CN204255802U - Liquid parameter measuring system - Google Patents

Abstract

The utility model provides a kind of liquid parameter measuring system.This liquid parameter measuring system comprises: Taylor bubble flow generation device; Visual measurement microtubule, it has a microchannel, and the front end of this microchannel is connected with Taylor bubble flow generation device; Camera, is arranged at the radial outer periphery of visual measurement microtubule; And thickness of liquid film measurement mechanism, be arranged at the radial outer periphery of visual measurement microtubule.Wherein, Taylor bubble flow generation device generates the Taylor bubble flow of testing liquid, and this Taylor bubble flow flows through the microchannel of visual measurement microtubule, and the initial thickness of liquid film δ of bubble periphery in microchannel measured by thickness of liquid film measurement mechanism ₀, multiple instantaneous pictures of bubbly flow in cameras capture microchannel.The utility model obtains the kinetic viscosity μ of fluid to be measured based on this same physical phenomenon of Taylor two-phase flow simultaneously _lwith surface tension σ, do not need to measure respectively different parameters, operation steps is easier.

Description

Liquid parameter measuring system

Technical field

The utility model relates to surveying instrument/field of instrumentation technology, particularly relates to a kind of liquid parameter measuring system.

Background technology

Viscosity, surface tension are the main physical parameters of liquid, are the important parameters that the industrial circle such as petrochemical complex, medicine detects.Viscosity and capillary measurement have great importance on scientific research, technological development and product manufacturing.The method measuring liquid viscosity has capillary tube technique, column spinner method etc.The method of surface tension has maximum bubble method, bubble amplitude-frequency Equivalent method etc.

It is Poiseulle law that capillary tube technique measures the theoretical foundation of liquid viscosity, namely under certain differential pressure action, flowing through the kapillary of the certain length time used by measuring liquid, calculating viscosity.Capillary tube technique complex operation, can bring subjectivity error with stopwatch, greatly reduce measuring accuracy, be not suitable for On-line rapid measurement writing time.

2004, Silber etc. have developed the minisize capillary pipe viscosity meter (SilberZ.H. based on computer system, Tan Y. P., Wen P.F.A Microtube Viscometer with a Thermostat.Experiments in Fluids, 2004,36 (4): 586-592), its apparatus structure as shown in Figure 1.Device is by being equipped with the flow velocity of stereo microscope monitoring stream of liquid droplets through kapillary of CCD, by pressure transducer and temperature sensor, fluid pressure and temperature are monitored, conversion Hou tri-road signal carries out data collection and analysis by computer system, and then calculates the viscosity number of liquid.According to Hagen-Poiseuille equation, liquid viscosity can be calculated by following formula:

$\mathrm{\μ}=\frac{{\mathrm{\πd}}^4}{128\mathrm{Ql}}\mathrm{\Δp}---\left(1\right)$

$Q=\frac{{\mathrm{\πd}}^{4}S}{4t}---\left(2\right)$

In formula, d is capillary diameter, and l is capillary pipe length, and Q is the flow of capillary liquid in pipe, and Δ p is kapillary two ends fluid pressure differential, and S is the effective liquid length flow through in the t time, and t is Measuring Time.

This measuring method is identical with traditional capillary tube technique, is to measure liquid viscosity based on the flow resistance of the single-phase flowing of fluid and the relation of viscosity.But this measuring method measures liquid viscosity based on the flow resistance of the single-phase flowing of fluid and the relation of viscosity, can only be used for the viscosity measuring liquid, cannot measure other physical parameters.

Please refer to Fig. 2, the ultimate principle adopting rotating cylinder method to measure liquid viscosity is: fill between interior outer cylindrical body with testing liquid, when exterior circular column uniform rotation, during inner cylinder transfixion, friction in liquid internal between two cylinders produces, internal rotating cylinder applies a shearing stress, can calculate liquid viscosity value by measuring this shearing stress.Adopt the method to measure liquid viscosity, require fricton-tight friction between liquid and interior outer cylindrical body, therefore fluid to be measured must be good with inner/outer tube material wetting state, needs for the different cylinder material of different liquid selective; Liquid must ensure uniform composition and be in laminar condition in measuring process in addition, and the speed that relatively rotates between interior outer cylindrical body is not easily excessive, and therefore rotor speed limits to some extent.

Maximum bubble method measures the surface tension of liquid, is by being blown into inert gas gently to the kapillary inserting liquid, utilizing the quantitative relationship of maximum differential pressure and bubble radius to carry out gauging surface tension force.The method need ensure that bubble is subsphaeroidal, need select suitable capillary inner diameter.

Please refer to Fig. 3, the principle of employing bubble amplitude-frequency Equivalent method surface tension is: utilize a constant voltage source of the gas, blown to fluid to be measured by a standard capillary in limiting time, the process that monitoring bubble is constantly formed, grows up and vanishes, can obtain a continuous oscillation curve.The amplitude of curve and frequency represent bubble inner pressure difference change amplitude respectively and bubble forms speed, and bubble inner pressure difference change amplitude and bubble form speed and surface tension of liquid is closely related, therefore, a numerical value suitable with real surface tension force can be solved according to curve amplitude and frequency, be called equivalent scale surface tension.Calculating the capillary formula of equivalent is formula (3):

σ _ein=a Δ P+bN-c Δ ρ+d (3) formula (3): σ _efor liquid equivalent scale surface tension (10 ^-3n/m), Δ P is bubble inner pressure difference change amplitude, and N is the number of blowout bubble in limiting time, and Δ ρ is the difference (g/cm of fluid to be measured mass density and quality density ³), a, b, c, d are respectively the experience factor and constant testing and determine.

It should be noted that bubble amplitude-frequency Equivalent method is that empirical equation (3) surface tension to fluid to be measured obtained according to regretional analysis calculates, experience factor a, b, c, d directly determine measuring accuracy.In different surfaces tension force section, experience factor a, b, c, d get different numerical value, and when surface tension section residing for indefinite fluid to be measured, select suitable regression formula to calculate with regard to being difficult to, therefore, its measuring accuracy is difficult to ensure.According to the surface tension that the measurement of bubble amplitude-frequency Equivalent method obtains, a numerical value suitable with real surface tension force, i.e. equivalent scale surface tension, be not equal to accurate surface tension value, its measuring accuracy only can meet commercial measurement requirement, cannot meet the measurement requirement to the higher field such as scientific research, sophisticated technology of accuracy requirement.Bubble amplitude-frequency Equivalent method only can surface tension, cannot measure the viscosity of liquid.

These methods above-mentioned all can only obtain a physical parameter of fluid to be measured: surface tension or viscosity, rarely have the measuring method and device that record surface tension and viscosity simultaneously.

