CN204924854U - Viscosimeter based on electromechanical impedance method - Google Patents

Abstract

The utility model discloses a viscosimeter based on electromechanical impedance method. The utility model discloses a viscosimeter includes: piezoelectricity roof beam, fixed station, impedance analyzer and computer, wherein, piezoelectricity roof beam involving vibrations piece, cantilever beam and piezoelectric patches, the one end of cantilever beam is fixed on the fixed station, and the other end is the free end, be provided with the trembler on the free end of cantilever beam, paste the piezoelectric patches that has thickness the same respectively on two surfaces of cantilever beam, the piezoelectric patches is connected to impedance analyzer. The utility model discloses a measuring the resonance frequency of the electromechanical impedance of piezoelectricity roof beam, calculating the dynamic viscosity who obtains being surveyed liquid, the method is accurate reliable, because the measurement of electromechanical impedance is very accurate, so rather than relevant also can accurately being obtained by the viscosimetric value, and the test part is the piezoelectricity roof beam, its test mode is simple and convenient, receives space geometrical constraint little, and test performance can all keep good stability under environment such as various temperature, atmospheric pressure, so can satisfy different environment's in situ test requirement.

Description

A kind of viscosity meter based on dynamo-electric impedance method

Technical field

The utility model relates to viscosity meter preparation field, is specifically related to a kind of viscosity meter based on dynamo-electric impedance method.

Background technology

During liquid flow, the character rubbed in intermolecular generation, is called the viscosity of liquid, and the size of viscosity represents by viscosity.Viscosity is one of the index needing in many commercial production to monitor, and viscometric principle is mostly generally derive expression formula about the coefficient of viscosity by Stokes formula and Poiseuille's formula, tries to achieve the coefficient of viscosity.The mensuration of viscosity parameter, for the prediction technology controlling and process of process of producing product, transporting and product operability in use, has important guiding value, has great significance in all conglomeraties such as chemical industry, printing, medicine, oil, automobiles.

At present, the viscosity meter for measuring kinematic viscosity comprises capillary type, rotary and oscillatory type.Capillary viscosimeter is generally Saybolt viscosimeter, is a kind of common viscosity meter.Under constant temperature and pressure condition, fluid to be measured is utilized to flow through the viscosity of the time calculation sample of regular length kapillary.Common rotary viscosimeter is cone and plate viscometer, to utilize under steady flow condition fluid to border with constant acting force, by the moment of torsion of cylindrical boundary and the viscosity reflecting sample.Vibration viscometer utilizes the resistance being subject to fluid during the object vibration in fluid to obtain the viscosity of fluid, certainly the size of this acting force is relevant with the viscosity of fluid, but because this acting force can not directly record, so common vibration viscometer is all the viscosity indirectly being obtained fluid to be measured by measurement mechanical impedance.

Utility model content

In order to realize the Measurement accuracy of viscosity, the utility model proposes a kind of viscosity meter based on dynamo-electric impedance method, utilizing dynamo-electric impedance method to carry out tested viscosity, the viscosity of fluid to be measured can be reflected exactly, can in site measurement be realized again.

The purpose of this utility model is to propose a kind of viscosity meter based on dynamo-electric impedance method.

Viscosity meter based on dynamo-electric impedance method of the present utility model comprises: piezoelectric beam, fixed station, electric impedance analyzer and computing machine; Wherein, piezoelectric beam involving vibrations sheet, semi-girder and piezoelectric patches; One end of semi-girder is fixed on fixed station, and the other end is free end; The free end of semi-girder is provided with vibrating reed, the axis of symmetry of semi-girder and the axis of symmetry conllinear of vibrating reed, and the plane at the plane at semi-girder place and vibrating reed place is orthogonal; Vibrating reed immerses in fluid to be measured; Two surfaces of semi-girder are pasted with the identical piezoelectric patches of thickness respectively; Piezoelectric patches is connected to electric impedance analyzer; Electric impedance analyzer is connected to computing machine.

Such as, measure the admittance value of piezoelectric beam at each Frequency point, thus obtain the resonant frequency of piezoelectric beam, obtain the kinetic viscosity of fluid to be measured according to resonant frequency.

Semi-girder adopts the material of rigidity, as steel disc, to ensure having certain rigidity.

Vibrating reed is the shape of rule, and thickness h is between 0.1mm ~ 0.2mm, and material is identical with semi-girder.

