[go: up one dir, main page]

CN107389502B - A method and system for measuring liquid viscosity - Google Patents

A method and system for measuring liquid viscosity Download PDF

Info

Publication number
CN107389502B
CN107389502B CN201710563487.8A CN201710563487A CN107389502B CN 107389502 B CN107389502 B CN 107389502B CN 201710563487 A CN201710563487 A CN 201710563487A CN 107389502 B CN107389502 B CN 107389502B
Authority
CN
China
Prior art keywords
liquid
group
channel
experiment
slope
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201710563487.8A
Other languages
Chinese (zh)
Other versions
CN107389502A (en
Inventor
曹炳阳
杨敏
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tsinghua University
Original Assignee
Tsinghua University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tsinghua University filed Critical Tsinghua University
Priority to CN201710563487.8A priority Critical patent/CN107389502B/en
Publication of CN107389502A publication Critical patent/CN107389502A/en
Application granted granted Critical
Publication of CN107389502B publication Critical patent/CN107389502B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N11/00Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties
    • G01N11/02Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material
    • G01N11/04Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material through a restricted passage, e.g. tube, aperture
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N11/00Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties
    • G01N11/02Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material
    • G01N11/04Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material through a restricted passage, e.g. tube, aperture
    • G01N11/06Investigating flow properties of materials, e.g. viscosity, plasticity; Analysing materials by determining flow properties by measuring flow of the material through a restricted passage, e.g. tube, aperture by timing the outflow of a known quantity

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Automatic Analysis And Handling Materials Therefor (AREA)
  • Measuring Volume Flow (AREA)

Abstract

本发明公开一种测量液体粘度的方法及系统。该方法包括:建立液体在微/纳通道中做毛细流动时流动长度与时间的实际关系模型;确定液体动力粘度与实际拟合斜率之间的关系模型:确定未知参数的值,确定液体动力粘度与实际拟合斜率之间的关系模型的表达式;根据液体实际毛细流动过程的拟合斜率,确定所述液体的动力粘度。采用本发明的方法或系统,通过拟合斜率可以直接确定动力粘度,而且所需液体量极少,测量准确。

The invention discloses a method and system for measuring liquid viscosity. The method includes: establishing the actual relationship model of the flow length and time when the liquid is in capillary flow in the micro/nano channel; determining the relationship model between the dynamic viscosity of the liquid and the actual fitting slope: Determine the value of the unknown parameter, determine the expression of the relationship model between the dynamic viscosity of the liquid and the actual fitting slope; determine the dynamic viscosity of the liquid according to the fitting slope of the actual capillary flow process of the liquid. Using the method or system of the present invention, the dynamic viscosity can be directly determined by fitting the slope, and the required liquid amount is very small, and the measurement is accurate.

Description

一种测量液体粘度的方法及系统A method and system for measuring liquid viscosity

技术领域technical field

本发明涉及液体测量领域,特别是涉及一种测量液体粘度的方法及系统。The present invention relates to the field of liquid measurement, in particular to a method and system for measuring liquid viscosity.

背景技术Background technique

粘度是表征液体性质的重要物理量之一,反映了液体抵抗变形的能力。粘度的准确测量对于石油化工、医学、国防等领域有着重要的意义。现有的粘度测量方法主要是毛细管法。由于毛细管法简单实用,因此目前基于毛细管法设计的测量装置的应用范围较广。毛细管法的原理是哈根-泊肃叶公式,通过外部压力驱动液体流过毛细管,测出毛细管两端的压差和液体的流量,并加以修正,就可以计算得到液体的粘度。目前基于毛细管法测量粘度的装置存在的主要问题有:压差、流量的精确测量较为困难,另外测量所需要的实验液体较多(测量装置中毛细管内径一般为mm量级,所需实验液体在几十毫升),但有时所能提供的实验液体却非常有限(例如血液或者某些生理液体样品一般为几十微升),如果此时仍然用毛细管法进行测量,则测量结果准确度很低,甚至可能无法实现液体粘度的测量,这些都给毛细管法测量技术的发展带来了挑战。Viscosity is one of the important physical quantities that characterize the properties of liquids, reflecting the ability of liquids to resist deformation. Accurate measurement of viscosity is of great significance to petrochemical, medical, national defense and other fields. The existing viscosity measurement method is mainly the capillary method. Because the capillary tube method is simple and practical, the current measuring devices designed based on the capillary tube method have a wide range of applications. The principle of the capillary tube method is the Hagen-Poiseuille formula. The liquid is driven by external pressure to flow through the capillary tube, the pressure difference at both ends of the capillary tube and the flow rate of the liquid are measured and corrected, and the viscosity of the liquid can be calculated. At present, the main problems of the device for measuring viscosity based on the capillary method are: it is difficult to accurately measure the pressure difference and flow rate, and more experimental liquids are required for the measurement (the inner diameter of the capillary tube in the measuring device is generally of the order of mm, and the required experimental liquid is in the tens of milliliters), but sometimes the experimental liquid that can be provided is very limited (for example, blood or some physiological fluid samples are generally tens of microliters). If the capillary method is still used for measurement at this time, the accuracy of the measurement results is very low , and may not even be able to measure the viscosity of liquids, all of which bring challenges to the development of capillary measurement technology.

发明内容SUMMARY OF THE INVENTION

本发明的目的是提供一种测量液体粘度的方法及系统,通过极少的液体实现液体粘度的测量,提高测量的准确性。The purpose of the present invention is to provide a method and a system for measuring the viscosity of a liquid, which can measure the viscosity of the liquid with very little liquid and improve the accuracy of the measurement.

为实现上述目的,本发明提供了如下方案:For achieving the above object, the present invention provides the following scheme:

一种测量液体粘度的方法,所述方法包括:A method of measuring the viscosity of a liquid, the method comprising:

建立液体流动长度与时间的实际关系模型:Model the actual relationship between liquid flow length and time:

其中a和b为与通道深度有关的未知参数,Aexp为实际的拟合斜率,l(t)表示t时刻液体的流动距离,σ表示液体表面张力,θe表示液体与通道壁间的平衡接触角,η表示液体动力粘度,h表示通道高度; where a and b are unknown parameters related to the channel depth, A exp is the actual fitting slope, l(t) is the flow distance of the liquid at time t, σ is the surface tension of the liquid, and θ e is the equilibrium between the liquid and the channel wall contact angle, η is the fluid dynamic viscosity, h is the channel height;

确定液体动力粘度与实际拟合斜率之间的关系模型:Determine the relationship between the hydrodynamic viscosity and the actual fitted slope:

确定未知参数a和b的值,确定所述关系模型 Determine the values of the unknown parameters a and b, determine the relationship model

根据液体流动的实际的拟合斜率,确定所述液体的动力粘度。From the actual fitted slope of the liquid flow, the dynamic viscosity of the liquid is determined.

可选的,所述确定未知参数a和b的值,具体包括:Optionally, the determining the values of the unknown parameters a and b specifically includes:

利用N种已知液体对应进行N组实验,N为大于1的整数;Use N kinds of known liquids to carry out N groups of experiments, where N is an integer greater than 1;

根据公式获取N组实验中的每组实验的拟合斜率AexpAccording to the formula Obtain the fitting slope A exp of each group of experiments in the N groups of experiments;

根据公式获取N组实验中的每组实验的理论斜率ALWAccording to the formula Obtain the theoretical slope ALW of each group of experiments in the N groups of experiments;

获取N组实验中的每组实验的拟合斜率和对应理论斜率的比值,得到:其中Aexp(k)表示第k组实验得到的拟合斜率,k=1,2,……N,ALW(k)表示第k组实验对应的理论斜率,σ(k)表示第k组实验中液体表面张力,θe(k)表示第k组实验中液体与通道壁间的平衡接触角,η(k)表示第k组实验中液体动力粘度的理论值;Obtain the ratio of the fitted slope and the corresponding theoretical slope of each group of experiments in the N groups of experiments, and get: where A exp(k) represents the fitting slope obtained from the kth group of experiments, k=1, 2,...N, A LW(k) represents the theoretical slope corresponding to the kth group of experiments, and σ (k) represents the kth group of experiments The surface tension of the liquid in the experiment, θ e(k) represents the equilibrium contact angle between the liquid and the channel wall in the k-th group of experiments, η (k) represents the theoretical value of the dynamic viscosity of the liquid in the k-th group of experiments;

根据所述N组实验的已知液体的相关参数,获得每组实验已知液体对应的参数,其中所述相关参数包括液体表面张力σ(k)、液体与通道壁间的平衡接触角θe(k)、液体动力粘度的理论值η(k)According to the relevant parameters of the known liquids in the N groups of experiments, the corresponding parameters of the known liquids in each group of experiments are obtained. parameters, wherein the relevant parameters include the liquid surface tension σ (k) , the equilibrium contact angle θ e(k) between the liquid and the channel wall, and the theoretical value of the liquid dynamic viscosity η (k) ;

确定所述a和所述b的值。Determine the values of the a and the b.

可选的,所述确定所述a和b的值之后,还包括:Optionally, after determining the values of a and b, the method further includes:

获得M组不同深度的通道对应的液体流动过程中流动长度与时间的关系模型中的未知参数a(i)和b(i)的值,其中M为大于1的整数,其中a(i)和b(i)为与通道深度h(i)有关的未知参数,通道深度h(i)为通道i的深度;Obtain the relationship model of flow length and time in the liquid flow process corresponding to M groups of channels with different depths The values of the unknown parameters a (i) and b (i) in , where M is an integer greater than 1, where a (i) and b (i) are unknown parameters related to the channel depth h (i) , the channel depth h (i) is the depth of channel i;

确定通道深度h与未知参数a、b之间的关系函数h=f(a,b)以及未知参数a和b之间的关系函数a=g(b)。The relationship function h=f(a,b) between the channel depth h and the unknown parameters a, b and the relationship function a=g(b) between the unknown parameters a and b are determined.

