管管壁,有利于提高吸收池的有效光程。According to the use method of the present invention, when the outer wall of the tube is used to realize the waveguide, the tube wall of the liquid core waveguide is thinner, which is beneficial to increase the effective optical path of the absorption pool.
根据本发明的使用方法,对于采用透光材料制作管壁的波导管,采用在波导管的光进入口外壁,覆盖不透光的遮光材料,减少不经过流体的无用光线的进入,能显著提高光度检测的灵敏度。更为有利的是,在液芯波导管与芯片的耦合端外壁及端面都覆盖不透光的遮光材料,能进一步提高光度检测的灵敏度。According to the use method of the present invention, for the waveguide adopting the light-transmitting material to make the tube wall, the outer wall of the light entrance of the waveguide is used to cover the light-proof light-shielding material, so as to reduce the entry of useless light that does not pass through the fluid, and can significantly improve the performance of the waveguide. Sensitivity of photometric detection. More advantageously, the outer wall and end surface of the coupling end of the liquid core waveguide and the chip are covered with opaque light-shielding material, which can further improve the sensitivity of photometric detection.
本发明的主要优点在于:在小体积的微分析芯片上可进行灵敏度高光度检测;所需的试样体积在低于1微升的数量级时,检测灵敏度完全可以达到和超过常规的紫外可见分光光度计;此外,波导管的长度不受芯片大小的限制,液芯波导管吸收池可长达厘米至分米级,甚至米级,达到很高的检测灵敏度;当液芯波导管很长时,可以采用盘成螺旋状的方法,减小系统体积。液芯波导管光的损耗极小,抗干扰能力强;检测系统结构简单,容易加工,性能稳定可靠,体积小,易于集成化。The main advantages of the present invention are: on the small-volume micro-analysis chip, high-sensitivity and high-photometry detection can be carried out; when the required sample volume is in the order of magnitude lower than 1 microliter, the detection sensitivity can reach and exceed the conventional ultraviolet-visible spectroscopic Photometer; in addition, the length of the waveguide is not limited by the size of the chip, and the liquid-core waveguide absorption cell can be as long as centimeters to decimeters, or even meters, to achieve high detection sensitivity; when the liquid-core waveguide is very long , you can use the method of coiling into a spiral to reduce the volume of the system. The light loss of the liquid core waveguide is extremely small, and the anti-interference ability is strong; the detection system has a simple structure, easy processing, stable and reliable performance, small size, and easy integration.
本发明的另一个突出优点在于吸收池对光源要求比较简单,用小型激光器或者发光二极管即可作光源,而且不需要任何其他光源校准器件,即可得到较强的光检测信号;为了提高系统的集成性,可以使用光电二极管作光检测器件,以达到整体微型化的要求。Another outstanding advantage of the present invention is that the absorption pool has relatively simple requirements on the light source, and a small laser or light-emitting diode can be used as the light source, and a strong light detection signal can be obtained without any other light source calibration devices; in order to improve the system Integrative, photodiodes can be used as light detection devices to meet the overall miniaturization requirements.
本发明的另一个优点是可以实现多样品连续进样检测。检测样品通过液芯波导管,即排出芯片体系,因此可以连续进样,可用于在线监控。Another advantage of the present invention is that it can realize continuous injection and detection of multiple samples. The detection sample passes through the liquid core waveguide, that is, it is discharged from the chip system, so it can be continuously injected and used for online monitoring.
本发明可广泛应用于基于芯片的连续流动和流动注射分析。The invention can be widely applied to chip-based continuous flow and flow injection analysis.
附图说明Description of drawings
图1.是根据本发明一个优选实施例的基于液芯波导原理的用于长光程吸收光度检测的微分析芯片。Fig. 1 is a micro-analysis chip for long optical path absorption photometric detection based on liquid core waveguide principle according to a preferred embodiment of the present invention.
图2.是图1芯片上液芯波导管与微流控芯片耦合接口的局部放大图。Figure 2 is a partially enlarged view of the coupling interface between the liquid core waveguide on the chip and the microfluidic chip in Figure 1.
图3.是根据本发明优选实施例中所用液芯波导管的一个实例。Figure 3. An example of a liquid core waveguide used in a preferred embodiment according to the present invention.