The utility model arranges vibrating reed at the free end of semi-girder, the direction of vibration of vibrating reed is parallel with the plane at vibrating reed place, after vibrating reed immerses fluid to be measured, the skin-friction force of the vibrating reed caused by the viscosity of liquid will change the resonant frequency of piezoelectric beam, measure and obtain the resonant frequency relevant with the viscosity of liquid, and then by setting up mechanical model, recycling the resonant frequency recorded and calculating the kinetic viscosity obtaining fluid to be measured.Vibrating reed, semi-girder and piezoelectric patches constitute dynamo-electric impedance coupler system, by measuring the resonant frequency of the dynamo-electric impedance (admittance) of piezoelectric beam, calculate the kinetic viscosity of fluid to be measured.

The method of testing of the viscosity meter based on dynamo-electric impedance method of the present utility model, comprises the following steps:

1) according to the range of viscosities of fluid to be measured, arrange the test parameter of computing machine, test parameter comprises swept frequency range f ₁~ f ₂and driving voltage, wherein, f ₁and f ₂be respectively initial frequency and stop frequency;

2) vibrating reed is immersed in fluid to be measured completely, the stiff end of fixing piezoelectric beam;

3) according to the swept frequency range of setting, from f ₁~ f ₂sweep check is carried out in pointwise, obtains the admittance Y of each Frequency point, obtains the frequency response curve of frequency and admittance;

4) according to frequency response curve, if obtain resonant frequency f ₀, then step 5 is entered), if do not obtain resonant frequency, then return step 1), adjustment swept frequency range re-starts measurement;

5) the kinetic viscosity η obtaining fluid to be measured is calculated according to the resonant frequency recorded:

$\mathrm{\η}=j{\[\frac{1}{2{\mathrm{A\ω}}_0}\left(m_t{\mathrm{\ω}}_0^2+\stackrel{\‾}{k_b}{\mathrm{\λ}}_{b0}^3\frac{1+{\mathrm{cos\λ}}_{b0}L{\mathrm{cos\λ}}_{b0}L}{{\mathrm{cos\λ}}_{b0}L{\mathrm{sinh\λ}}_{b0}L-{\mathrm{sin\λ}}_{b0}L{\mathrm{cosh\λ}}_{b0}L}\right)\]}^2/{\mathrm{\ω}}_0\mathrm{\ρ}$

Wherein, ω ₀for resonant angular frequency, ω ₀=2 π f ₀f ₀for resonant frequency, A is the area of vibrating reed, m _tfor the lumped mass that piezoelectric beam free end simplifies, for the equivalent stiffness of piezoelectric beam, for piezoelectric beam linear mass, L is the length of piezoelectric beam, $j=\sqrt{-1},{\mathrm{\λ}}_{b0}={({\mathrm{\ω}}_0^2{\stackrel{\‾}{\mathrm{\ρ}}}_b/{\stackrel{\‾}{K}}_b)}^{1/4},$ ρ is the density of fluid to be measured.

Advantage of the present utility model:

The utility model, by measuring the resonant frequency of dynamo-electric impedance of piezoelectric beam, calculates the kinetic viscosity of fluid to be measured, method accurately and reliably, because the measurement of dynamo-electric impedance is very accurate, so relative tested viscosity number also can accurately obtain; Further, test component of the present utility model is piezoelectric beam, and its test mode is easy, and little by space geometry constraint, test performance can keep good stability, so can meet the in-situ test requirement of varying environment under the environment such as various temperature, air pressure.

Accompanying drawing explanation

Fig. 1 is the schematic diagram of the viscosity meter based on dynamo-electric impedance method of the present utility model;

Fig. 2 is the schematic diagram of the piezoelectric beam of the viscosity meter based on dynamo-electric impedance method of the present utility model;

Fig. 3 is the mechanical simplified model figure of the piezoelectric beam of the viscosity meter based on dynamo-electric impedance method of the present utility model;

Fig. 4 is the equivalent circuit diagram of the piezoelectric beam of the viscosity meter based on dynamo-electric impedance method of the present utility model;

Fig. 5 is the curve map of resonant frequency with the viscosity B coefficent of liquid of the viscosity meter based on dynamo-electric impedance method of the present utility model.

Embodiment

Below in conjunction with accompanying drawing, by specific embodiment, set forth the utility model further.

As shown in Figure 1, the viscosity meter based on dynamo-electric impedance method of the present embodiment comprises: piezoelectric beam 2, fixed station 3, electric impedance analyzer 4 and computing machine 5; Wherein, as shown in Figure 2, piezoelectric beam 2 involving vibrations sheet 21, semi-girder 22 and piezoelectric patches 23; One end of semi-girder 22 is fixed on fixed station 3, and the other end is free end; The free end of semi-girder is provided with vibrating reed 21, and the axis of symmetry of semi-girder 22 is positioned at the plane at vibrating reed 21 place, and the plane at semi-girder place and the plane at vibrating reed place orthogonal; Two surfaces of semi-girder are pasted with two pieces of thickness identical piezoelectric patches 23 respectively; Piezoelectric patches is connected to electric impedance analyzer 4; Electric impedance analyzer 4 is connected to computing machine 5; Vibrating reed 21 immerses in fluid to be measured 1.Semi-girder 22 adopts steel disc, and vibrating reed 21 is circular, and vibrating reed and semi-girder all adopt steel disc.