一种测量液体粘度的系统,所述系统包括:A system for measuring the viscosity of a liquid, the system comprising:

流动长度与时间的关系模型建立模块,用于建立液体流动长度与时间的实际关系模型:其中a和b为与通道深度有关的未知参数,Aexp为实际的拟合斜率,l(t)表示t时刻液体的流动距离,σ表示液体表面张力,θe表示液体与通道壁间的平衡接触角,η表示液体动力粘度,h表示通道高度;The relationship model building module of flow length and time is used to establish the actual relationship model of liquid flow length and time: where a and b are unknown parameters related to the channel depth, A exp is the actual fitting slope, l(t) is the flow distance of the liquid at time t, σ is the surface tension of the liquid, and θ e is the equilibrium between the liquid and the channel wall contact angle, η is the fluid dynamic viscosity, h is the channel height;

液体动力粘度与实际拟合斜率关系模型确定模块,用于确定液体动力粘度与实际拟合斜率之间的关系模型: The model determination module for the relationship between hydrodynamic viscosity and actual fitting slope is used to determine the relationship model between hydrodynamic viscosity and actual fitting slope:

未知参数确定模块,用于确定未知参数a和b的值,确定所述关系模型 an unknown parameter determination module for determining the values of the unknown parameters a and b to determine the relationship model

动力粘度确定模块,用于根据液体流动的实际的拟合斜率,确定所述液体的动力粘度。The dynamic viscosity determination module is used for determining the dynamic viscosity of the liquid according to the actual fitting slope of the liquid flow.

可选的,所述未知参数确定模块,具体包括:Optionally, the unknown parameter determination module specifically includes:

实验控制单元,用于利用N种已知液体对应进行N组实验,N为大于1的整数;An experiment control unit, used to perform N groups of experiments using N kinds of known liquids, where N is an integer greater than 1;

拟合斜率获取模块,用于根据公式获取N组实验中的每组实验的拟合斜率AexpFitting slope acquisition module, which is used according to the formula Obtain the fitting slope A exp of each group of experiments in the N groups of experiments;

理论斜率获取单元,用于根据公式获取N组实验中的每组实验的理论斜率ALWTheoretical slope acquisition unit, which is used according to the formula Obtain the theoretical slope ALW of each group of experiments in the N groups of experiments;

比值计算单元,用于计算N组实验中的每组实验的拟合斜率和对应理论斜率的比值,得到:其中Aexp(k)表示第k组实验得到的拟合斜率,k=1,2,……N,ALW(k)表示第k组实验对应的理论斜率,σ(k)表示第k组实验中液体表面张力,θe(k)表示第k组实验中液体与通道壁间的平衡接触角,η(k)表示第k组实验中液体动力粘度的理论值;The ratio calculation unit is used to calculate the ratio of the fitted slope of each group of experiments in the N groups of experiments to the corresponding theoretical slope, and obtain: where A exp(k) represents the fitting slope obtained from the kth group of experiments, k=1, 2,...N, A LW(k) represents the theoretical slope corresponding to the kth group of experiments, and σ (k) represents the kth group of experiments The surface tension of the liquid in the experiment, θ e(k) represents the equilibrium contact angle between the liquid and the channel wall in the k-th group of experiments, η (k) represents the theoretical value of the dynamic viscosity of the liquid in the k-th group of experiments;

液体参数计算单元,用于根据所述N组实验的已知液体的相关参数,获得每组实验已知液体对应的参数,其中所述相关参数包括液体表面张力σ(k)、液体与通道壁间的平衡接触角θe(k)、液体动力粘度的理论值η(k)The liquid parameter calculation unit is used to obtain the corresponding parameters of the known liquid in each group of experiments according to the relevant parameters of the known liquid in the N groups of experiments parameters, wherein the relevant parameters include the liquid surface tension σ (k) , the equilibrium contact angle θ e(k) between the liquid and the channel wall, and the theoretical value of the liquid dynamic viscosity η (k) ;

未知参数确定单元,用于确定所述a和b的值。An unknown parameter determination unit for determining the values of a and b.

可选的,所述系统还包括:Optionally, the system further includes:

不同深度通道对应的未知参数确定模块,用于确定所述a和b的值之后,获得M组不同深度的通道对应的液体流动过程中流动长度与时间的关系模型中的未知参数a(i)和b(i)的值,其中M为大于1的整数,a(i)和b(i)为与通道深度h(i)有关的未知参数,通道深度h(i)为通道i的深度;The unknown parameter determination module corresponding to the channels of different depths is used to obtain the relationship model between the flow length and time in the liquid flow process corresponding to the M groups of channels of different depths after determining the values of a and b The values of the unknown parameters a (i) and b (i) in , where M is an integer greater than 1, a (i) and b (i) are unknown parameters related to the channel depth h (i) , and the channel depth h ( i) is the depth of channel i;

关系函数确定模块,用于确定通道深度h与未知参数a、b之间的关系函数h=f(a,b)以及未知参数a和b之间的关系函数a=g(b)。The relationship function determination module is used to determine the relationship function h=f(a,b) between the channel depth h and the unknown parameters a and b and the relationship function a=g(b) between the unknown parameters a and b.

一种测量液体粘度的装置,所述装置包括:电源、进样装置、微米/纳米通道、温控装置、控制器、数据采集装置;A device for measuring liquid viscosity, the device comprising: a power supply, a sample introduction device, a micro/nano channel, a temperature control device, a controller, and a data acquisition device;

所述电源连接所述进样装置;所述进样装置的输出端与所述微米/纳米通道的入口连接,所述微米/纳米通道的出口直通大气;the power supply is connected to the sampling device; the output end of the sampling device is connected to the inlet of the micro/nano channel, and the outlet of the micro/nano channel is directly connected to the atmosphere;

所述控制器的第一输出端连接所述进样装置的输入端;所述控制器的第二输出端连接所述温控装置的输入端;所述微米/纳米通道位于所述温控装置内部;The first output end of the controller is connected to the input end of the sampling device; the second output end of the controller is connected to the input end of the temperature control device; the micro/nano channel is located in the temperature control device internal;

所述数据采集装置用于采集液体的流动距离和时间;The data collection device is used to collect the flow distance and time of the liquid;

所述控制器的输入端连接所述数据采集装置,用于根据所述数据采集装置采集的液体距离和时间,利用液体的流动长度与时间的关系模型The input end of the controller is connected to the data acquisition device, and is used for using the relationship model between the flow length of the liquid and the time according to the distance and time of the liquid collected by the data acquisition device

获得实际的拟合斜率Aexp,还用于结合液体流动长度与时间的理论关系式确定未知参数a和b的值,确定液体动力粘度与实际拟合斜率之间的关系模型根据液体流动的实际的拟合斜率,确定所述液体的动力粘度,其中l(t)表示t时刻液体的流动距离,σ表示液体表面张力,η表示液体动力粘度,h表示通道高度,θe表示液体与通道壁间的平衡接触角,a和b为与通道深度有关的未知参数。 Obtain the actual fitted slope A exp , which is also used to combine the theoretical relationship between liquid flow length and time Determine the values of the unknown parameters a and b, and determine the relationship model between the hydrodynamic viscosity and the actual fitted slope According to the actual fitting slope of the liquid flow, determine the dynamic viscosity of the liquid, where l(t) represents the flow distance of the liquid at time t, σ represents the surface tension of the liquid, η represents the dynamic viscosity of the liquid, h represents the channel height, θ e represents the equilibrium contact angle between the liquid and the channel wall, a and b are unknown parameters related to the channel depth.

可选的,所述数据采集装置具体包括:E组光电组件、计时电路、第一数据处理装置;其中E为大于2的整数;Optionally, the data acquisition device specifically includes: a group E of photoelectric components, a timing circuit, and a first data processing device; wherein E is an integer greater than 2;

每组光电组件包括一个光发射器和一个光接收器,所述E组光电组件的E个光发射器依次位于所述微米/纳米通道的下方,所述E组光电组件的E个光接收器依次位于所述微米/纳米通道的上方,与所述E个光发射器对应设置;Each group of optoelectronic components includes an optical transmitter and an optical receiver, the E optical emitters of the E group of optoelectronic components are sequentially located below the micro/nano channel, and the E optical receivers of the E group of optoelectronic components are sequentially positioned above the micro/nano channels, and are arranged corresponding to the E light emitters;

所述E组光电组件的E个光接收器与所述计时电路相连;E light receivers of the E group photoelectric components are connected to the timing circuit;

所述第一数据处理装置与所述计时电路的输出端连接,用于根据所述E组光电组件之间的距离和所述微米/纳米通道中液体到达每一组光电组件的时间,获得液体的E组流动距离和时间。The first data processing device is connected to the output end of the timing circuit, and is used to obtain liquid according to the distance between the E groups of optoelectronic components and the time when the liquid in the micro/nano channel reaches each group of optoelectronic components E group flow distance and time.

可选的,所述数据采集装置具体包括:F个光源、F个光电传感器、第二数据处理装置;其中F为大于2的整数;Optionally, the data acquisition device specifically includes: F light sources, F photoelectric sensors, and a second data processing device; wherein F is an integer greater than 2;

所述F个光源与所述F个光电传感器一一对应;所述F个光电传感器依次位于所述微米/纳米通道的上方,所述F个光源依次位于所述微米/纳米通道的下方,与所述F个光电传感器相对设置;The F light sources are in one-to-one correspondence with the F photoelectric sensors; the F photoelectric sensors are sequentially located above the micro/nano channel, the F light sources are sequentially located below the micro/nano channel, and The F photoelectric sensors are relatively arranged;

所述第二数据处理装置与所述F个光电传感器的输出端连接,用于根据所述F个光电传感器之间的距离和所述微米/纳米通道中液体到达每一个光电传感器的时间,获得液体的F组流动距离和时间。The second data processing device is connected to the output ends of the F photoelectric sensors, and is used to obtain the information according to the distance between the F photoelectric sensors and the time when the liquid in the micro/nano channel reaches each photoelectric sensor. Group F flow distance and time for liquids.