Within 2007, Harbin University of Science and Technology have developed a kind of energy Quick Measurement Normal Atmospheric Temperature Liquid viscosity, density and capillary integrate more parameters testing instrument (Gao Guili simultaneously, Li great Yong, Shi Dequan. the development of viscosity density surface tension multi-parameter fast test apparatus for normal temperature liquid, Chinese journal of scientific instrument, 2007,28 (7): 1332-1336).As shown in Figure 4, this integrate more parameters testing instrument is made up of Multi-functional probe 5, viscosity test unit, air supply unit, weighing unit 3 and computer measurement and control unit.Multi-functional probe 5 and viscosity test unit matching, can complete the measurement of Normal Atmospheric Temperature Liquid viscosity, density, surface tension and temperature.Air supply unit forms primarily of micro air pump 11, solenoid directional control valve, glass ball float flowmeter 10, and micro air pump 11, to the kapillary air feed of probe, completes capillary measurement.Computer measurement and control unit is responsible for data acquisition and action control, and by test result by LED7 display and printer 8 printout.

For the integrate more parameters testing instrument shown in Fig. 4, it is actually the combination of three kinds of measuring methods: liquid viscosity adopts rotating cylinder method to measure; Density adopts liquid statics weighing method to measure; Surface tension adopts bubble amplitude-frequency Equivalent method to measure; Viscosity and surface tension are measured based on different measuring principles respectively.And, when this integrate more parameters testing instrument adopts rotating cylinder method to measure the viscosity of liquid, require equally fluid to be measured and inner/outer tube material wetting state good, need, for different cylinder material, the different motor speeds of different liquid selective, measurement range and rotor speed to limit to some extent; When adopting bubble amplitude-frequency Equivalent method and rotating cylinder method to measure surface tension and the viscosity of liquid respectively, the memory space of fluid to be measured at least reaches the order magnitude range of 10ml ~ 100ml.When the supply of fluid to be measured is very little, be difficult to ensure measuring accuracy.

At present, need in the industry a kind of structure badly simple, easy to use, the instrument of the measurement of the multiple physical parameter of fluid can be carried out simultaneously.

Utility model content

(1) technical matters that will solve

In view of above-mentioned technical matters, it is simple, easy to use that the utility model provides a kind of structure, can carry out the liquid parameter measuring system of the measurement of the multiple physical parameter of fluid simultaneously.

(2) technical scheme

The utility model liquid parameter measuring system comprises: Taylor bubble flow generation device; Visual measurement microtubule, it has a microchannel, and the front end of this microchannel is connected with Taylor bubble flow generation device; Camera, is arranged at the radial outer periphery of visual measurement microtubule; And thickness of liquid film measurement mechanism 109, be arranged at the radial outer periphery of visual measurement microtubule.Wherein, Taylor bubble flow generation device generates the Taylor bubble flow of testing liquid, this Taylor bubble flow flows through the microchannel of visual measurement microtubule, and thickness of liquid film measurement mechanism 109 measures the initial thickness of liquid film δ of bubble periphery in microchannel through visual measurement microtubule ₀, camera catches multiple instantaneous pictures of bubbly flow in microchannel through visual measurement microtubule.

Preferably, in the utility model liquid parameter measuring system, Taylor bubble flow generation device comprises: actuator, syringe 102, compressed gas source and the first three-way pipe 106; Actuator withstands the rear end of the piston core bar of syringe 102; The first interface of the first three-way pipe 106 is connected to the outlet of syringe 102, and its 3rd interface is connected to the outlet of compressed gas source, and its second interface is as the outlet of Taylor bubble flow; Syringe 102 injects fluid to be measured; The piston core bar motion of actuator pushing syringe 102, extruding testing liquid flows out, and enters the first three-way pipe 106; This testing liquid mixes in the first three-way pipe 106 with compressed gas source effluent air, forms Taylor bubble flow, is exported by the second interface of the first three-way pipe 106.

Preferably, in the utility model liquid parameter measuring system, actuator is drive motor 101.

Preferably, in the utility model liquid parameter measuring system, Taylor bubble flow generation device also comprises: the first variable valve 103, is arranged between the outlet of syringe 102 and the first interface of the first three-way pipe 106; And/or second variable valve 105, be arranged between compressed gas source and the 3rd interface of the first three-way pipe 106.

Preferably, in the utility model liquid parameter measuring system, Taylor bubble flow generation device comprises: compressed gas source; Reservoir 203, its pressure port is connected to the outlet of compressed gas source; And second three-way pipe 206, its first interface is connected to the liquid outlet of reservoir 203, and its 3rd interface is connected to the outlet of compressed gas source, and its second interface is as the outlet of Taylor bubble flow; Wherein, testing liquid in reservoir 203 is pressed into the second three-way pipe 206 by the gas in compressed gas source, this testing liquid mixes in the second three-way pipe 206 with compressed gas source effluent air, forms Taylor bubble flow, is exported by the second interface of the second three-way pipe 206.

Preferably, in the utility model liquid parameter measuring system, Taylor bubble flow generation device also comprises: the 3rd variable valve 202, is arranged between the outlet of compressed gas source and the pressure port of reservoir 203; 4th variable valve 204, is arranged between the liquid outlet of reservoir 203 and the first interface of the second three-way pipe 206; 5th variable valve 205, is arranged between the 3rd interface of the second three-way pipe 206 and the 3rd variable valve 202.

Preferably, in the utility model liquid parameter measuring system, compressed gas source is compressed gas cylinder 104 or air pump.

Preferably, in the utility model liquid parameter measuring system, visual measurement microtubule be plane with camera 110, wall that thickness of liquid film measurement mechanism 109 is relative.

Preferably, in the utility model liquid parameter measuring system, the xsect of the microchannel of visual measurement microtubule is in the axisymmetric shape with two and above axis of symmetry.

Preferably, in the utility model liquid parameter measuring system, the xsect of the microchannel of visual measurement microtubule is: circular, its diameter is less than 1.5mm; Square, its equivalent diameter is less than 1.5mm; Or rectangle, its ratio of width to height W/D >=20, and height D≤0.5mm.

Preferably, in the utility model liquid parameter measuring system, the xsect of the microchannel of visual measurement microtubule is circular, visual measurement microtubule: be the transparent glass tube of square-outside and round-inside, or comprise: micro-square tube; Be positioned at micro-pipe of micro-square tube, and be filled in the filled media between micro-square tube and micro-pipe; Wherein, micro-square tube is identical with the material of micro-pipe, and the refractive index of filled media material and the specific refractivity of micro-square tube material are less than 0.1.

Preferably, the utility model liquid parameter measuring system also comprises: data acquisition and analytical equipment 113, be connected with thickness of liquid film measurement mechanism 109 with camera 110, and its multiple instantaneous pictures utilizing camera 110 to catch bubbly flow obtain the apparent velocity U of bubble _b, and then utilize the internal diameter D of microchannel, the density p of testing liquid of visual measurement microtubule 107 _l, the initial thickness of liquid film δ of bubble periphery ₀, bubble apparent velocity U _bcalculate the kinetic viscosity μ of testing liquid _land/or surface tension σ.