When the vibrating reed of piezoelectric beam free end immerses in fluid to be measured, the mechanical simplified model of piezoelectric beam as shown in Figure 3.Wherein, L represents the length of piezoelectric beam, h _pand 2h _mbe respectively the thickness of piezoelectric patches and semi-girder, m _tfor the lumped mass that piezoelectric beam free end simplifies, c _trepresent the damping because fluid to be measured viscosity causes, here a is the area of vibrating reed, ω is angle of throw frequency and has ω=2 π f, and f is vibration frequency, and η is kinetic viscosity, and ρ is the density of fluid to be measured.According to the above model simplified, obtain the vibration equation of piezoelectric beam:

${\stackrel{\‾}{K}}_b\frac{{\∂}^{4}u}{\∂x^4}+{\stackrel{\‾}{\mathrm{\ρ}}}_b\frac{{\∂}^{2}u}{\∂t^2}=0---\left(1\right)$

Wherein, for the equivalent stiffness of piezoelectric beam, for the linear mass of piezoelectric beam, x and u is respectively transverse and longitudinal coordinate, and t is the time.

$\begin{array}{c}{\stackrel{\‾}{K}}_b=\frac{2}{3}w\[\frac{1}{S_{p_{11}}^E}\left({\left(h_p+h_m\right)}^3-h_m^3\right)+\frac{1}{S_{m_{11}}}{h}_m^3\]\\ {\stackrel{\‾}{\mathrm{\ρ}}}_b=2w\left({\mathrm{\ρ}}_p{h}_p+{\mathrm{\ρ}}_m{h}_m\right)\end{array}---\left(2\right)$

Wherein, ρ _pand ρ _mbe respectively the density of piezoelectric patches and semi-girder, with be respectively the elastic constant of piezoelectric patches and steel disc.

Boundary condition can be expressed as:

$u=0{|}_{x=0},\frac{\∂u}{\∂x}=0{|}_{x=0},\frac{{\∂}^{2}u}{\∂x^2}=0{|}_{x=L},\frac{{\∂}^{3}u}{\∂x^3}=\frac{\∂u}{\∂t}{c}_t{|}_{x=L}---\left(3\right)$

Like this, the general solution of equation (1) can be expressed as:

u＝[α ₁cosλ _bx+α ₂sinλ _bx+α ₃coshλ _bx+α ₄sinhλ _bx]e ^jωt(4)

Wherein α ₁, α ₂, α ₃and α ₄be respectively undetermined constant.

Correlative study shows, the vibrational system that piezoelectric beam is formed, and can replace with equivalent electrical circuit, the circuit diagram of equivalent electromechanical coupled circuit as shown in Figure 4.According to piezoelectricity continuity equation, in equivalent electromechanical coupled circuit, electric current I can be represented as:

$I=-N\frac{{\∂}^{2}u}{\∂x\∂t}{|}_{x=0}^{x=L}+C_c\frac{\∂V}{\∂t}---\left(5\right)$

Wherein: N is conversion coefficient, C _cfor equivalent capacity, V is on-load voltage.

$N=-\frac{d_{31}}{S_{p_{11}}^E}w\left(\frac{h_p+2h_m}{2}\right)---\left(6\right)$

$C_c=\frac{p_{33}^{\mathrm{\σ}}wL}{2h_p}\left(1-\frac{d_{31}^2}{S_{p_{11}}^E{p}_{33}^{\mathrm{\σ}}}\right)---\left(7\right)$

Wherein, d ₃₁for the piezoelectric constant of piezoelectric patches, for the specific inductive capacity of piezoelectric patches.

In addition, phase parameter C in Fig. 4 _m=-C _c/ N ², Z _a~ Z _cimpedance parameter is defined as foloows:

$Z_a=\frac{{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b}{j\mathrm{\ω}}\frac{sm-cn}{1-cm}-\frac{{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b^2}{j\mathrm{\ω}}\frac{sn}{1-cm}-\frac{N^2}{{\mathrm{j\ωC}}_c}$

$Z_b=\frac{{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b^2}{j\mathrm{\ω}}\frac{sn}{1-cm}---\left(8\right)$

$Z_a=\frac{{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b^3}{j\mathrm{\ω}}\frac{cn+sm}{1-cm}-\frac{{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b^2}{j\mathrm{\ω}}\frac{sn}{1-cm}$

Wherein, c=cos λ _bl, s=sin λ _bl, m=cosh λ _bl, n=sinh λ _bl.