可选的,所述测量装置还包括:显示装置,所述显示装置的输入端连接所述控制器的第三输出端,用于显示所述控制器输出的液体的动力粘度数据。Optionally, the measuring device further includes: a display device, the input end of the display device is connected to the third output end of the controller, for displaying the dynamic viscosity data of the liquid output by the controller.

根据本发明提供的具体实施例,本发明公开了以下技术效果:According to the specific embodiments provided by the present invention, the present invention discloses the following technical effects:

利用微/纳米通道中液体流动距离与时间的关系,确定动力粘度与实际拟合斜率的关系模型,进而通过拟合斜率可以直接确定动力粘度,而且所需液体量极少,实现了对试验液体较少的情况的粘度测量,提高了测量的准确度,同时避免浪费大量液体。本发明的测量装置将深度为微米甚至纳米量级的通道作为毛细管来减少实验液体的使用,液体在毛细压力驱动下流入微米/纳米通道组,不需要外部加压装置,不需要压力测量部件;操作简单、便于携带,测量迅速、结果可靠。Using the relationship between the liquid flow distance and time in the micro/nano channel, the relationship model between the dynamic viscosity and the actual fitting slope is determined, and then the dynamic viscosity can be directly determined by the fitting slope, and the amount of liquid required is very small. Fewer cases of viscosity measurement, increasing the accuracy of the measurement while avoiding wasting large amounts of liquid. The measuring device of the present invention uses channels with a depth of micrometers or even nanometers as capillaries to reduce the use of experimental liquids, and the liquids flow into the micro/nano channel group driven by capillary pressure, and no external pressure device or pressure measuring components are required; Simple operation, easy to carry, fast measurement and reliable results.

附图说明Description of drawings

为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动性的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the accompanying drawings required in the embodiments will be briefly introduced below. Obviously, the drawings in the following description are only some of the present invention. In the embodiments, for those of ordinary skill in the art, other drawings can also be obtained according to these drawings without creative labor.

图1为本发明测量液体粘度的方法流程图;Fig. 1 is the flow chart of the method for measuring liquid viscosity of the present invention;

图2为本发明测量液体粘度的系统结构图;Fig. 2 is the system structure diagram of the present invention measuring liquid viscosity;

图3为本发明测量液体粘度的装置结构图;Fig. 3 is the device structure diagram of the present invention measuring liquid viscosity;

图4为数据采集装置实施方式一的结构图;4 is a structural diagram of Embodiment 1 of a data acquisition device;

图5为数据采集装置实施方式二的结构图。FIG. 5 is a structural diagram of Embodiment 2 of the data acquisition device.

具体实施方式Detailed ways

下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, but not all of the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative efforts shall fall within the protection scope of the present invention.

为使本发明的上述目的、特征和优点能够更加明显易懂,下面结合附图和具体实施方式对本发明作进一步详细的说明。In order to make the above objects, features and advantages of the present invention more clearly understood, the present invention will be described in further detail below with reference to the accompanying drawings and specific embodiments.

图1为本发明测量液体粘度的方法流程图。如图1所示,所述方法包括:Fig. 1 is the flow chart of the method for measuring liquid viscosity of the present invention. As shown in Figure 1, the method includes:

步骤101:建立液体流动长度与时间的实际关系模型。建立实际关系模型为:其中a和b为与通道深度有关的未知参数,即通道深度不同,则a、b的值不同,l(t)表示t时刻液体的流动距离,σ表示液体表面张力,η表示液体动力黏度,h表示通道高度,θe表示液体与通道壁间的平衡接触角,θd表示液体与通道壁间的动态接触角。Step 101: Establish a model of the actual relationship between liquid flow length and time. The actual relationship model is established as: where a and b are unknown parameters related to the channel depth, that is, the values of a and b are different if the channel depth is different, l(t) represents the flow distance of the liquid at time t, σ represents the surface tension of the liquid, η represents the dynamic viscosity of the liquid, h is the height of the channel, θ e is the equilibrium contact angle between the liquid and the channel wall, and θ d is the dynamic contact angle between the liquid and the channel wall.

对于深为h宽为w的矩形截面通道,不可压牛顿液体在微/纳通道中做毛细流动时,牛顿动力学方程为:For a rectangular channel with a depth h and a width w, when the incompressible Newtonian liquid is capillary flow in the micro/nano channel, the Newtonian kinetic equation is:

其中l(t)表示t时刻液体的流动距离,l′(t)表示l(t)的一阶导数,l″(t)表示l(t)的二阶导数,ρ表示液体密度,σ表示液体表面张力,θe表示液体与通道壁间的平衡接触角,η表示液体动力粘度,h表示通道高度,w表示通道宽度,g表示重力加速度。对于微米/纳米尺度通道,可以忽略惯性力项及重力项的影响,且在微米/纳米通道中通道深度远小于通道宽度(即h<<w),因此可以推导出液体流动长度与时间的理论关系式为:其中ALW为理论斜率,也就是当液体确定时,其相关的各个参数是确定的,利用理论关系式便可得到理论上的流动长度与时间的关系,此理论关系式是目前预测毛细流动过程的宏观理论模型,即为LW模型。对于某一深度h的通道,如果液体表面张力σ、液体与通道壁间的平衡接触角θe、液体动力粘度η在液体流动过程中保持不变,那么流动距离l(t)与成线性关系,也就是说,ALW是常数。观察该模型,如果知道了通道深度h,以及的相关参数(液体表面张力σ、液体与通道壁间的平衡接触角θe、液体动力粘度η),就可以利用该模型预测液体在微米/纳米通道中的速度,从而根据实验需求设计微/纳流控系统。基于该模型,大量学者进行了实验研究,主要得到了以下三点结论:1.定性分析结果表明,目前微米/纳米通道中毛细流动过程的流动趋势可以用已有宏观理论模型进行预测,即流动时流动距离l(t)与成线性关系;2.定量分析结果表明,目前的宏观理论预测模型不能很好的解释实验现象,实验中液体的流动速度普遍低于理论预测值,即实验结果的拟合斜率(Aexp)<理论斜率(ALW);3.并不能确定到底是什么原因导致了实验值与理论值之间的偏差。这也就说,目前的宏观理论模型无法准确预测微米/纳米通道中的毛细流动过程,也就无法准确地预测液体的动力粘度。因此,在实际应用时,需要基于理论关系式,建立新的模型,即本发明建立的新的模型,基于本发明建立的模型,可以准确地测量液体的动态粘度。where l(t) is the flow distance of the liquid at time t, l′(t) is the first derivative of l(t), l″(t) is the second derivative of l(t), ρ is the liquid density, and σ is the Liquid surface tension, θ e is the equilibrium contact angle between the liquid and the channel wall, η is the liquid dynamic viscosity, h is the channel height, w is the channel width, and g is the gravitational acceleration. For micro/nano-scale channels, the inertial force term can be ignored and the influence of the gravity term, and in the micro/nano channel, the channel depth is much smaller than the channel width (ie h<<w), so the theoretical relationship between the liquid flow length and time can be deduced as: where A LW is the theoretical slope, That is, when the liquid is determined, its related parameters are determined, and the theoretical relationship between the flow length and time can be obtained by using the theoretical relationship. This theoretical relationship is the current macroscopic theoretical model for predicting the capillary flow process, which is LW model. For a channel of a certain depth h, if the liquid surface tension σ, the equilibrium contact angle θ e between the liquid and the channel wall, and the liquid dynamic viscosity η remain unchanged during the liquid flow, then the flow distance l(t) is the same as A linear relationship, that is, A LW is a constant. Observing the model, if you know the channel depth h, and the related parameters (liquid surface tension σ, the equilibrium contact angle θ e between the liquid and the channel wall, the liquid dynamic viscosity η), you can use this model to predict the liquid in micro/nano. velocity in the channel, thereby designing the micro/nanofluidic system according to the experimental needs. Based on this model, a large number of scholars have carried out experimental studies, and mainly obtained the following three conclusions: 1. The qualitative analysis results show that the current flow trend of the capillary flow process in the micro/nano channel can be predicted by the existing macro theoretical model, that is, the flow When the flow distance l(t) and 2. The quantitative analysis results show that the current macroscopic theoretical prediction model cannot explain the experimental phenomenon well, and the flow velocity of the liquid in the experiment is generally lower than the theoretical prediction value, that is, the fitting slope of the experimental results (A exp ) < Theoretical slope (A LW ); 3. It is not certain what causes the deviation between the experimental value and the theoretical value. That is to say, the current macroscopic theoretical model cannot accurately predict the capillary flow process in the micro/nano channel, and therefore cannot accurately predict the dynamic viscosity of the liquid. Therefore, in practical application, it is necessary to establish a new model based on the theoretical relationship, that is, the new model established by the present invention. Based on the model established by the present invention, the dynamic viscosity of the liquid can be accurately measured.

步骤102:确定液体动力粘度与实际拟合斜率之间的关系模型。根据步骤103的实际关系模型,推导出液体动力粘度与实际拟合斜率之间的关系模型: Step 102: Determine the relationship model between the hydrodynamic viscosity and the actual fitting slope. According to the actual relationship model in step 103, the relationship model between the fluid dynamic viscosity and the actual fitting slope is derived:

步骤103:确定未知参数a和b的值,从而确定液体动力粘度与实际拟合斜率之间的关系模型的表达式。Step 103: Determine the values of the unknown parameters a and b, thereby determining the relationship model between the hydrodynamic viscosity and the actual fitting slope expression.