Preferably, in the utility model liquid parameter measuring system, data acquisition and analytical equipment 113 calculate the kinetic viscosity μ of testing liquid according to following computing formula _land/or surface tension σ:

$\frac{{\mathrm{\δ}}_0}{D}=a+\frac{b\·C{a}^{2/3}}{1+c\·{\mathrm{Ca}}^{2/3}+d\·{\mathrm{Ca}}^{m}R{e}^n-e\·{\mathrm{We}}^p}$

Wherein: Ca is capillary constant: Ca=μ _lu _b/ σ; We is weber number: re is Reynolds number: a, b, c, d, e, m, n, p are the parameter relevant to the shape of cross section of the microchannel of visual measurement microtubule 107.

Preferably, in the utility model liquid parameter measuring system, the microchannel of visual measurement microtubule 107 is circular microchannel, and its internal diameter is less than 1.5mm, and in computing formula, the value of each parameter is as follows:

a＝0，b＝0.67，c＝3.13，d＝0.504，e＝0.352，m＝0.672，n＝0.589，p＝0.629。

Preferably, in the utility model liquid parameter measuring system, the microchannel of visual measurement microtubule 107 is square microchannel, and its equivalent diameter is less than 1.5mm, in computing formula, and the initial thickness of liquid film δ of bubble periphery ₀for micro-thickness of liquid film of square microchannel edge, i.e. δ _{0_corner}, the value of each parameter is as follows: a=0.243, b=2.43, c=7.28, d=0, e=0.255, p=0.215.

Preferably, in the utility model liquid parameter measuring system, the microchannel of visual measurement microtubule 107 is the Rectangular Microchannel of high the ratio of width to height, its the ratio of width to height W/D>=20, and height D≤0.5mm, wherein, in the calculating formula of weber number We and reynolds number Re, the internal diameter D of microchannel is the hydraulic diameter D of this Rectangular Microchannel _h: $\mathrm{We}=\frac{{\mathrm{\ρ}}_l{U_b}^2{D}_h}{\mathrm{\σ}};\mathrm{Re}=\frac{{\mathrm{\ρ}}_l{U}_b{D}_h}{{\mathrm{\μ}}_l};$ Wherein: $D_h=\frac{4A}{U}=\frac{2(W\×D)}{W+D};$ In computing formula, the value of each parameter is as follows: a=0, b=0.67, c=3.13, d=0.504, e=0.352, m=0.672, n=0.589, p=0.629.

Preferably, in the utility model liquid parameter measuring system, in data acquisition and analytical equipment 113: as kinetic viscosity μ _lduring with one of them the unknown of surface tension σ, calculate unknown parameter by the measured value of one group of Taylor bubble flow according to computing formula; Or as kinetic viscosity μ _ltime all unknown with surface tension σ, build the system of equations about computing formula by the measured value of two groups of different Taylor bubble flows, calculating kinetic viscosity μ by solving this system of equations _lwith surface tension σ.

Preferably, in the utility model liquid parameter measuring system, the measuring accuracy of thickness of liquid film measurement mechanism 109 is greater than 0.1 μm; The capture rate of camera 110 is not less than 1000 frames/second.

Preferably, in the utility model liquid parameter measuring system, thickness of liquid film measurement mechanism 109 is that confocal laser is apart from Displacement Meters or ellipsometer.

Preferably, the utility model liquid parameter measuring system also comprises: temperature sensor (111,112), is arranged at front end and/or the rear end of the microchannel of visual measurement microtubule 107; And/or returnable 108, be connected to the rear end of the microchannel of visual measurement microtubule 107.

(3) beneficial effect

As can be seen from technique scheme, the utility model liquid parameter measuring system has following beneficial effect:

(1) obtain the kinetic viscosity μ of fluid to be measured based on this same physical phenomenon of Taylor two-phase flow simultaneously _lwith surface tension σ, can record two parameters more easily, and not need to measure respectively different parameters, operation steps is easier;

(2) based on the micro-thickness of liquid film δ of bubble ₀and the quantitative relationship between capillary constant Ca and the measuring system designed, this relational expression under multiple flox condition, concludes by multiple fluid the rule-of-thumb relation obtained, widely applicable, measuring accuracy is high, in measuring process, by parameters such as adjust fluxes, multiple spot repetitive measurement is done to same physical property, further raising precision, can meet the measurement requirement to the higher field such as scientific research, sophisticated technology of accuracy requirement;

(3) can a tractor serves several purposes be realized: when the surface tension of fluid to be measured is known, can be used for measuring kinetic viscosity; When the kinetic viscosity of fluid to be measured is known, surface tension can be used for; When kinetic viscosity and surface tension are all unknown, can be used for measuring this two physical parameters simultaneously;

(4) fluid to be measured carries out visualization measurement in the current downflow of ordering about of driving force to visual measurement microtubule, as long as ensure corresponding measuring section transparent visual, the selection of microtubule material is not by the impact of fluid to be measured wettability;

(5) internal diameter of micro-pipe is very little, and only need the fluid to be measured of 1ml ~ 10ml capacity magnitude to complete measuring process, liquid demand is very little, can ensure precision equally when fluid to be measured quantity delivered is very little.

Accompanying drawing explanation

Fig. 1 is the structural representation of prior art 1 based on the minisize capillary pipe viscosity meter of computer system;

Fig. 2 is that prior art 2 adopts column spinner method to measure the schematic diagram of liquid viscosity;

Fig. 3 is the schematic diagram that prior art 3 adopts bubble amplitude-frequency Equivalent method surface tension;

Fig. 4 is the structural representation of prior art 4 fluid integrate more parameters testing instrument;

Fig. 5 is micro-liquid film schematic diagram bottom bubble in microchannel in Taylor flow theory;

Fig. 6 is the structural representation according to the utility model first embodiment liquid parameter measuring system;

Fig. 7 is the enlarged drawing of syringe in the measuring system of liquid parameter shown in Fig. 6;

Fig. 8 is the schematic cross-section of measurement microtubule visual in the measuring system of liquid parameter shown in Fig. 6;

Fig. 9 is the workflow diagram of the measuring system of liquid parameter shown in Fig. 6;

Figure 10 is the structural representation according to Taylor bubble flow generation device in the utility model second embodiment liquid parameter measuring system;

Figure 11 is the schematic cross-section according to visual measurement microtubule in the utility model the 3rd embodiment liquid parameter measuring system;

Figure 12 is the schematic diagram of the micro-thickness of liquid film of micro-square tube edge.