图4.是图3实施例中所用液芯波导管的横截面透光图,对比了没有进行遮光处理和进行了遮光处理的不同的效果。Fig. 4 is a cross-sectional light transmission diagram of the liquid core waveguide used in the embodiment of Fig. 3, comparing the different effects of the light-shielding treatment without light-shielding treatment and the light-shielding treatment.
图5.是根据本发明优选实施例吸收池中液芯波导管信号检测端局部放大图。Fig. 5 is a partial enlarged view of the signal detection end of the liquid core waveguide in the absorption cell according to the preferred embodiment of the present invention.
图6.显示安装有图3实施例装置的微芯片分析系统对不同浓度铁(II)-邻菲啰啉配合物检测的结果记录图。Fig. 6 shows the record diagram of the detection results of different concentrations of iron (II)-o-phenanthroline complexes by the microchip analysis system equipped with the device of the embodiment of Fig. 3 .
图7.显示安装有图3实施例装置的微芯片分析系统对不同浓度铁(II)-邻菲啰啉配合物检测的标准曲线以及在分光光度计平行测定的标准曲线图。Fig. 7 shows the standard curve of different concentration iron (II)-o-phenanthroline complexes detected by the microchip analysis system equipped with the device of Fig. 3 embodiment and the standard curve diagram of parallel determination in spectrophotometer.
图8.是根据本发明优选实施例中所用液芯波导管的另一个实例。Figure 8. is another example of a liquid core waveguide used in a preferred embodiment according to the present invention.
图9.显示安装有图8实施例结构的全Teflon AF液芯波导管微芯片分析系统对不同浓度铁(II)-邻菲啰啉配合物检测的结果记录图。Fig. 9. Shows the recorded results of the detection of different concentrations of iron (II)-o-phenanthroline complexes by the full Teflon AF liquid core waveguide microchip analysis system equipped with the structure of the embodiment in Fig. 8.
图10.显示安装有图8实施例结构的内镀银液芯波导管微芯片分析系统对铁(II)-邻菲啰啉配合物检测的结果记录图。Fig. 10 shows the record diagram of the detection results of the iron (II)-o-phenanthroline complex by the internal silver-plated liquid core waveguide microchip analysis system installed with the structure of the embodiment in Fig. 8.
具体实施方式 Detailed ways
参照附图,以下将详细描述根据本发明的一个优选实施例1。Referring to the accompanying drawings, a
图1是根据本发明一个优选实施例制得的耦合液芯波导管的微流控芯片构造图。微流控芯片由上(1)、下(2)两玻璃片组成,玻璃片厚度为1.7毫米。采用光掩膜和湿法刻蚀技术在上片(1)加工“工”字形通道,微通道(3)宽度为100微米,深度30微米。用1.7毫米的金刚石钻头分别在“工”字形通道的端部垂直于芯片钻孔(4)、(5)。采用经典的高温键合的方法实现上(1)、下(2)两片的永久封合。得到长度、宽度分别为30毫米、20毫米的微流控芯片。接近“工”字形上横通道2.5毫米位置处,用金刚石玻璃刀垂直于芯片、平行于横向通道,切割得到“T”形通道芯片。平行于横向通道的面用细砂纸研磨抛光,得到透明的平面(8),以便光源直接照射。采用0.35毫米钻头在芯片上钻孔的方法,在T字形通道的出口通道得到直径约390微米的芯片接口(6)。所接的波导管(7)为5.5厘米长。将内径0.5mm聚四氟乙烯管粘接于微流控芯片的进出口(4)、(5)处,使芯片和外部进样设备相连。Fig. 1 is a structural diagram of a microfluidic chip coupled with a liquid core waveguide manufactured according to a preferred embodiment of the present invention. The microfluidic chip is composed of upper (1) and lower (2) glass sheets, and the thickness of the glass sheets is 1.7 mm. A photomask and a wet etching technique are used to process an "I"-shaped channel on the upper sheet (1), and the microchannel (3) has a width of 100 microns and a depth of 30 microns. Use a 1.7 mm diamond drill bit to drill holes (4), (5) perpendicular to the chip at the end of the "I" shaped channel respectively. The classic high-temperature bonding method is used to realize the permanent sealing of the upper (1) and lower (2) pieces. A microfluidic chip with a length and a width of 30 mm and 20 mm, respectively, was obtained. Close to the position of 2.5mm on the upper transverse channel of the "I" shape, use a diamond glass knife to cut perpendicular to the chip and parallel to the transverse channel to obtain a "T" shaped channel chip. The surface parallel to the transverse channel is ground and polished with fine sandpaper to obtain a transparent plane (8) so that the light source is directly irradiated. A 0.35 mm drill bit is used to drill holes on the chip, and a chip interface (6) with a diameter of about 390 microns is obtained in the outlet channel of the T-shaped channel. The connected waveguide (7) is 5.5 centimeters long. Bond the polytetrafluoroethylene tube with an inner diameter of 0.5 mm to the inlet and outlet (4) and (5) of the microfluidic chip, so as to connect the chip with the external sampling device.