具体确定未知参数的过程为:The specific process of determining the unknown parameters is as follows:

利用N种已知液体对应进行N组实验,N为大于1的整数;Use N kinds of known liquids to carry out N groups of experiments, where N is an integer greater than 1;

根据公式获取N组实验中的每组实验的拟合斜率AexpAccording to the formula Obtain the fitting slope A exp of each group of experiments in the N groups of experiments;

根据公式获取N组实验中的每组实验的理论斜率ALWAccording to the formula Obtain the theoretical slope ALW of each group of experiments in the N groups of experiments;

获取N组实验中的每组实验的拟合斜率和对应理论斜率的比值,得到:其中Aexp(k)表示第k组实验得到的拟合斜率,k=1,2,……N,ALW(k)表示第k组实验对应的理论斜率,σ(k)表示第k组实验中液体表面张力,θe(k)表示第k组实验中液体与通道壁间的平衡接触角,η(k)表示第k组实验中液体动力粘度的理论值;Obtain the ratio of the fitted slope and the corresponding theoretical slope of each group of experiments in the N groups of experiments, and get: where A exp(k) represents the fitting slope obtained from the kth group of experiments, k=1, 2,...N, A LW(k) represents the theoretical slope corresponding to the kth group of experiments, and σ (k) represents the kth group of experiments The surface tension of the liquid in the experiment, θ e(k) represents the equilibrium contact angle between the liquid and the channel wall in the k-th group of experiments, η (k) represents the theoretical value of the dynamic viscosity of the liquid in the k-th group of experiments;

根据所述N组实验的已知液体的相关参数,获得每组实验已知液体对应的参数,其中所述相关参数包括液体表面张力σ(k)、液体与通道壁间的平衡接触角θe(k)、液体动力粘度的理论值η(k)According to the relevant parameters of the known liquids in the N groups of experiments, the corresponding parameters of the known liquids in each group of experiments are obtained. parameters, wherein the relevant parameters include the liquid surface tension σ (k) , the equilibrium contact angle θ e(k) between the liquid and the channel wall, and the theoretical value of the liquid dynamic viscosity η (k) ;

确定所述a和b的值。Determine the values of the a and b.

此过程为利用已知液体的各个已知参数(包括液体的动力粘度为已知,液体动力粘度的理论值是指已知液体的已知粘度)进行实验,从而确定模型未知参数,确定模型的表达式,进而可以在未知液体动力粘度的情况下,利用该模型确定液体的动力粘度。This process is to use the known parameters of the known liquid (including the dynamic viscosity of the liquid is known, and the theoretical value of the dynamic viscosity of the liquid refers to the known viscosity of the known liquid) to conduct experiments, so as to determine the unknown parameters of the model and determine the model. The expression of , and then the dynamic viscosity of the liquid can be determined by using this model when the dynamic viscosity of the liquid is unknown.

由于a和b为与通道相关的参数,因此,通道参数不变的情况下参数a和b的值是不变的,也就是对应的实际的拟合斜率和动力粘度的关系模型是固定的。此确定参数a和b值的方法更适用于通道数量少甚至只有一个时,通过液体实验得到参数a和b值,比较快捷。Since a and b are parameters related to the channel, the values of parameters a and b are unchanged when the channel parameters are unchanged, that is, the relationship between the corresponding actual fitting slope and dynamic viscosity. It is fixed. This method of determining the values of parameters a and b is more suitable for obtaining the values of parameters a and b through liquid experiments when the number of channels is small or even only one, which is relatively fast.

当通道参数发生变化时(通道高度h发生变化),则参数a和b发生变化,关系模型也由于参数a和b的变化而变化。因此,对于通道变化的情况,可以通过几组实验得出通道高度h与参数a和b的关系,那么在通道高度已知的情况下,无需再通过多组已知液体进行实验来确定参数a和b的值,可以直接根据通道高度h与参数a和b的关系确定参数a和b的的值,对应的模型则很容易确定。具体的确定通道高度h与参数a和b的关系的过程为:When the channel parameters change (the channel height h changes), the parameters a and b change, and the relationship model Also varies due to changes in parameters a and b. Therefore, in the case of channel changes, the relationship between the channel height h and the parameters a and b can be obtained through several sets of experiments, then when the channel height is known, there is no need to conduct experiments with multiple groups of known liquids to determine the parameter a. and b, the values of parameters a and b can be determined directly according to the relationship between the channel height h and the parameters a and b, and the corresponding model is easy to determine. The specific process of determining the relationship between the channel height h and the parameters a and b is:

获得M组不同深度的通道对应的液体流动过程中流动长度与时间的关系模型中的未知参数a(i)和b(i)的值,其中M为大于1的整数,a(i)和b(i)为与通道深度h(i)有关的未知参数,通道深度h(i)为通道i的深度;Obtain the relationship model of flow length and time in the liquid flow process corresponding to M groups of channels with different depths The values of the unknown parameters a (i) and b (i) in , where M is an integer greater than 1, a (i) and b (i) are unknown parameters related to the channel depth h (i) , and the channel depth h ( i) is the depth of channel i;

确定通道深度h与未知参数a、b之间的关系函数h=f(a,b)以及未知参数a和b之间的关系函数a=g(b)。The relationship function h=f(a,b) between the channel depth h and the unknown parameters a, b and the relationship function a=g(b) between the unknown parameters a and b are determined.

此确定参数a和b值的方法更适用于通道数量较多时,此时对每一通道进行液体实验确定参数a和b值需要耗费大量的时间和液体,效率较低,因此,通过有限个通道的液体实验确定参数a和b值之后,确定通道深度与参数a和b的关系函数,可以直接根据通道深度确定参数a和b的值,从而直接确定关系模型,可以大大节约时间,避免浪费,同时提高模型确定的效率。This method of determining the values of parameters a and b is more suitable for a large number of channels. At this time, it takes a lot of time and liquid to determine the values of parameters a and b by performing liquid experiments on each channel, and the efficiency is low. Therefore, through a limited number of channels After determining the values of parameters a and b in the liquid experiment, determine the relationship function between the channel depth and parameters a and b, you can directly determine the values of parameters a and b according to the channel depth, so as to directly determine the relationship model, which can greatly save time and avoid waste, At the same time, the efficiency of model determination is improved.

步骤104:根据实际的拟合斜率确定液体的动力粘度。在通道壁面和液体确定的情况下,液体的相关参数是确定的,那么利用模型根据实际的拟合斜率,便可得到液体的动力粘度η。Step 104: Determine the dynamic viscosity of the liquid according to the actual fitting slope. In the case where the channel wall and the liquid are determined, the relevant parameters of the liquid are determined, then the model is used According to the actual fitting slope, the dynamic viscosity η of the liquid can be obtained.

图2为本发明测量液体粘度的系统结构图。如图2所示,所述系统包括:Fig. 2 is a system structure diagram of the present invention for measuring liquid viscosity. As shown in Figure 2, the system includes:

流动长度与时间的关系模型建立模块201,用于建立液体流动长度与时间的实际关系模型:其中a和b为与通道深度有关的未知参数,Aexp为实际的拟合斜率,l(t)表示t时刻液体的流动距离,σ表示液体表面张力,η表示液体动力黏度,h表示通道高度,θe表示液体与通道壁间的平衡接触角,θd表示液体与通道壁间的动态接触角;The relationship model establishment module 201 between the flow length and time is used to establish the actual relationship model between the liquid flow length and time: where a and b are unknown parameters related to the channel depth, A exp is the actual fitting slope, l(t) is the flow distance of the liquid at time t, σ is the liquid surface tension, η is the liquid dynamic viscosity, and h is the channel height , θ e represents the equilibrium contact angle between the liquid and the channel wall, θ d represents the dynamic contact angle between the liquid and the channel wall;

液体动力粘度与实际拟合斜率关系模型确定模块202,用于确定液体动力粘度与实际拟合斜率之间的关系模型: The relationship model determination module 202 between the hydrodynamic viscosity and the actual fitting slope is used to determine the relation model between the hydrodynamic viscosity and the actual fitting slope:

未知参数确定模块203,用于确定未知参数a和b的值,确定所述关系模型 The unknown parameter determination module 203 is used to determine the values of the unknown parameters a and b, and determine the relationship model

所述未知参数确定模块203,具体包括:The unknown parameter determination module 203 specifically includes:

实验控制单元,用于利用N种已知液体对应进行N组实验;N为大于1的整数;An experiment control unit, used to perform N groups of experiments using N kinds of known liquids; N is an integer greater than 1;

拟合斜率获取模块,用于根据公式获取N组实验中的每组实验的拟合斜率AexpFitting slope acquisition module, which is used according to the formula Obtain the fitting slope A exp of each group of experiments in the N groups of experiments;

理论斜率获取单元,用于根据公式获取N组实验中的每组实验的理论斜率ALWTheoretical slope acquisition unit, which is used according to the formula Obtain the theoretical slope ALW of each group of experiments in the N groups of experiments;

比值计算单元,用于计算N组实验中的每组实验的拟合斜率和对应理论斜率的比值,得到:其中Aexp(k)表示第k组实验得到的拟合斜率,k=1,2,……N,ALW(k)表示第k组实验对应的理论斜率,σ(k)表示第k组实验中液体表面张力,θe(k)表示第k组实验中液体与通道壁间的平衡接触角,η(k)表示第k组实验中液体动力粘度的理论值;The ratio calculation unit is used to calculate the ratio of the fitted slope of each group of experiments in the N groups of experiments to the corresponding theoretical slope, and obtain: where A exp(k) represents the fitting slope obtained from the kth group of experiments, k=1, 2,...N, A LW(k) represents the theoretical slope corresponding to the kth group of experiments, and σ (k) represents the kth group of experiments The surface tension of the liquid in the experiment, θ e(k) represents the equilibrium contact angle between the liquid and the channel wall in the k-th group of experiments, η (k) represents the theoretical value of the dynamic viscosity of the liquid in the k-th group of experiments;

液体参数计算单元,用于根据所述N组实验的已知液体的相关参数,获得每组实验已知液体对应的参数,其中所述相关参数包括液体表面张力σ(k)、液体与通道壁间的平衡接触角θe(k)、液体动力粘度的理论值η(k)The liquid parameter calculation unit is used to obtain the corresponding parameters of the known liquid in each group of experiments according to the relevant parameters of the known liquid in the N groups of experiments parameters, wherein the relevant parameters include the liquid surface tension σ (k) , the equilibrium contact angle θ e(k) between the liquid and the channel wall, and the theoretical value of the liquid dynamic viscosity η (k) ;

未知参数确定单元,用于确定所述a和b的值。An unknown parameter determination unit for determining the values of a and b.