[the utility model main element symbol description]

101-drive motor; 102-syringe;

103-first variable valve; 104-compressed gas source;

105-second variable valve; 106-first three-way pipe;

The visual measurement microtubule of 107-; 108-returnable;

109-thickness of liquid film measurement mechanism; 110-high speed camera;

111-first temperature sensor; 112-second temperature sensor;

113-data acquisition and analytic system;

201-compressed gas cylinder; 202-the 3rd variable valve;

203-reservoir; 204-the 4th variable valve;

205-the 5th variable valve; 206-the two or two three-way pipe.

Embodiment

For making the purpose of this utility model, technical scheme and advantage clearly understand, below in conjunction with specific embodiment, and with reference to accompanying drawing, the utility model is further described.It should be noted that, in accompanying drawing or instructions describe, similar or identical part all uses identical figure number.The implementation not illustrating in accompanying drawing or describe is form known to a person of ordinary skill in the art in art.In addition, although herein can providing package containing the demonstration of the parameter of particular value, should be appreciated that, parameter without the need to definitely equaling corresponding value, but can be similar to corresponding value in acceptable error margin or design constraint.The direction term mentioned in embodiment, such as " on ", D score, "front", "rear", "left", "right" etc., be only the direction with reference to accompanying drawing.Therefore, the direction term of use is used to illustrate and is not used for limiting protection domain of the present utility model.

The utility model obtains the kinetic viscosity μ of fluid to be measured based on this same physical phenomenon of Taylor two-phase flow simultaneously _lwith surface tension σ.Understand the utility model in order to clearer, first the principle of work of Taylor two-phase flow is illustrated as follows.

Form long bubble flow or slug flow after the bubble of motion in micro-channel or gas column arrange liquid, be called as Taylor flowing, this kind is flowing in fluid mechanics and is widely studied.As far back as 1961, Bretherton etc. find that the bubble underlying liquid film thickness that Taylor flowing is formed has uniform distribution properties, and carried out theoretical and dimensional analysis (F.P.Bretherton.The motion of long bubbles intubes, J.Fluid Mech.1961,10: 166-188).As shown in Figure 5, the micro-liquid film district under bubble column, liquid-gas interface is cylindric distribution, and its curvature should be K ≈ 1/ (R-δ ₀), and at nose of bubble, liquid-gas interface is semisphere, its curvature should be K ≈ 2/ (R-δ ₀), wherein R represents microchannel radius, δ ₀it is the original depth of micro-liquid film.

Due to capillary effect, the increase of curvature means the reduction of liquid internal pressure, and this pressure gradient from straight liquid film to head arranges the expulsive force of liquid when liquid-gas interface is pushed ahead just.For micro-thin film drainage, reynolds number Re is less, and the convective term of the equation of momentum can be ignored, and the speed of liquid-gas interface vertical direction is also very little, therefore axial velocity u _lthe governing equation of (x, z) can be simplified by Reynolds lubrication theory:

$\frac{{\mathrm{dP}}_l}{\mathrm{dx}}={\mathrm{\μ}}_l\frac{d^2{\mathrm{\μ}}_l}{{\mathrm{dz}}^2}---\left(4\right)$

The boundary condition at wall place is:

u _l| _z＝0＝0 (5)

The boundary condition at liquid-gas interface place is:

du _l/dz| _z＝δ＝0 (6)

P in formula _l, μ _lbe respectively liquid phase pressure and kinetic viscosity, x and z represents liquid film axis and normal direction (as shown in Figure 5) respectively.The solution of equation (4) can be tried to achieve thus:

$u_l(x,z)=\frac{1}{{\mathrm{\μ}}_l}\frac{{\∂P}_l}{\∂x}[\frac{z^2}{2}-\mathrm{\δ}\left(x\right)z]---\left(7\right)$

Therefore liquid film at the mean flow rate at x place, certain cross section is:

${\stackrel{\‾}{u}}_l={\mathrm{\δ}}^{-1}{\∫}_0^{\mathrm{\δ}}u(x,z)\mathrm{dz}=-\frac{{\mathrm{\δ}}^2}{3u_l}\frac{{\∂P}_l}{\∂x}---\left(8\right)$

δ in above formula refers to thickness of liquid film.

Assuming that the superficial velocity of bubble movement is U _b, at the mass velocity of x place, nose of bubble cross section liquid be:

$G\left(x\right)={\mathrm{\ρ}}_l{\stackrel{\‾}{u}}_l\mathrm{\δ}={\mathrm{\ρ}}_l{U}_b(\mathrm{\δ}-{\mathrm{\δ}}_0)---\left(9\right)$

In formula, ρ _lfor density of liquid phase.

In addition, liquid internal pressure gradient is produced by capillary force, that is:

$\frac{{\∂P}_l}{\∂x}=\frac{\∂\left(\mathrm{\σK}\right)}{\∂x}---\left(10\right)$

In formula, σ is liquid phase surface tension coefficient.

Convolution (8)-(10) can provide the kinematical equation about initial liquid film forming:

$\frac{\∂K}{\∂x}=\frac{3{\mathrm{\μ}}_l{U}_b}{\mathrm{\σ}{\mathrm{\δ}}^3}(\mathrm{\δ}-{\mathrm{\δ}}_0)---\left(11\right)$

Bretherton etc. are by being derived the dimension relation formula of liquid film and flow velocity by equation (11) to the simplification of liquid film curvature distribution.Thereafter when people are larger on flow velocity again, the impact of the effect such as inertial force conducts in-depth analysis, Youngbae Han and Naoki Shikazono continues to use the dimensional method of Bretherton, consider various effect and arrange film thickness measurement data (Naoki Shikazonoand Youngbae Han (2011) .Liquid Film Thickness in Micro-Scale Two-PhaseFlow in micro-pipe, Two Phase Flow, Phase Change and Numerical Modeling, Dr.AmimulAhsan (Ed.), ISBN:978-953-307-584-6, InTech), obtain following correlation:

$\frac{{\mathrm{\δ}}_0}{D}=\frac{0.670C{a}^{2/3}}{1+3.13C{a}^{2/3}+0.504C{a}^{0.672}{\mathrm{Re}}^{0.589}-0.352W{e}^{0.629}}---\left(12\right)$

In formula (12), D represents the diameter (D=2R) of micro-pipe; Ca=μ _lu _b/ σ is capillary constant; The computing formula of weber number We and reynolds number Re is:

$\mathrm{We}=\frac{{\mathrm{\ρ}}_l{U_b}^{2}D}{\mathrm{\σ}}---\left(13\right)$

$\mathrm{Re}=\frac{{\mathrm{\ρ}}_l{U}_{b}D}{{\mathrm{\μ}}_l}---\left(14\right)$

The scope of application of formula (12) is:

Ca＜0.3，Re＜2000 (15)

Formula (12) has accurately quantized the initial thickness of liquid film δ of Taylor bubble periphery ₀with the relation of capillary constant Ca, be applicable to the Taylor flowing of multiple fluid in micro-pipe that internal diameter is 0.3 ~ 1.3mm.