图2是液芯波导管与微流控芯片耦合接口的局部放大图。采用Teflon AF1600液芯波导管(7)外径375微米,内径为50微米。用黑色油漆笔(ZEBRA,Japan)在洁净的玻璃表面挤出一小滴油漆液,将液芯波导管的一端接泵管泵气,防止中间通道进漆;另一端垂直在油漆小液滴中浸一下,快速拿起,泵气直至漆干为止。用较干的油漆笔在波导管侧壁涂上一薄层均匀的油漆(11),油漆厚约5~10微米。得到的液芯波导管端部外径略小于390微米。将Teflon液芯波导管涂漆端小心的插入,液芯波导管端部与接口底部紧密接合。用环氧树脂胶(14)固定波导管。为了在芯片上集成发光二极管光源,如图2所示在接近微流控芯片通道与波导光接口处用金刚钻透(1)、(2)玻璃片,用锉刀研磨,然后用细砂纸抛光,得到一个方形框(15)用于嵌入集成发光二极管光源。Fig. 2 is a partially enlarged view of the coupling interface between the liquid core waveguide and the microfluidic chip. A Teflon AF1600 liquid core waveguide (7) has an outer diameter of 375 microns and an inner diameter of 50 microns. Use a black paint pen (ZEBRA, Japan) to squeeze out a small drop of paint liquid on the clean glass surface, connect one end of the liquid core waveguide to the pump tube to pump air to prevent the middle channel from entering the paint; the other end is vertically placed in the small paint droplet Give it a dip, pick it up quickly, and pump until the paint is dry. Apply a thin layer of uniform paint (11) on the side wall of the waveguide with a relatively dry paint pen, and the thickness of the paint is about 5-10 microns. The outer diameter of the resulting liquid-core waveguide tip is slightly less than 390 microns. Carefully insert the painted end of the Teflon liquid-core waveguide, and the end of the liquid-core waveguide is tightly bonded to the bottom of the interface. Fix the waveguide with epoxy glue (14). In order to integrate light-emitting diode light sources on the chip, as shown in Figure 2, use diamond drills to penetrate (1) and (2) glass sheets near the interface between the microfluidic chip channel and the waveguide light, grind them with a file, and then polish them with fine sandpaper to obtain A square frame (15) is used to embed the integrated LED light source.
图3是一种外覆Teflon AF膜(9)的石英液芯波导管吸收池光路示意图。Teflon AF膜(9)的折射率为1.29,通道中水溶液(10)的折射率为1.3333,石英壁(8)折射率为1.51。波导管入口处用波导管的全反射条件均为入射角大于θ0=75.4°。沿通道轴向以小于15.6°入射角入射的光能在液芯波导管中全反射传播,当溶液中有吸光物质时,光被吸收,产生吸光度变化。从图3可以看出,当以15.6°入射角入射时,通过溶液的光程占总光程的三分之一左右。用纯Teflon AF毛细管或内壁全反射金属毛细管,可以使光程大于等于波导管的长度;采用石英壁很薄的波导管,以减少光在石英壁中传播光程的比例,也可以提高光程。Fig. 3 is a schematic diagram of the optical path of a quartz liquid core waveguide absorption cell coated with a Teflon AF film (9). The refractive index of the Teflon AF film (9) is 1.29, the refractive index of the aqueous solution (10) in the channel is 1.3333, and the refractive index of the quartz wall (8) is 1.51. The total reflection condition of the waveguide used at the entrance of the waveguide is that the incident angle is greater than θ 0 =75.4°. Light incident along the axis of the channel at an incident angle of less than 15.6° propagates through total reflection in the liquid core waveguide. When there is a light-absorbing substance in the solution, the light is absorbed, resulting in a change in absorbance. It can be seen from Figure 3 that when the incident angle is 15.6°, the optical path through the solution accounts for about one-third of the total optical path. Using pure Teflon AF capillary or total reflection metal capillary on the inner wall can make the optical path greater than or equal to the length of the waveguide; using a waveguide with a very thin quartz wall can reduce the proportion of the optical path of light propagating in the quartz wall, and can also increase the optical path. .