动力粘度确定模块204,用于根据液体流动的实际的拟合斜率,确定所述液体的动力粘度。The kinematic viscosity determination module 204 is configured to determine the kinematic viscosity of the liquid according to the actual fitting slope of the liquid flow.

所述系统还包括:不同深度通道对应的未知参数确定模块,用于确定所述a和b的值之后,获得M组不同深度的通道对应的液体流动过程中流动长度与时间的关系模型中的未知参数a(i)和b(i)的值,其中M为大于1的整数,a(i)和b(i)为与通道深度h(i)有关的未知参数,通道深度h(i)为通道i的深度;The system further includes: a module for determining unknown parameters corresponding to channels of different depths, which is used to obtain a relationship model between flow length and time in the liquid flow process corresponding to M groups of channels with different depths after determining the values of a and b. The values of the unknown parameters a (i) and b (i) in , where M is an integer greater than 1, a (i) and b (i) are unknown parameters related to the channel depth h (i) , and the channel depth h ( i) is the depth of channel i;

关系函数确定模块,用于确定通道深度h与未知参数a、b之间的关系函数h=f(a,b)以及未知参数a和b之间的关系函数a=g(b)。The relationship function determination module is used to determine the relationship function h=f(a,b) between the channel depth h and the unknown parameters a and b and the relationship function a=g(b) between the unknown parameters a and b.

图3为本发明测量液体粘度的装置结构图。如图3所示,所述测量装置包括:电源301、进样装置302、微米/纳米通道303、温控装置304、控制器305、数据采集装置306、显示装置307。Fig. 3 is the structure diagram of the device for measuring liquid viscosity according to the present invention. As shown in FIG. 3 , the measurement device includes: a power supply 301 , a sample introduction device 302 , a micro/nano channel 303 , a temperature control device 304 , a controller 305 , a data acquisition device 306 , and a display device 307 .

电源301连接进样装置302;The power supply 301 is connected to the sampling device 302;

进样装置302的输出端与微米/纳米通道303的入口连接,微米/纳米通道303的出口直通大气;控制器305的第一输出端连接进样装置302的输入端;进样装置302是一个开放的系统,可以选择人工手动进样,也可以选择通过控制器305控制进样装置实现自动进样。The output end of the sampling device 302 is connected to the inlet of the micro/nano channel 303, and the outlet of the micro/nano channel 303 is directly connected to the atmosphere; the first output end of the controller 305 is connected to the input end of the sampling device 302; the sampling device 302 is a In an open system, manual injection can be selected, or automatic injection can be realized by controlling the injection device through the controller 305.

控制器305的第二输出端连接温控装置304的输入端;微米/纳米通道303位于温控装置内部;温控装置304用于根据控制器305的指令控制微米/纳米通道303的温度,从而控制内部液体的温度。由于微米/纳米通道303尺寸小,因此需要的液体量极少,当如此少量的液体进入微米/纳米通道303时,液体与通道壁面充分接触换热,液体温度会瞬间接近通道壁面温度,可近似认为液体温度等于壁面温度,可以达到控制液体温度的目的。The second output end of the controller 305 is connected to the input end of the temperature control device 304; the micro/nano channel 303 is located inside the temperature control device; the temperature control device 304 is used to control the temperature of the micro/nano channel 303 according to the instruction of the controller 305, thereby Controls the temperature of the liquid inside. Due to the small size of the micro/nano channel 303, the amount of liquid required is extremely small. When such a small amount of liquid enters the micro/nano channel 303, the liquid and the channel wall are fully contacted for heat exchange, and the liquid temperature will instantly approach the channel wall temperature, which can be approximated Considering that the liquid temperature is equal to the wall temperature, the purpose of controlling the liquid temperature can be achieved.

数据采集装置306用于采集液体的流动距离和时间;数据采集装置306可以采用两种结构:The data collection device 306 is used to collect the flow distance and time of the liquid; the data collection device 306 can adopt two structures:

(1)图4为数据采集装置实施方式一的结构图,如图4所示,数据采集装置包括:E组光电组件401,E为大于2的整数(图中依次并列的第一光电组件10、第二光电组件11、第三光电组件12、第四光电组件13、第五光电组件14、第六光电组件15)、计时电路402、第一数据处理装置403;每组光电组件401包括一个光发射器4011和一个光接收器4012,所述E组光电组件401的E个光发射器依次位于微米/纳米通道404的下方,所述E组光电组件401的E个光接收器4012依次位于所述微米/纳米通道的上方,与所述E个光发射器对应设置;所述E组光电组件401的E个光接收器4012与所述计时电路402相连;所述第一数据处理装置403与所述计时电路402的输出端连接,用于根据所述E组光电组件401之间的距离和所述微米/纳米通道404中液体到达每一组光电组件的时间,获得液体的E组流动距离和时间。具体实施时,相邻两组光电组件可以设置相距1μm—100μm。在测量过程中,液体在毛细力作用下流过微米/纳米通道404,当第一组光电组件10检测到微米/纳米通道404中的液体端面经过时,计时电路402记录下时间,同理,第二光电组件11、第三光电组件12、第四光电组件13、第五光电组件14、第六光电组件15分别在液体端面经过时计时电路402记录下时间,数据最终传输到第一数据处理装置403中,第一数据处理装置403根据记录时间与光电组件401之间的距离,获得液体的多组流动距离和时间。(1) FIG. 4 is a structural diagram of the first embodiment of the data acquisition device. As shown in FIG. 4 , the data acquisition device includes: an E group of photoelectric components 401 , where E is an integer greater than 2 (the first photoelectric components 10 are arranged in sequence in the figure). , the second optoelectronic component 11, the third optoelectronic component 12, the fourth optoelectronic component 13, the fifth optoelectronic component 14, the sixth optoelectronic component 15), the timing circuit 402, and the first data processing device 403; each group of optoelectronic components 401 includes a An optical transmitter 4011 and an optical receiver 4012, the E optical transmitters of the E group optoelectronic components 401 are located under the micro/nano channel 404 in turn, and the E optical receivers 4012 of the E group optoelectronic components 401 are located in sequence. The top of the micro/nano channel is arranged corresponding to the E light emitters; the E light receivers 4012 of the E group photoelectric components 401 are connected to the timing circuit 402 ; the first data processing device 403 It is connected to the output end of the timing circuit 402, and is used to obtain the E group flow of the liquid according to the distance between the E group photoelectric components 401 and the time when the liquid in the micro/nano channel 404 reaches each group of photoelectric components distance and time. In a specific implementation, two adjacent groups of optoelectronic components may be set at a distance of 1 μm to 100 μm. During the measurement process, the liquid flows through the micro/nano channel 404 under the action of capillary force. When the first group of optoelectronic components 10 detects the passage of the liquid end face in the micro/nano channel 404, the timing circuit 402 records the time. The second optoelectronic component 11, the third optoelectronic component 12, the fourth optoelectronic component 13, the fifth optoelectronic component 14, and the sixth optoelectronic component 15 respectively record the time when the liquid end face passes by the timing circuit 402, and the data is finally transmitted to the first data processing device In 403, the first data processing device 403 obtains multiple sets of flow distances and times of the liquid according to the distance between the recording time and the photoelectric component 401.

(2)图5为数据采集装置实施方式二的结构图。如图5所示,数据采集装置包括:F个光源501、F个光电传感器502(可以采用光电管)、第二数据处理装置503;F个光源501与所述F个光电传感器502一一对应;F为大于2的整数,所述F个光电传感器502依次位于微米/纳米通道504的上方,F个光源501依次位于所述微米/纳米通道504的下方,与所述F个光电传感器502相对设置;第二数据处理装置503与所述F个光电传感器502的输出端连接,用于根据所述F个光电传感器502之间的距离和所述微米/纳米通道504中液体到达每一个光电传感器的时间,获得液体的F组流动距离和时间。测量时,LED光源501发光,当液体流过时,挡住了光,光电管502接收不到光信号而发生变化,系统将这种光信号转变为电信号并记录,也就是自动记录液体流过的时刻。(2) FIG. 5 is a structural diagram of Embodiment 2 of the data acquisition device. As shown in FIG. 5 , the data acquisition device includes: F light sources 501 , F photoelectric sensors 502 (photocells can be used), and a second data processing device 503 ; the F light sources 501 correspond to the F photoelectric sensors 502 one-to-one ; F is an integer greater than 2, the F photosensors 502 are sequentially located above the micro/nano channel 504, and the F light sources 501 are sequentially located below the micro/nano channel 504, opposite to the F photosensors 502 Setting; the second data processing device 503 is connected to the output ends of the F photosensors 502 for reaching each photosensor according to the distance between the F photosensors 502 and the liquid in the micro/nano channel 504 time to obtain the flow distance and time of group F of the liquid. During measurement, the LED light source 501 emits light. When the liquid flows, the light is blocked, and the photocell 502 cannot receive the light signal and changes. The system converts this light signal into an electrical signal and records it, that is, automatically records the flow of the liquid. time.