Based on the micro-thickness of liquid film δ of bubble that formula (12) represents ₀and the relation between capillary constant Ca, by adjustment air bubble flow rate, can obtain the δ under different Reynolds number Re condition ₀with Ca, W _erelational expression, thus solve the kinetic viscosity μ of liquid phase _lwith surface tension σ.

The utility model is according to thickness of liquid film δ initial bottom Taylor bubble in above-mentioned microtubule ₀with the quantitative relationship of capillary constant Ca, by the initial thickness of liquid film δ of bubble periphery in microtubule under measurement different in flow rate condition ₀, realize hydrodynamic viscosity, mu _lmeasure with while surface tension σ.

One, the first embodiment

In an exemplary embodiment of the present utility model, provide a kind of liquid parameter measuring system.Fig. 6 is the structural representation according to the utility model first embodiment liquid parameter measuring system.As shown in Figure 6, the present embodiment liquid parameter measuring system comprises: Taylor bubble flow generation device; Visual measurement microtubule 107, it has a microchannel, and the front end of this microchannel is connected with Taylor bubble flow generation device, and rear end is connected to returnable 108; Temperature sensor assembly, is arranged at the front-end and back-end of visual measurement microtubule 107; Thickness of liquid film measurement mechanism 109, is arranged at the periphery of visual measurement microtubule 107 radial direction; High speed camera 110, is arranged at the periphery of visual measurement microtubule 107 radial direction; And data acquisition and analytic system 113, be electrically connected to thickness of liquid film measurement mechanism 109 and high speed camera 110.

Wherein, the Taylor bubble flow of testing liquid is generated by Taylor bubble flow generation device, this Taylor bubble flow flows through visual measurement microtubule 107, measured the temperature of this Taylor bubble flow by temperature sensor assembly, measure the initial thickness of liquid film δ of bubble periphery in microchannel by thickness of liquid film measurement mechanism 109 through visual measurement microtubule 107 ₀, caught multiple instantaneous pictures of bubbly flow in microchannel through visual measurement microtubule 107 by high speed camera 110; Final Taylor bubble flow flows into returnable 108 and reclaims.Data acquisition and analytic system 113 obtain the apparent velocity U of bubble by multiple instantaneous pictures of bubble flow _b, and then by the initial thickness of liquid film δ of bubble periphery ₀, bubble apparent velocity U _b, the internal diameter D of visual measurement microtubule 107, the density p of testing liquid _lcalculate the kinetic viscosity μ of testing liquid _land/or surface tension σ.

Below each ingredient of the present embodiment liquid parameter measuring system is described in detail.

Please refer to Fig. 6, Taylor bubble flow generation device, for generating the Taylor bubble flow of testing liquid, comprising: drive motor 101, syringe 102, the first variable valve 103, compressed gas cylinder 104, the second variable valve 105 and the first three-way pipe 106.

The function of syringe 102 stores fluid to be measured, and the magnitude of its capacity is about 1ml ~ 10ml.The rear end of the piston core bar of this syringe 102 is driven by drive electrode 101, and its outlet is connected to the first pass-through interface of the first three-way pipe 106 by the first variable valve 103.Compressed gas source 104 is connected to the bypass interface of the first three-way pipe 106 by the second variable valve 105.Second pass-through interface of the first three-way pipe 106 is connected to the entrance of the microchannel of visual measurement microtubule 107.

Wherein, the function of drive motor 101 is for the flowing of fluid to be measured in micro-pipe provides power.The function of the first variable valve 103 is the flows regulating fluid to be measured, makes flowing keep stable.The function of compressed gas cylinder 104 is for Taylor stream provides stable filling bubble.The function of the second variable valve 105 regulates the flow of filling gas, Taylor flowed and keeps stable.The function of the first three-way pipe 106 is mixing fluids to be measured and fills gas, forms stable Taylor stream.Wherein, the first variable valve 103 and the second variable valve 105 can be arranged as required, in some cases, can omit the first variable valve 103.

Fig. 7 is the enlarged drawing of syringe in the measuring system of liquid parameter shown in Fig. 6.Please refer to Fig. 6 and Fig. 7, the outside of piston core bar is barrel, and the front end of piston core bar is sealed and matched by the barrel in O RunddichtringO and outside.Before measurement, syringe fills fluid to be measured.After drive motor 101 starts, promote piston core bar and travel forward, extruding testing liquid flows out, and enters first three-way pipe 106 after being regulated by the first variable valve 103.Open compressed gas cylinder 104, and regulate the aperture of the second variable valve 105, make filling gas slowly inject the first three-way pipe 106.The testing liquid flowed out in syringe 102 mixes in the first three-way pipe 106 with the filling gas that compressed gas cylinder flows out, and forms stable Taylor bubble flow.

In the present embodiment, the gas in compressed gas cylinder 104 is air, the apparent velocity U of the bubble of the Taylor bubble flow of formation _bfor 4m/s.But the utility model is not as limit, in other embodiments of the utility model, can also be other gases such as nitrogen in compressed gas cylinder, measure the surface tension coefficient of liquid in other gas, and the apparent velocity U of the bubble of Taylor bubble flow _bthe utility model can be realized between 0 ~ 10m/s.

Wherein, compressed gas cylinder 104 can be replaced by micro air pump.In this case, micro air pump can be fluid to be measured provides air to fill gas, thus forms stable Taylor steam bubble stream.

Also it should be noted that, provide a kind of specific Taylor bubble flow generation device in the present embodiment, but the utility model is not as limit.In other embodiments of the present utility model, the implementation of other a kind of Taylor bubble flow generation device will be provided.

The function of visual measurement microtubule 107 is for the flow process of Taylor bubble flow provides observation window, facilitates thickness of liquid film measurement mechanism 109 to measure thickness of liquid film, and high speed camera 110 catches flowing instantaneous picture.As shown in Figure 8, visual measurement microtubule 107 is the transparent glass tube of square-outside and round-inside.The diameter of microchannel is 0.5mm, but the utility model is not as limit.As long as the diameter of microchannel is not more than 1.5mm.Because the internal diameter of visual measurement microtubule 107 is very little, only need the fluid to be measured of 1ml ~ 10ml capacity magnitude to complete measuring process, liquid demand is very little.

Conveniently observation also convenience of calculation, the present embodiment adopts the transparent glass tube of square-outside and round-inside, but the utility model is not as limit.In other embodiments of the present utility model, the visual measurement microtubule of other shapes will be provided.It should be noted that in this case, the kinetic viscosity μ of testing liquid _lalso can correspondingly adjust with the computing formula of surface tension σ.

In the present embodiment, as long as ensure the measuring section transparent visual of visual measurement microtubule, the selection of visual measurement microtubule material is not by the impact of fluid to be measured wettability, and selectable range is wider, and for the visual measurement microtubule of same material, the type of its measurable liquid is also more.