Can be calculated by above a few formula, the admittance Y of piezoelectric beam is:

$Y=j\mathrm{\ω}\left(C_c+\frac{N^2}{{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b}\frac{cn+sm+cm\mathrm{\β}-\mathrm{\β}}{1+cm+sm\mathrm{\β}-cn\mathrm{\β}}\right)---\left(9\right)$

Wherein, $\mathrm{\β}=(-{\mathrm{\ω}}^2{m}_t+k_t)/{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_b^3.$

As the resonant frequency ω that frequency is piezoelectric cantilever ₀time, admittance can reach maximal value, so have:

1+cm+smβ ₀-cnβ ₀＝0(10)

In addition, β ₀and λ _b0also be the parameter value obtained at resonant frequency place, so have:

$\begin{array}{c}{\mathrm{\β}}_0=\left(-{\mathrm{\ω}}_0^2{m}_t+k_t\right)/{\stackrel{\‾}{K}}_b{\mathrm{\λ}}_{b0}^3\\ {\mathrm{\λ}}_{b0}={\left({\mathrm{\ω}}_0^2{\stackrel{\‾}{\mathrm{\ρ}}}_b/{\stackrel{\‾}{K}}_b\right)}^{1/4}\end{array}---\left(11\right)$

According to above expression formula, ratio of damping c can be calculated _tfor:

$c_t=\frac{1}{{\mathrm{j\ω}}_0}\left(m_t{\mathrm{\ω}}_0^2+{\stackrel{\‾}{k}}_b{\mathrm{\λ}}_{b0}^3\frac{1+{\mathrm{cos\λ}}_{b0}L{\mathrm{cosh\λ}}_{b0}L}{{\mathrm{cos\λ}}_{b0}L{\mathrm{sinh\λ}}_{b0}L-{\mathrm{sin\λ}}_{b0}L{\mathrm{cosh\λ}}_{b0}L}\right)---\left(12\right)$

Again so finally calculate the kinetic viscosity of fluid to be measured:

$\mathrm{\η}=j{\[\frac{1}{2{\mathrm{A\ω}}_0}\left(m_t{\mathrm{\ω}}_0^2+{\stackrel{\‾}{k}}_b{\mathrm{\λ}}_{b0}^3\frac{1+{\mathrm{cos\λ}}_{b0}L{\mathrm{cosh\λ}}_{b0}L}{{\mathrm{cos\λ}}_{b0}L{\mathrm{sinh\λ}}_{b0}L-{\mathrm{sin\λ}}_{b0}L{\mathrm{cosh\λ}}_{b0}L}\right)\]}^2/{\mathrm{\ω}}_0\mathrm{\ρ}---\left(13\right)$

Known according to formula (13), once record the resonant frequency of the dynamo-electric impedance (admittance etc.) of piezoelectric beam, the kinetic viscosity of fluid to be measured can be calculated.Simultaneously known according to solution (13), along with the increase of viscosity, each rank resonance of piezoelectric cantilever will reduce gradually, as shown in Figure 5.

The range of viscosities of fluid to be measured can be obtained by the viscosity of common liquid and density value table.Following table is 25 DEG C, the viscosity of common liquid under normal pressure and density value table:

It is finally noted that, the object publicizing and implementing example is to help to understand the utility model further, but it will be appreciated by those skilled in the art that: in the spirit and scope not departing from the utility model and appended claim, various substitutions and modifications are all possible.Therefore, the utility model should not be limited to the content disclosed in embodiment, and the scope that the claimed scope of the utility model defines with claims is as the criterion.

Claims (4)

1. based on a viscosity meter for dynamo-electric impedance method, it is characterized in that, described viscosity meter comprises: piezoelectric beam, fixed station, electric impedance analyzer and computing machine; Wherein, described piezoelectric beam involving vibrations sheet, semi-girder and piezoelectric patches; One end of described semi-girder is fixed on fixed station, and the other end is free end; The free end of semi-girder is provided with vibrating reed, the axis of symmetry of semi-girder and the axis of symmetry conllinear of vibrating reed, and the plane at the plane at semi-girder place and vibrating reed place is orthogonal; Described vibrating reed immerses in fluid to be measured; Two surfaces of semi-girder are pasted with the identical piezoelectric patches of thickness respectively; Described piezoelectric patches is connected to electric impedance analyzer; Described electric impedance analyzer is connected to computing machine.

2. viscosity meter as claimed in claim 1, is characterized in that, described vibrating reed is the shape of rule.

3. viscosity meter as claimed in claim 1, it is characterized in that, the thickness of described vibrating reed is between 0.1mm ~ 0.2mm.

4. viscosity meter as claimed in claim 1, is characterized in that, described semi-girder adopts the material of rigidity.