控制器305的输入端连接数据采集装置306,用于根据数据采集装置306采集的液体距离和时间,利用液体的流动长度与时间的关系模型获得实际的拟合斜率Aexp,还用于结合液体流动长度与时间的理论关系式确定未知参数a和b的值,确定液体动力粘度与实际拟合斜率之间的关系模型根据液体流动的实际的拟合斜率,确定所述液体的动力粘度,其中l(t)表示t时刻液体的流动距离,σ表示液体表面张力,η表示液体动力粘度,h表示通道高度,θe表示液体与通道壁间的平衡接触角,a和b为与通道深度有关的未知参数。The input end of the controller 305 is connected to the data acquisition device 306, and is used for using the relationship model of the liquid flow length and time according to the liquid distance and time collected by the data acquisition device 306 Obtain the actual fitted slope A exp , which is also used to combine the theoretical relationship between liquid flow length and time Determine the values of the unknown parameters a and b, and determine the relationship model between the hydrodynamic viscosity and the actual fitted slope According to the actual fitting slope of the liquid flow, determine the dynamic viscosity of the liquid, where l(t) represents the flow distance of the liquid at time t, σ represents the surface tension of the liquid, η represents the dynamic viscosity of the liquid, h represents the channel height, θ e represents the equilibrium contact angle between the liquid and the channel wall, a and b are unknown parameters related to the channel depth.

测量装置还包括显示装置307,显示装置307的输入端连接控制器305的第三输出端,用于显示控制器305输出的液体动力粘度数据。The measuring device further includes a display device 307 , the input end of the display device 307 is connected to the third output end of the controller 305 for displaying the hydrodynamic viscosity data output by the controller 305 .

为提高测量效率,微米/纳米通道303包括多个不同深度的通道,通道深度至少有5种;为避免感染,微米/纳米通道303中的通道均为为一次性使用;为提高准确度,微米/纳米通道为长直型。将深度为纳米量级的通道作为毛细管来减少实验液体的使用,通过毛细压力驱动液体流动,省去压差测量系统。深度为纳米量级的微米/纳米通道所需液体量极少,可以小于1μl;微米/纳米通道为一次性使用,避免感染,不需要清洗装置,而且通道加工技术成熟;装置简单,液体在毛细压力驱动下流入微米/纳米通道,不需要外部加压装置,不需要压力测量部件;操作简单、便于携带,测量迅速、结果可靠。In order to improve the measurement efficiency, the micro/nano channel 303 includes a plurality of channels with different depths, and there are at least 5 channel depths; in order to avoid infection, the channels in the micro/nano channel 303 are all disposable; /Nanochannels are long straight. The channel with a depth of nanometers is used as a capillary to reduce the use of experimental liquid, and the liquid flow is driven by capillary pressure, eliminating the need for a differential pressure measurement system. The micro/nano channel with a depth of nanometers requires a very small amount of liquid, which can be less than 1 μl; the micro/nano channel is one-time use, avoids infection, does not need to clean the device, and the channel processing technology is mature; the device is simple, and the liquid is in the capillary. It flows into the micro/nano channel driven by pressure, no external pressure device is required, and no pressure measurement components are required; the operation is simple, easy to carry, and the measurement is fast and the result is reliable.

整个测量装置的测量过程为:The measurement process of the whole measurement device is as follows:

对于已知深度h1、h2、h3、h4、h5的微米/纳米通道303而言,首先将进样装置302中的微量注射泵取下,吸取1种简单牛顿液体(比如去离子水),之后将微量注射泵放入进样装置302;For the micro/nano channel 303 with known depths h 1 , h 2 , h 3 , h 4 , h 5 , first remove the micro syringe pump in the sampling device 302 and suck a simple Newtonian liquid (such as ionized water), then put the micro-syringe pump into the sampling device 302;

打开电源301和控制器305,开启温控装置304,待其稳定工作,进样装置302将该牛顿液体送到微米/纳米通道303入口处,液体在毛细力作用下流入微米/纳米通道303中的一个单通道,数据采集装置306对不同时刻液体的距离进行测量,以图4所示的数据采集装置为例,过程如下:液体端面经过光电组件10时,计时电路402记录下该时刻t1,同理,光电组件11、12、13、14、15分别记录液体端面流过时的时刻t2、t3、t4、t5、t6,所有数据均传输到第一数据处理装置403中,第一数据处理装置403根据光电组件之间的距离及时刻t1、t2、t3、t4、t5、t6,得到6组流动距离l与时间t的数据;Turn on the power supply 301 and the controller 305, turn on the temperature control device 304, wait for it to work stably, the sampling device 302 sends the Newtonian liquid to the inlet of the micro/nano channel 303, and the liquid flows into the micro/nano channel 303 under the action of capillary force The data acquisition device 306 measures the distance of the liquid at different times. Taking the data acquisition device shown in FIG. 4 as an example, the process is as follows: when the liquid end face passes through the photoelectric component 10, the timing circuit 402 records the time t1 . , in the same way, the photoelectric components 11, 12, 13, 14, 15 respectively record the time t 2 , t 3 , t 4 , t 5 , t 6 when the liquid end face flows, and all the data are transmitted to the first data processing device 403 , the first data processing device 403 obtains 6 groups of data of flow distance l and time t according to the distance between the photoelectric components and the times t 1 , t 2 , t 3 , t 4 , t 5 , and t 6 ;

控制器305接收数据采集装置306中第一数据处理装置403传输的采集数据(6组流动距离l与时间t的数据),拟合得到并记录下该组实验数据的实验斜率Aexp1、Aexp2、Aexp3、Aexp4、Aexp5The controller 305 receives the collected data (6 groups of data of flow distance l and time t) transmitted by the first data processing device 403 in the data collection device 306, and obtains and records the experimental slopes A exp1 and A exp2 of the experimental data by fitting and recording. , A exp3 , A exp4 , A exp5 ;

同理,接着使用其他牛顿液体(比如异丙醇、乙醇、70%甘油、30%甘油等)开展类似实验,分别得到每次试验的斜率Aexp,控制器305会根据记录的每种深度通道(例如包括5个通道,则对应5种通道深度,可一次性测量5种待测液体的粘度)中的液体实验的Aexp/ALW与(σ·cosθe/η)值,每一种深度通道对应的实验数据作为一组数据,在直角坐标系中画出Aexp/ALW与(σ·cosθe/η)关系图,从而依据公式得到该深度通道的a、b值。依次得到的5组a、b值,拟合得到a、b值与通道深度之间的关系,以及a、b值之间的关系,我们可以得到h=f(a,b)以及a=f(b),也就说,对于任意已知深度为h的通道(深度为纳米量级),就可以根据已知的h=f(a,b)和a=f(b),直接计算得到该深度通道对应的a、b值,从而确定该深度通道对应的模型 In the same way, then use other Newtonian liquids (such as isopropanol, ethanol, 70% glycerol, 30% glycerol, etc.) to carry out similar experiments to obtain the slope A exp of each experiment, and the controller 305 will record the depth channel according to each depth channel. (For example, if 5 channels are included, corresponding to 5 channel depths, the viscosity of 5 kinds of liquids to be tested can be measured at one time) A exp /A LW and (σ·cosθ e /η) values of the liquid experiment in the liquid experiment, each The experimental data corresponding to the depth channel is used as a set of data, and the relationship between A exp /A LW and (σ·cosθ e /η) is drawn in the rectangular coordinate system, so that according to the formula Get the a and b values of the depth channel. The five groups of a and b values obtained in turn are fitted to obtain the relationship between the a and b values and the channel depth, as well as the relationship between the a and b values. We can obtain h=f(a,b) and a=f (b), that is to say, for any channel with a known depth of h (the depth is on the order of nanometers), it can be directly calculated according to the known h=f(a,b) and a=f(b) The a and b values corresponding to the depth channel, so as to determine the model corresponding to the depth channel

结合拟合斜率,利用上式就可以得到该液体在该深度通道中的动力粘度;Combined with the fitting slope, the dynamic viscosity of the liquid in the depth channel can be obtained by using the above formula;

显示装置307实时显示测得的动力粘度的值。The display device 307 displays the measured value of the kinematic viscosity in real time.

本发明使用测量液体粘度的装置,根据测量液体粘度的方法进行测量的具体实施例1:The present invention uses the device for measuring liquid viscosity, and the specific embodiment 1 of measuring according to the method for measuring liquid viscosity:

已知微米/纳米通道中某一个单通道的通道深度h=68nm,具体操作时,首先将进样装置中的微量注射泵取下,吸取乙醇,之后将微量注射泵放入进样装置;It is known that the channel depth h=68nm of a single channel in the micro/nano channel. In the specific operation, first remove the micro-syringe pump in the sampling device, absorb ethanol, and then put the micro-syringe pump into the sampling device;

打开电源和控制器,开启温控装置,待其稳定工作,进样装置将乙醇送到通道组入口处,液体在毛细力作用下流入该单通道,数据采集装置对不同时刻液体的距离进行测量,过程如下:液体端面经过光电组件10时,计时电路记录下该时刻t1,同理,分别记录液体端面流过光电组件11、12、13、14、15时的时刻t2、t3、t4、t5、t6,所有数据均传输到第一数据处理装置中,第一数据处理装置会根据光电组件之间的距离及时刻t1、t2、t3、t4、t5、t6得到6组流动距离l与时间t的数据;Turn on the power supply and controller, turn on the temperature control device, and wait for it to work stably. The sampling device sends ethanol to the inlet of the channel group, and the liquid flows into the single channel under the action of capillary force. The data acquisition device measures the distance of the liquid at different times. , the process is as follows: when the liquid end surface passes through the photoelectric component 10, the timing circuit records the time t 1 , and similarly, the time t 2 , t 3 , and the time t 2 , t 3 , and t 4 , t 5 , t 6 , all data are transmitted to the first data processing device, the first data processing device will according to the distance between the photoelectric components and the time t 1 , t 2 , t 3 , t 4 , t 5 , t 6 to obtain 6 groups of data of flow distance l and time t;