Temperature sensor assembly comprises: the second temperature sensor 112 of the first temperature sensor 111 being positioned at the front end, microchannel of visual measurement microtubule 107 and the rear end, microchannel being positioned at visual measurement microtubule 107.The temperature of testing liquid can be obtained by the mean value of this first temperature sensor 111 and the second temperature sensor 112.Due to kinetic viscosity μ _lare all the parameters with temperature correlation with surface tension σ, therefore, obtain measuring tempeature, then calculate kinetic viscosity μ _lnamely be kinetic viscosity μ corresponding to this temperature with surface tension σ _lwith surface tension σ.

It should be noted that, the present embodiment comprises two temperature sensors, and the utility model is not as limit.And in other embodiments of the utility model, also only can adopt a temperature sensor, or when Current Temperatures is known, omit temperature sensor, can the utility model be realized equally.

The function of thickness of liquid film measurement mechanism 109 measures the thickness of the micro-liquid film of Taylor bubble periphery in microchannel.Existing many high-precision measuring methods and instrument at present, such as conventional confocal laser is apart from Displacement Meters (LFDM), and measuring error is only 1%, and precision, up to 0.01 μm, accurately can measure the thickness of liquid film of 10 ~ 600 μm of magnitudes.

It will be apparent to those skilled in the art that except confocal laser is except Displacement Meters, the instruments such as ellipsometer can also be adopted as thickness of liquid film measurement mechanism, can meet the demands as long as measuring accuracy is greater than 0.1 μm.

The function of high speed camera 110 is instantaneous pictures of Taylor bubble flow in capture channel, and the flow velocity being convenient to data acquisition and analytic system 113 pairs of Taylor streams carries out analytical calculation.Wherein, the capture rate of this high speed camera 110 should be not less than 1000 frames/second.

In the present embodiment, the capture rate of high speed camera 110 can reach 10000 frames/second, and shutter speed can reach the magnitude of 1 ~ 10 μ s usually; Be equipped with CCD camera lens and can reach the even less measuring accuracy of 0.01mm; The measuring error of thickness of liquid film can be controlled in about 1%.Therefore, measuring error is very little, far above common measuring method.

In order to eliminate the focusing error that outer tube wall curvature is brought, the curvature of the outside wall surface on thickness of liquid film measurement mechanism 109 and the visual measurement microtubule 107 corresponding to high speed camera 110 should be 0, namely this outside wall surface should be plane, otherwise measuring accuracy may be affected.

The temperature signal that data acquisition and analytic system 113 collecting temperature sensor (111 and 112) obtain and the initial thickness of liquid film δ that thickness of liquid film measurement mechanism 109 records ₀, the instantaneous picture of Taylor bubble flow that catches of high speed camera 110.First, the flow velocity U of bubble flow is obtained by multiple instantaneous pictures of Taylor bubble flow _b, and then according to formula (12 ~ 14) by the initial thickness of liquid film δ of bubble periphery ₀, bubble flow flow velocity U _b, the internal diameter D of microchannel of visual measurement microtubule 107, the density p of testing liquid _lthe kinetic viscosity μ of testing liquid under calculating Current Temperatures _lwith surface tension σ:

$\frac{{\mathrm{\δ}}_0}{D}=\frac{0.670C{a}^{2/3}}{1+3.13C{a}^{2/3}+0.504C{a}^{0.672}{\mathrm{Re}}^{0.589}-0.352W{e}^{0.629}}---\left(12\right)$

In formula (12), D represents the internal diameter (D=2R) of the microchannel of visual measurement microtubule 107; Ca=μ _lu _b/ σ is capillary constant; The computing formula of weber number We and reynolds number Re is:

$\mathrm{We}=\frac{{\mathrm{\ρ}}_l{U_b}^{2}D}{\mathrm{\σ}}---\left(13\right)$

$\mathrm{Re}=\frac{{\mathrm{\ρ}}_l{U}_{b}D}{{\mathrm{\μ}}_l}---\left(14\right)$

The micro-thickness of liquid film δ of the bubble that formula (12) represents ₀and the quantitative relationship between capillary constant Ca and the measuring system designed, this relational expression concludes by multiple fluid the rule-of-thumb relation obtained under multiple flox condition, widely applicable, and measuring accuracy is high.

In formula (12), there is the kinetic viscosity μ of two unknown quantity-testing liquids _lwith surface tension σ.When the surface tension σ of fluid to be measured is known, the kinetic viscosity μ that one-shot measurement (i.e. one group of Taylor bubble flow) obtains testing liquid can be passed through _l.As the kinetic viscosity μ of fluid to be measured _ltime known, the surface tension σ that one-shot measurement (i.e. one group of Taylor bubble flow) obtains testing liquid can be passed through.As kinetic viscosity μ _ltime all unknown with surface tension σ, can by regulating Taylor bubble flow parameter (testing liquid flow and/or blanketing gas amount), obtain two groups of Taylor bubble flows, and obtain two equations, the system of equations of these two equation compositions is solved, kinetic viscosity μ can be measured simultaneously _lwith surface tension σ.

Further, multiple spot repetitive measurement can also be done to same physical property, improve precision further, to meet the measurement requirement to the higher field such as scientific research, sophisticated technology of accuracy requirement.

It should be noted that, formula (12) ~ formula (14) is only the form of easy understand, in actual computation process, may adopt other equivalents derived by this formula, all should be included within protection domain of the present utility model.

Can find out, the present embodiment obtains the kinetic viscosity μ of fluid to be measured based on this same physical phenomenon of Taylor two-phase flow simultaneously _lwith surface tension σ, be not the combination of different measuring method, kinetic viscosity μ can be recorded more easily like this _lwith surface tension σ two parameters, and do not need to measure respectively different parameters, operate more easy.

Below introduce the workflow of the present embodiment liquid parameter measuring system.

Fig. 9 is the workflow diagram of the measuring system of liquid parameter shown in Fig. 6.Please refer to Fig. 8 and Fig. 9, this workflow comprises:

Steps A: produce Taylor bubble flow;

In the present embodiment, first, after the syringe 102 filling testing liquid is connected to system pipeline, drive motor 101 starts, and the liquid in pushing syringe 102, through the first variable valve 103, first three-way pipe 106, flows into visual measurement microtubule 107; Secondly, open compressed gas cylinder 104, and regulate the aperture of the second variable valve 105, make gas slowly inject the first three-way pipe 106, mix with the testing liquid flowed out in syringe 102, form stable Taylor bubble flow.