图4对比了图3的波导管在没有进行遮光处理和进行了遮光处理的不同的效果。A1、A2、B1、B2均为Teflon液芯波导管检测端CCD显微拍照实图。光源为505纳米的发光二极管。A1、A2为入射端面没有涂油漆的光分布图。B1、B2为入射端进行了图4所示的遮光处理的光分布图。其中A1、B1注射0.2mM邻菲啰啉-铁(II)显色溶液,A2、B2注射空白邻菲啰啉溶液。可以看到,没有进行遮光处理时,溶液变化对总光量的变化贡献不大,因为大部分光是通过石英壁中传播。进行遮光处理后,通道中心变化更加明显。证明遮光处理有助于降低背景,提高系统的检测灵敏度。FIG. 4 compares the different effects of the waveguide in FIG. 3 without light-shielding treatment and with light-shielding treatment. A1, A2, B1, and B2 are real microscopic pictures taken by the CCD at the detection end of the Teflon liquid core waveguide. The light source is a 505 nm light emitting diode. A1 and A2 are light distribution diagrams without paint on the incident end surface. B1 and B2 are light distribution diagrams in which the light-shielding treatment shown in FIG. 4 is performed on the incident end. Among them, A1 and B1 were injected with 0.2mM o-phenanthroline-iron(II) chromogenic solution, and A2 and B2 were injected with blank o-phenanthroline solution. It can be seen that when no shading treatment is performed, the solution change does not contribute much to the change of the total light quantity, because most of the light is transmitted through the quartz wall. After shading treatment, the change of the channel center is more obvious. It is proved that the shading treatment helps to reduce the background and improve the detection sensitivity of the system.
图5为液芯波导管检测端口设计。液芯波导管出口由一外径大于液芯波导管的单芯光纤(17),由光纤将光导入光电倍增管检测。检测端口同时也是检测溶液出口,我们设计了一个稀释液池(16),保持出口检测处的环境稳定。也可以采用其他方法进行检测,如采用光电二极管,对准液芯波导管出口直接检测,这样将大大简化系统,实现整体的小型化。Figure 5 shows the design of the liquid core waveguide detection port. A single-core optical fiber (17) with an outer diameter larger than that of the liquid-core waveguide is used at the exit of the liquid-core waveguide, and the light is guided into a photomultiplier tube by the optical fiber for detection. The detection port is also the outlet of the detection solution, and we have designed a diluent pool (16) to keep the environment at the detection outlet stable. Other methods can also be used for detection, such as using a photodiode to directly detect the outlet of the liquid core waveguide, which will greatly simplify the system and achieve overall miniaturization.
图6显示安装有图3实施例装置的微芯片分析系统对不同浓度铁(II)-邻菲啰啉配合物检测的结果记录图。采用以上图1微流控芯片耦合液芯波导管系统装置,及505纳米的发光二极管作光源,光电倍增管和微光测量仪作为检测器,检测邻菲啰啉-铁(II)混合显色溶液。T形通道芯片的两个通道分别交替注射Fe(II)标准系列溶液(一个数量级五个溶液)和空白液。Fig. 6 shows the record diagram of the detection results of different concentrations of iron (II)-o-phenanthroline complexes by the microchip analysis system equipped with the device of the embodiment in Fig. 3 . Using the microfluidic chip coupling liquid core waveguide system device in Figure 1 above, and a 505-nm light-emitting diode as a light source, a photomultiplier tube and a low-light measuring instrument as a detector, detect the mixed color of o-phenanthroline-iron (II) solution. The two channels of the T-shaped channel chip are alternately injected with Fe(II) standard series solutions (five solutions in one order of magnitude) and blank solutions.