控制器根据6组流动距离l与时间t的数据拟合得到并记录下该组实验数据的实验斜率AexpThe controller obtains and records the experimental slope A exp of this group of experimental data according to the data fitting of 6 groups of flow distances l and time t;

接着分别使用异丙醇、70%甘油、30%甘油3种牛顿流体开展类似实验,得到实验斜率Aexp,控制器会根据记录的每种流体实验的Aexp/ALW与(σ·cosθe/η)值,在直角坐标系中画出Aexp/ALW与(σ·cosθe/η)关系图,根据公式得到a、b值。从拟合线可以得到,a=0.86107,b=-0.00983,确定该深度通道对应的模型 Then use isopropanol, 70% glycerol, and 30% glycerol to carry out similar experiments respectively, to obtain the experimental slope A exp , the controller will record A exp /A LW and (σ·cosθ e of each fluid experiment recorded) /η) value, draw the relationship between A exp /A LW and (σ·cosθ e /η) in the Cartesian coordinate system, according to the formula Get a and b values. It can be obtained from the fitted line, a=0.86107, b=-0.00983, to determine the model corresponding to the depth channel

最后,使用微量注射泵吸取待测液体(去离子水),重复上述步骤,利用计时电路记录下待测液体在不同时刻的流动距离,利用上述模型,即可得到待测液体的粘度,约为1.008cP,该值与已有文献资料中去离子水的粘度值基本一致。Finally, use a micro syringe pump to suck the liquid to be tested (deionized water), repeat the above steps, use the timing circuit to record the flow distance of the liquid to be tested at different times, and use the above model to obtain the viscosity of the liquid to be tested, which is about 1.008cP, which is basically consistent with the viscosity value of deionized water in the existing literature.

本发明使用测量液体粘度的装置,根据测量液体粘度的方法进行测量的具体实施例2:The present invention uses the device for measuring liquid viscosity, and the specific embodiment 2 of measuring according to the method for measuring liquid viscosity:

已知微米/纳米通道中某一个单通道的通道深度h=116nm,具体操作时,首先将进样装置中的微量注射泵取下,吸取乙醇,之后将微量注射泵放入进样装置;It is known that the channel depth h=116nm of a single channel in the micro/nano channel. During the specific operation, first remove the micro-syringe pump in the sampling device, absorb ethanol, and then put the micro-syringe pump into the sampling device;

打开电源和控制器,开启温控装置,待其稳定工作,进样装置将乙醇送到通道组入口处,液体在毛细力作用下流入该单通道,数据采集装置对不同时刻液体的距离进行测量,过程如下:液体端面经过光电组件10时,计时电路记录下该时刻t1,同理,分别记录液体端面流过光电组件11、12、13、14、15时的时刻t2、t3、t4、t5、t6,所有数据均传输到第一数据处理装置中,第一数据处理装置会根据光电组件之间的距离及时刻t1、t2、t3、t4、t5、t6得到6组流动距离l与时间t的数据;Turn on the power supply and controller, turn on the temperature control device, and wait for it to work stably. The sampling device sends ethanol to the inlet of the channel group, and the liquid flows into the single channel under the action of capillary force. The data acquisition device measures the distance of the liquid at different times. , the process is as follows: when the liquid end surface passes through the photoelectric component 10, the timing circuit records the time t 1 , and similarly, the time t 2 , t 3 , and the time t 2 , t 3 , and t 4 , t 5 , t 6 , all data are transmitted to the first data processing device, the first data processing device will according to the distance between the photoelectric components and the time t 1 , t 2 , t 3 , t 4 , t 5 , t 6 to obtain 6 groups of data of flow distance l and time t;

控制器根据6组流动距离l与时间t的数据拟合得到并记录下该组实验数据的实验斜率AexpThe controller obtains and records the experimental slope A exp of this group of experimental data according to the data fitting of 6 groups of flow distances l and time t;

接着分别使用异丙醇、30%甘油2种牛顿流体开展类似实验,得到实验斜率Aexp,控制器会根据记录的每种流体实验的Aexp/ALW与(σ·cosθe/η)值,在直角坐标系中画出Aexp/ALW与(σ·cosθe/η)关系图,根据公式得到a、b值。从拟合线可以得到,a=1.0593,b=-0.0097,确定该深度通道对应的模型 Then use isopropanol and 30% glycerol to carry out similar experiments respectively to obtain the experimental slope A exp , and the controller will record the values of A exp /A LW and (σ·cosθ e /η) of each fluid experiment , draw the relationship between A exp /A LW and (σ·cosθ e /η) in the Cartesian coordinate system, according to the formula Get a and b values. It can be obtained from the fitted line, a=1.0593, b=-0.0097, to determine the model corresponding to the depth channel

最后,使用微量注射泵吸取待测液体(去离子水),重复上述步骤,利用计时电路记录下待测液体在不同时刻的流动距离,利用上述模型,即可得到待测液体的粘度,约为1.010cP,该值与已有文献资料中去离子水的粘度值基本一致,且与68nm深通道中测量数据基本吻合。Finally, use a micro syringe pump to suck the liquid to be tested (deionized water), repeat the above steps, use the timing circuit to record the flow distance of the liquid to be tested at different times, and use the above model to obtain the viscosity of the liquid to be tested, which is about 1.010cP, this value is basically consistent with the viscosity value of deionized water in the existing literature, and is basically consistent with the measurement data in the 68nm deep channel.

本说明书中各个实施例采用递进的方式描述,每个实施例重点说明的都是与其他实施例的不同之处,各个实施例之间相同相似部分互相参见即可。对于实施例公开的系统而言,由于其与实施例公开的方法相对应,所以描述的比较简单,相关之处参见方法部分说明即可。The various embodiments in this specification are described in a progressive manner, and each embodiment focuses on the differences from other embodiments, and the same and similar parts between the various embodiments can be referred to each other. For the system disclosed in the embodiment, since it corresponds to the method disclosed in the embodiment, the description is relatively simple, and the relevant part can be referred to the description of the method.

本文中应用了具体个例对本发明的原理及实施方式进行了阐述,以上实施例的说明只是用于帮助理解本发明的方法及其核心思想;同时,对于本领域的一般技术人员,依据本发明的思想,在具体实施方式及应用范围上均会有改变之处。综上所述,本说明书内容不应理解为对本发明的限制。In this paper, specific examples are used to illustrate the principles and implementations of the present invention. The descriptions of the above embodiments are only used to help understand the methods and core ideas of the present invention; meanwhile, for those skilled in the art, according to the present invention There will be changes in the specific implementation and application scope. In conclusion, the contents of this specification should not be construed as limiting the present invention.

Claims (8)