Step B: microchannel Taylor bubble flow being passed into visual measurement microtubule 107, measures the initial thickness of liquid film δ of bubble periphery in microchannel by thickness of liquid film measurement mechanism 109 ₀; Several instantaneous pictures of Taylor bubble flow in microchannel are caught by high speed camera 110; Measured the medial temperature of fluid to be measured by temperature sensor 111,112, fluid to be measured finally flows into returnable 108 and reclaims;

Step C: data acquisition and analytic system 113 obtain the flow velocity U of bubble flow by multiple instantaneous pictures of Taylor bubble flow _b;

Step D: data acquisition and analytic system 113 according to formula (12 ~ 14) by the initial thickness of liquid film δ of bubble periphery ₀, bubble flow flow velocity U _b, the internal diameter D of microchannel of visual measurement microtubule 107, the density p of testing liquid _lthe kinetic viscosity μ of testing liquid under calculating Current Temperatures _land/or surface tension σ.

It should be noted that, in the present embodiment steps A, be first open drive motor to make fluid to be measured flow into visual measurement microtubule 107, and then add bubble wherein, form stable Taylor bubble flow.And in other embodiments of the utility model, this step can be replaced by following steps: first open compressed gas cylinder 104, air is made to be full of visual measurement microtubule 107, and then start drive motor 101, in pushing syringe, the fluid to be measured of 102 flows, in the first three-way pipe 106, be mixed to form stable Taylor two-phase flow with air, can the utility model be realized equally.

So far, the present embodiment liquid parameter measuring system is introduced complete.

Two, the second embodiment

In second exemplary embodiment of the present utility model, additionally provide another kind of liquid parameter measuring system, the difference of itself and the first embodiment is, have employed different Taylor bubble flow generation devices.

Figure 10 is the structural representation according to Taylor bubble flow generation device in the utility model second embodiment liquid parameter measuring system.As shown in Figure 10, in the present embodiment, Taylor bubble flow generation device comprises: compressed gas cylinder 201; Reservoir 203, its pressure port is connected to the outlet of compressed gas cylinder 201 by the 3rd variable valve 202; Second three-way pipe 206, its first pass-through interface is connected to the liquid outlet of reservoir 203 by the 4th variable valve 204, its bypass interface is connected to compressed gas cylinder 201 by the 5th variable valve 205 and the 3rd variable valve 202 successively, and its second pass-through interface is as the outlet of Taylor bubble flow.

The present embodiment is compared with the first embodiment, and drive motor 101 is replaced by compressed gas cylinder 201; The flowing that compressed gas cylinder 201 1 aspect is fluid to be measured provides power, can provide stable filling bubble on the other hand.Syringe 102 is replaced by reservoir 203.

When measuring, open the 3rd variable valve 202, then the 4th variable valve 204, the 5th variable valve 205 is regulated respectively, testing liquid in reservoir 203 is pressed into the second three-way pipe 206 by the gas in compressed gas cylinder, this testing liquid mixes in the second three-way pipe 206 with compressed gas cylinder effluent air, form Taylor bubble flow, exported by the second pass-through interface of the second three-way pipe 206.

The course of work and first embodiment of the present embodiment are similar, no longer repeat to provide.

Three, the 3rd embodiment

In the 3rd exemplary embodiment of the present utility model, additionally provide another kind of liquid parameter measuring system, the difference of itself and the first embodiment is, have employed different visual measurement microtubules.

Figure 11 is the schematic cross-section according to visual measurement microtubule in the utility model the 3rd embodiment liquid parameter measuring system.In the present embodiment, visual measurement microtubule 107 is replaced by the structure of micro-square tube as shown in figure 11+micro-pipe+filled media.

Now, the overlay error caused is reflected continuously in order to reduce laser beam, the refractive index of filled media must as far as possible identical with the refractive index of micro-pipe with micro-square tube (difference of both Refractive Index of Materials is less than 0.1), as: when micro-square tube and micro-pipe are Pyrex glass (its refractive index is 1.474), filled media can adopt glycerine (its refractive index is 1.47).

Four, the 4th embodiment

The inner side of the visual measurement microtubule of first to fourth embodiment is circle, but in this enforcement, the inner side of visual measurement microtubule can also be that other have the rotational symmetry cross sectional shape of two and above axis of symmetry, such as rectangle, square, oval etc., can adopt similar theoretical analysis method to obtain following computation formula:

$\frac{{\mathrm{\δ}}_0}{D}=a+\frac{{b\·\mathrm{Ca}}^{2/3}}{1+c\·C{a}^{2/3}+d\·C{a}^m{\mathrm{Re}}^n-e\·W{e}^p}---\left(15\right)$

Wherein, a, b, c, d, e, m, n, p are the parameter relevant to the shape of the microchannel of visual measurement microtubule 107.

(1) for diameter be the circular microchannel of D, its internal diameter should be less than 1.5mm, and in formula (15), each parameter value is as follows:

a＝0，b＝0.67，c＝3.13，d＝0.504，e＝0.352

m＝0.672，n＝0.589，p＝0.629

Wherein, now, formula (15) is identical with formula (12);

(2) for the Rectangular Microchannel of high the ratio of width to height, during as the ratio of width to height W/D>=20, height D≤0.5mm, it is the coefficient that micro-pipe of D is identical that formula (12) can adopt with internal diameter, but the characteristic dimension D in formula (13), formula (14) must change the hydraulic diameter D of narrow Rectangular Microchannel into _h:

$D_h=\frac{4A}{U}=\frac{2(W\×D)}{W+D};\mathrm{We}=\frac{{\mathrm{\ρ}}_l{U_b}^2{D}_h}{\mathrm{\σ}};\mathrm{Re}=\frac{{\mathrm{\ρ}}_l{U}_b{D}_h}{{\mathrm{\μ}}_l}---\left(16\right)$

Formula (15) each parameter value is identical with circular microchannel, specific as follows:

a＝0，b＝0.67，c＝3.13，d＝0.504，e＝0.352

m＝0.672，n＝0.589，p＝0.629。

(3) for the length of side be the square microchannel of D, its equivalent diameter should be less than 1.5mm.Need the δ measured ₀for micro-thickness of liquid film of micro-square tube edge, i.e. δ _{0_corner}, as shown in figure 12.In formula (15), each coefficient value is as follows:

a＝0.243，b＝2.43，c＝7.28，d＝0，e＝0.255，p＝0.215

For other shapes, can be derived by similar method and draw, no longer describe in detail herein.Just, in order to the accuracy calculated is considered, preferably, the shape inside visual measurement microtubule is circular.

Wherein, as kinetic viscosity μ _lduring with one of them the unknown of surface tension σ, calculate unknown parameter by the measured value of one group of Taylor bubble flow according to described computing formula; Or as kinetic viscosity μ _ltime all unknown with surface tension σ, build the system of equations about described computing formula by the measured value of two groups of different Taylor bubble flows, calculating kinetic viscosity μ by solving this system of equations _lwith surface tension σ.

So far, by reference to the accompanying drawings the multiple embodiment of the utility model has been described in detail.Describe according to above, the system and method that those skilled in the art should measure the utility model liquid parameter has had clearly to be familiar with.

In addition, the above-mentioned definition to each element and method is not limited in various concrete structures, shape or the mode mentioned in embodiment, those of ordinary skill in the art can change simply it or replace, such as: adopt except circle or square except other shapes as the inner shape of visual measurement microtubule; Adopt other devices except Taylor air Bubble generating apparatus in above-mentioned two embodiments to produce Taylor bubble etc., all should be included within protection domain of the present utility model.

In sum, the utility model obtains the kinetic viscosity μ of fluid to be measured simultaneously based on this same physical phenomenon of Taylor two-phase flow _lwith surface tension σ, system architecture is simple, and it is convenient to measure, and precision is higher, has high application value.

Above-described specific embodiment; the purpose of this utility model, technical scheme and beneficial effect are further described; be understood that; the foregoing is only specific embodiment of the utility model; be not limited to the utility model; all within spirit of the present utility model and principle, any amendment made, equivalent replacement, improvement etc., all should be included within protection domain of the present utility model.

Claims (15)

1. a liquid parameter measuring system, is characterized in that, comprising:

Taylor bubble flow generation device;

Visual measurement microtubule (107), it has a microchannel, and the front end of this microchannel is connected with described Taylor bubble flow generation device;

Camera (110), is arranged at the radial outer periphery of described visual measurement microtubule (107); And

Thickness of liquid film measurement mechanism (109), is arranged at the radial outer periphery of described visual measurement microtubule (107);

Wherein, described Taylor bubble flow generation device generates the Taylor bubble flow of testing liquid, this Taylor bubble flow flows through the microchannel of described visual measurement microtubule (107), and described thickness of liquid film measurement mechanism (109) measures the initial thickness of liquid film δ of bubble periphery in microchannel through visual measurement microtubule ₀, described camera (110) catches multiple instantaneous pictures of bubbly flow in microchannel through visual measurement microtubule.

2. liquid parameter measuring system according to claim 1, is characterized in that, described Taylor bubble flow generation device comprises: actuator, syringe (102), compressed gas source and the first three-way pipe (106);

Described actuator withstands the rear end of the piston core bar of described syringe (102); The first interface of described first three-way pipe (106) is connected to the outlet of described syringe (102), and its 3rd interface is connected to the outlet of described compressed gas source, and its second interface is as the outlet of Taylor bubble flow;

Described syringe (102) injects fluid to be measured; Described actuator promotes the piston core bar motion of described syringe (102), and extruding testing liquid flows out, and enters the first three-way pipe (106); This testing liquid mixes in the first three-way pipe (106) with compressed gas source effluent air, forms Taylor bubble flow, is exported by the second interface of described first three-way pipe (106).

3. liquid parameter measuring system according to claim 2, is characterized in that, described actuator is drive motor (101).

4. liquid parameter measuring system according to claim 2, is characterized in that, described Taylor bubble flow generation device also comprises:

First variable valve (103), is arranged between the outlet of described syringe (102) and the first interface of described first three-way pipe (106); And/or

Second variable valve (105), is arranged between described compressed gas source and the 3rd interface of described first three-way pipe (106).

5. liquid parameter measuring system according to claim 1, is characterized in that, described Taylor bubble flow generation device comprises:

Compressed gas source;

Reservoir (203), its pressure port is connected to the outlet of described compressed gas source; And

Second three-way pipe (206), its first interface is connected to the liquid outlet of described reservoir (203), and its 3rd interface is connected to the outlet of described compressed gas source, and its second interface is as the outlet of Taylor bubble flow;

Wherein, gas in described compressed gas source is by described second three-way pipe (206) of testing liquid press-in in described reservoir (203), this testing liquid mixes in the second three-way pipe (206) with compressed gas source effluent air, form Taylor bubble flow, exported by the second interface of described second three-way pipe (206).

6. liquid parameter measuring system according to claim 5, is characterized in that, described Taylor bubble flow generation device also comprises:

3rd variable valve (202), is arranged between the outlet of described compressed gas source and the pressure port of described reservoir (203);

4th variable valve (204), is arranged between the liquid outlet of described reservoir (203) and the first interface of the second three-way pipe (206);

5th variable valve (205), is arranged between the 3rd interface of described second three-way pipe (206) and described 3rd variable valve (202).

7. the liquid parameter measuring system according to any one of claim 2 to 6, is characterized in that, described compressed gas source is compressed gas cylinder (104) or air pump.

8. liquid parameter measuring system according to claim 1, is characterized in that, described visual measurement microtubule is plane with described camera (110), outside wall surface that thickness of liquid film measurement mechanism (109) is relative.

9. liquid parameter measuring system according to claim 1, is characterized in that, the xsect of the microchannel of described visual measurement microtubule is in the axisymmetric shape with two and above axis of symmetry.

10. liquid parameter measuring system according to claim 9, is characterized in that, the xsect of the microchannel of described visual measurement microtubule is:

Circle, its diameter is less than 1.5mm;

Square, its equivalent diameter is less than 1.5mm; Or

Rectangle, its ratio of width to height W/D >=20, and height D≤0.5mm.

11. liquid parameter measuring systems according to claim 10, is characterized in that, the xsect of the microchannel of described visual measurement microtubule is circular, described visual measurement microtubule:

For the transparent glass tube of square-outside and round-inside, or

Comprise: micro-square tube; Be positioned at micro-pipe of micro-square tube; And the filled media be filled between described micro-square tube and micro-pipe; Wherein, described micro-square tube is identical with the material of micro-pipe, and the refractive index of described filled media material and the specific refractivity of described micro-square tube material are less than 0.1.

12. liquid parameter measuring systems according to claim 1, is characterized in that, also comprise:

Data acquisition and analytical equipment (113), be connected with thickness of liquid film measurement mechanism (109) with described camera (110), its multiple instantaneous pictures utilizing described camera (110) to catch bubbly flow obtain the apparent velocity U of bubble _b, and then utilize the internal diameter D of microchannel, the density p of testing liquid of visual measurement microtubule (107) _l, the initial thickness of liquid film δ of bubble periphery ₀, bubble apparent velocity U _bcalculate the kinetic viscosity μ of testing liquid _land/or surface tension σ.

13. liquid parameter measuring systems according to any one of claim 1 to 6,8 to 12, it is characterized in that, the measuring accuracy of described thickness of liquid film measurement mechanism (109) is greater than 0.1 μm; The capture rate of described camera (110) is not less than 1000 frames/second.

14. liquid parameter measuring systems according to claim 13, is characterized in that, described thickness of liquid film measurement mechanism (109) is for confocal laser is apart from Displacement Meters or ellipsometer.

15. liquid parameter measuring systems according to any one of claim 1 to 6,8 to 12, is characterized in that, also comprise:

Temperature sensor (111,112), is arranged at front end and/or the rear end of the microchannel of described visual measurement microtubule (107); And/or

Returnable (108), is connected to the rear end of the microchannel of described visual measurement microtubule (107).