图7显示安装有图3实施例装置的微芯片分析系统对不同浓度铁(II)-邻菲啰啉配合物检测的标准曲线以及在分光光度计平行测定的标准曲线图。检测范围2.0~10微摩尔/升标准溶液。曲线方程为y=0.0184x+0.0056,R2=0.9991;在分光光度计上平行实验测得的曲线方程为y=0.011x-0.0028,R2=0.9994。检测吸光度超过分光光度计,但没有达到理论计算的最低值。检测灵敏度同时受到光源单色性,遮光层的遮光不完全等的影响。Fig. 7 shows the standard curve of the detection of different concentrations of iron (II)-o-phenanthroline complexes by the microchip analysis system equipped with the device of the embodiment of Fig. 3 and the standard curve of the parallel determination in the spectrophotometer. The detection range is 2.0-10 micromole/liter standard solution. The curve equation is y=0.0184x+0.0056, R2=0.9991; the curve equation measured in parallel experiments on the spectrophotometer is y=0.011x-0.0028, R2=0.9994. The detected absorbance exceeds the spectrophotometer, but does not reach the minimum value of theoretical calculation. The detection sensitivity is also affected by the monochromaticity of the light source and the incomplete shading of the shading layer.
图8为一种通过内部全反射进行液芯波导的吸收池光路示意图。全反射管壁可以是低折射率透明物质或者高反射率的非透明物质表面。Fig. 8 is a schematic diagram of an optical path of an absorption cell for liquid core waveguide through internal total reflection. The total reflection tube wall can be a transparent material with a low refractive index or a non-transparent material surface with a high reflectivity.
图9为采用图8结构的一个实施例,全TeflonAF液芯波导管吸收池,管长6.3厘米,对铁(II)-邻菲啰啉配合物检测的标准曲线以及在分光光度计平行测定的标准曲线图。检测范围2.0~10微摩尔/升标准溶液。曲线方程为y=0.0514x+0.0135,R2=0.9995,在分光光度计上平行实验测得的曲线方程为y=0.0117x-0.0123,R2=0.9992。Fig. 9 is an embodiment adopting the structure of Fig. 8, full TeflonAF liquid core waveguide absorption cell, tube length 6.3 centimeters, to the standard curve that iron (II)-o-phenanthroline complex detects and parallel determination in spectrophotometer Standard Curve Chart. The detection range is 2.0-10 micromole/liter standard solution. The curve equation is y=0.0514x+0.0135, R 2 =0.9995, and the curve equation measured in parallel experiments on the spectrophotometer is y=0.0117x-0.0123, R 2 =0.9992.
图10为采用图8结构的另一个实施例,内镀银液芯波导管的吸收池,对铁(II)-邻菲啰啉配合物检测的结果记录图。采用3cm吸收池,其吸光度可达到分光光度计的3.7~4倍。Fig. 10 is another embodiment adopting the structure of Fig. 8, the absorption cell of the inner silver-plated liquid core waveguide, and the record diagram of the detection results of iron (II)-o-phenanthroline complex. Using a 3cm absorption cell, its absorbance can reach 3.7 to 4 times that of a spectrophotometer.
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CN102486456A (en) * | 2010-12-03 | 2012-06-06 | 鲍元进 | Liquid core waveguide detection device |
CN102954938A (en) * | 2011-08-29 | 2013-03-06 | 中国科学院电子学研究所 | Absorption luminosity detecting sensor based on micro-fluid control channel full-reflection integration light waveguide |
CN102954938B (en) * | 2011-08-29 | 2014-08-27 | 中国科学院电子学研究所 | Absorption luminosity detecting sensor based on micro-fluid control channel full-reflection integration light waveguide |
CN102539361A (en) * | 2012-01-10 | 2012-07-04 | 浙江大学 | Long-path optical fiber-microfluidic chip sensor for detecting absorbance and refraction index |
CN102539361B (en) * | 2012-01-10 | 2014-07-23 | 浙江大学 | Long-path optical fiber-microfluidic chip sensor for detecting absorbance and refraction index |
CN103630638A (en) * | 2012-08-21 | 2014-03-12 | 株式会社岛津制作所 | Flow cell |
CN103630638B (en) * | 2012-08-21 | 2015-06-24 | 株式会社岛津制作所 | Flow cell |
CN105092492A (en) * | 2014-05-06 | 2015-11-25 | 黄辉 | Light guide capillary-based photometric analyzer and detection method thereof |
CN105575842A (en) * | 2015-12-20 | 2016-05-11 | 合肥艾斯克光电科技有限责任公司 | Testing method for LED packaging adhesive |
CN105642508A (en) * | 2015-12-20 | 2016-06-08 | 合肥艾斯克光电科技有限责任公司 | LED glue injecting and testing all-in-one machine |
CN109001168A (en) * | 2018-03-27 | 2018-12-14 | 黄辉 | A kind of light-conducting capillaries photometer |
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