1. a kind of method for measuring liquid viscosity, which is characterized in that the described method includes:
Establish the actual relationship model of liquid length of flow and time:
Wherein a and b is related with channel depth Unknown parameter, AexpFor actual fit slope, l (t) indicates the flow distance of t moment liquid, and σ indicates surface tension of liquid, θe Indicate that the equilibrium contact angle between liquid and conduit wall, η indicate hydrodynamic viscosity, h indicates channel height;
Determine the relational model between hydrodynamic viscosity and practical fit slope:
The value for determining unknown parameter a and b determines the relational model The value of the determining unknown parameter a and b, specifically includes: being tested using the corresponding N group that carries out of liquid known to N kind, N is whole greater than 1 Number;According to formulaObtain every group in the experiment of N group The fit slope A of experimentexp;According to formulaObtain every group in the experiment of N group The theoretical slope A of experimentLW;The fit slope of every group of experiment in the experiment of N group and the ratio of theory of correspondences slope are obtained, is obtained:Wherein Aexp(k)The fit slope that expression kth group is tested, k=1,2 ... ... N, ALW(k)Indicate that kth group tests corresponding theoretical slope, σ(k)Indicate surface tension of liquid in the experiment of kth group, θe(k)Indicate kth Equilibrium contact angle in group experiment between liquid and conduit wall, η(k)Indicate the theoretical value of hydrodynamic viscosity in the experiment of kth group;Root According to the relevant parameter of the known liquid of N group experiment, it is corresponding to obtain liquid known to every group of experimentGinseng Number, wherein the relevant parameter includes surface tension of liquid σ(k), equilibrium contact angle θ between liquid and conduit walle(k), liquid it is dynamic The theoretical value η of power viscosity(k);Determine the value of a and the b;
According to the actual fit slope that liquid flows, the dynamic viscosity of the liquid is determined.
2. the method according to claim 1, wherein after the value of the determination a and b, further includes:
The relational model of length of flow and time during the corresponding liquid flowing in the channel of acquisition M group different depthIn unknown parameter a(i)And b(i)Value, wherein M is big In 1 integer, a(i)And b(i)For with channel depth h(i)Related unknown parameter, channel depth h(i)For the depth of channel i;
Determine the pass between the relation function h=f (a, b) and unknown parameter a and b between channel depth h and unknown parameter a, b It is function a=g (b).
3. a kind of system for measuring liquid viscosity, which is characterized in that the system comprises:
Length of flow and the relational model of time establish module, for establishing the actual relationship mould of liquid length of flow and time Type:Wherein a and b is related with channel depth Unknown parameter, AexpFor actual fit slope, l (t) indicates the flow distance of t moment liquid, and σ indicates surface tension of liquid, θe Indicate that the equilibrium contact angle between liquid and conduit wall, η indicate hydrodynamic viscosity, h indicates channel height;
Hydrodynamic viscosity and practical fit slope relational model determining module, for determining hydrodynamic viscosity and practical fitting Relational model between slope:
Unknown parameter determining module determines the relational model for determining the value of unknown parameter a and bThe unknown parameter determining module, specifically includes: experiment control list Member, for being tested using the corresponding N group that carries out of liquid known to N kind;Fit slope obtains module, for according to formulaThe fitting for obtaining every group of experiment in the experiment of N group is oblique Rate Aexp;Theoretical slope acquiring unit, for according to formulaObtain the experiment of N group In every group of experiment theoretical slope ALW;Ratio calculation unit, for calculate N group experiment in every group of experiment fit slope and The ratio of theory of correspondences slope, obtains:Wherein Aexp(k)Indicate that kth group is tested The fit slope arrived, k=1,2 ... ... N, ALW(k)Indicate that kth group tests corresponding theoretical slope, σ(k)It indicates in the experiment of kth group Surface tension of liquid, θe(k)Indicate the equilibrium contact angle in the experiment of kth group between liquid and conduit wall, η(k)It indicates in the experiment of kth group The theoretical value of hydrodynamic viscosity;Liquid parameter computing unit, the related ginseng of the known liquid for being tested according to the N group Number, it is corresponding to obtain liquid known to every group of experimentParameter, wherein the relevant parameter includes liquid surface Power σ(k), equilibrium contact angle θ between liquid and conduit walle(k), hydrodynamic viscosity theoretical value η(k);Unknown parameter determines single Member, for determining the value of a and b;
Dynamic viscosity determining module, the actual fit slope for being flowed according to liquid, determines the dynamic viscosity of the liquid.
4. system according to claim 3, which is characterized in that the system also includes:
The corresponding unknown parameter determining module in different depth channel after the value for determining a and b, obtains the different depths of M group The relational model of length of flow and time during the corresponding liquid flowing in the channel of degree
In unknown parameter a(i)And b(i)Value, wherein a(i)And b(i)For with channel depth h(i)Related unknown parameter, channel depth h(i)For the depth of channel i;
Relation function determining module, for determine the relation function h=f (a, b) between channel depth h and unknown parameter a, b with And the relation function a=g (b) between unknown parameter a and b.
5. a kind of device for measuring liquid viscosity, which is characterized in that described device includes: power supply, sampling device, micrometer/nanometer Channel, temperature control device, controller, data acquisition device;
The power supply connects the sampling device;The output end of the sampling device and the entrance in the micrometer/nanometer channel connect It connects, the outlet in the micrometer/nanometer channel leads directly to atmosphere;
First output end of the controller connects the input terminal of the sampling device;The second output terminal of the controller connects The input terminal of the temperature control device;The micrometer/nanometer channel is located inside the temperature control device;
The data acquisition device is used to acquire flow distance and the time of liquid;
The input terminal of the controller connects the data acquisition device, the liquid for acquiring according to the data acquisition device Away from discrete time, the length of flow of liquid and the relational model of time are utilized
Obtain actual fit slope Aexp, also For combining the theoretical relationship of liquid length of flow and time The value for determining unknown parameter a and b determines the relational model between hydrodynamic viscosity and practical fit slopeAccording to the actual fit slope that liquid flows, the liquid is determined Dynamic viscosity, wherein l (t) indicates the flow distance of t moment liquid, and σ indicates that surface tension of liquid, η indicate that hydrodynamic is viscous Degree, h indicate channel height, θeIndicate that the equilibrium contact angle between liquid and conduit wall, a and b are related with channel depth unknown Parameter.
6. device according to claim 5, which is characterized in that the data acquisition device specifically includes: E group photoelectricity group Part, timing circuit, the first data processing equipment;Wherein E is the integer greater than 2;
Every group of photoelectric subassembly includes an optical transmitting set and an optical receiver, E optical transmitting set of the E group photoelectric subassembly according to The secondary lower section positioned at the micrometer/nanometer channel, E optical receiver of the E group photoelectric subassembly are sequentially located at the micron/receive The top in rice grain pattern road is correspondingly arranged with the E optical transmitting set;
E optical receiver of the E group photoelectric subassembly is connected with the timing circuit;
First data processing equipment is connect with the output end of the timing circuit, for according to the E group photoelectric subassembly it Between distance and the micrometer/nanometer channel in liquid reach time of each group of photoelectric subassembly, obtain the E group flowing of liquid away from Discrete time.
7. device according to claim 5, which is characterized in that the data acquisition device specifically includes: F light source, F Photoelectric sensor, the second data processing equipment;Wherein F is the integer greater than 2;
The F light source and the F photoelectric sensor correspond;The F photoelectric sensor be sequentially located at the micron/ The top of nanochannel, the F light source are sequentially located at the lower section in the micrometer/nanometer channel, with the F photoelectric sensor It is oppositely arranged;
Second data processing equipment is connect with the output end of the F photoelectric sensor, for according to the F photoelectric transfer Liquid reaches the time of each photoelectric sensor in the distance between sensor and the micrometer/nanometer channel, obtains the F of liquid Group flow distance and time.
8. device according to claim 5, which is characterized in that the measuring device further include: display device, the display The input terminal of device connects the third output end of the controller, for showing the hydrodynamic viscosity number of the controller output According to.
CN201710563487.8A 2017-07-12 2017-07-12 A method and system for measuring liquid viscosity Active CN107389502B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710563487.8A CN107389502B (en) 2017-07-12 2017-07-12 A method and system for measuring liquid viscosity

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710563487.8A CN107389502B (en) 2017-07-12 2017-07-12 A method and system for measuring liquid viscosity

Publications (2)

Publication Number Publication Date
CN107389502A CN107389502A (en) 2017-11-24
CN107389502B true CN107389502B (en) 2019-07-26

Family

ID=60339093

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710563487.8A Active CN107389502B (en) 2017-07-12 2017-07-12 A method and system for measuring liquid viscosity

Country Status (1)

Country Link
CN (1) CN107389502B (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113324874A (en) * 2021-05-14 2021-08-31 大连海事大学 Liquid viscosity measuring device
CN114216950B (en) * 2021-11-30 2024-04-12 清华大学 Method and device for measuring liquid-liquid interface charge density
CN117606980B (en) * 2023-09-22 2024-07-09 中煤科工开采研究院有限公司 Method for measuring the flow properties of a liquid and device for observing liquid drops

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1847849A (en) * 2004-04-13 2006-10-18 中国科学院力学研究所 A measuring instrument capable of detecting human blood viscosity in real time
CN204255802U (en) * 2014-12-17 2015-04-08 中国科学院工程热物理研究所 Liquid parameter measuring system
CN105547922A (en) * 2015-12-11 2016-05-04 清华大学 Microviscosimeter based on micro/nano channel

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2006036833A2 (en) * 2004-09-24 2006-04-06 The Regents Of The University Of Michigan A nanoliter viscometer for analyzing blood plasma and other liquid samples
US20140232853A1 (en) * 2013-02-21 2014-08-21 Neil E. Lewis Imaging microviscometer

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1847849A (en) * 2004-04-13 2006-10-18 中国科学院力学研究所 A measuring instrument capable of detecting human blood viscosity in real time
CN204255802U (en) * 2014-12-17 2015-04-08 中国科学院工程热物理研究所 Liquid parameter measuring system
CN105547922A (en) * 2015-12-11 2016-05-04 清华大学 Microviscosimeter based on micro/nano channel

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
"Nanoliter Viscometer for Analyzing Blood Plasma and Other Liquid Samples";Nimisha Srivastava 等;《Analytical Chemistry》;20050115;第77卷;第383-392页
"微纳通道中牛顿流体毛细流动的研究进展";杨敏 等;《科学通报》;20160531;第61卷(第14期);第1574-1584页

Also Published As

Publication number Publication date
CN107389502A (en) 2017-11-24

Similar Documents

Publication Publication Date Title
CN106644900B (en) Impedance pulse particle counting device based on non-uniform electric field and counting method thereof
CN107389502B (en) A method and system for measuring liquid viscosity
CN104568287B (en) Pressure apparatus in a kind of deformation direct measurement microchannel of utilization PDMS film
CN207907955U (en) A kind of micro-flowmeter based on line array CCD
CN107631958A (en) A kind of small test device for testing super hydrophobic material resistance reducing performance
CN103257099A (en) Device for measuring seepage of porous medium
CN103471981A (en) A high-throughput particle counting device and method based on a microfluidic chip
CN103185808A (en) Photoelectric technology-based bubble velocity-measuring system
JP2007521478A (en) Blood cell deformability measuring device
CN106443061A (en) Micro-flow-velocity optical measuring apparatus based on optical fiber F-P cavity
CN106885762A (en) Closed loop liquid drop microfluidic system based on capacitance detecting
CN114659935A (en) A kind of measuring method and device of micro-liquid viscosity and micro-channel flow resistance
CN206321568U (en) A device for detecting moisture content in lubricating oil based on optofluidic technology
CN107084918B (en) A kind of concentration sensor manipulating single microballoon based on optical fiber
CN109932283B (en) Apparatus and method for measuring apparent viscosity of non-Newtonian fluids at high shear rates
CN109142675A (en) A kind of micron capillary column gas-liquid dynamic phase interface test device
CN105352849B (en) Online oil viscosity detector
CN107314952A (en) A kind of method and system for measuring dynamic contact angle under extremely low capillary number
CN207964570U (en) Particle counting device with adjustable detection precision
CN106970014A (en) A kind of automatic measurement calculates the displacement method of testing of rock core physical parameter
CN105547922A (en) Microviscosimeter based on micro/nano channel
CN108562514B (en) High-temperature, high-pressure, low-speed gas microtube viscosity measuring device and measuring method thereof
CN100549695C (en) A kind of measuring instrument of real-time human body blood viscosity
CN110646044B (en) A method and device for non-contact detection of thermal fluid flow
CN102944500B (en) For the lane device of tracer liquid viscosity and system and application thereof

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant