JPH10104040A - Mass flowmeter converter - Google Patents

Abstract

PROBLEM TO BE SOLVED: To perform the simple correction of an instrumental error without the complicated operation of a vibrating system. SOLUTION: A coaxial double vibrating pipe 10 is constituted of an inner tube 1 and an outer tube 2. A vibrator 5 is provided at the center of the coaxial double vibrating pipe 10, and sensors 6 and 7 are provided at the symmetrical positions from the center. When the vibrator 5 is driven at the resonant frequency with a driving circuit 20, a mass flow rate Q in proportion to a phase difference signal ΔT at the sensors 6 and 7 is obtained. An instrumental-difference change ΔE, which is generated from the change in temperature (t) and density ρ of fluid to be measured flowing in the inner tube 1 with respect to the obtained mass flow rate, is determined as the sum of the following instrumental differences: the first instrumental-difference correcting value Ct from the temperature difference of the reference temperature and the actually measured temperature of the inner tube, the second instrumental- difference correcting value Cdt based on the temperature difference of the inner tube 1 and the outer tube 2 and third instrumental-difference correcting value Cf obtained with the instrumental error by the density difference of the fluid to be measured as the frequency difference. The mass flow rate Qa to be corrected is determined as Q(1+ΔE).

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a mass flow meter converter, and more particularly, to a method for easily correcting an instrumental difference caused by a change in temperature and density of a fluid to be measured in a coaxial double straight tube type Coriolis flow meter. Mass flow meter converter.

[0002]

2. Description of the Related Art As is well known, a Coriolis flowmeter supports a measuring tube through which a fluid to be measured flows at both ends, and alternately drives a central portion of the supported measuring tube in a direction perpendicular to a supporting line of the measuring tube. Then, a direct type mass flow meter that detects a phase difference signal proportional to the Coriolis force generated at a symmetrical position between both ends of the measuring tube at both ends and the central part and obtains a mass flow rate proportional to the Coriolis force is obtained. is there. Thus, the phase difference signal is an amount proportional to the mass flow rate, and when the drive frequency is fixed,
The phase difference can be detected as a time difference at a symmetric position of the measuring tube.

If the driving frequency for driving the measuring tube is made equal to the natural frequency of the measuring tube, a constant driving frequency corresponding to the density of the measuring tube and the fluid to be measured can be obtained, and it is possible to drive with a small driving energy. Therefore, it is general to drive the measuring tube at the natural frequency, and the phase difference signal is detected as a time difference signal.

The applicant of the present invention has previously constructed a coaxial double straight tube comprising an inner tube as a measuring tube through which a fluid to be measured flows, and an outer tube supported at both ends outside the inner tube. We have proposed a Coriolis flow meter with a coaxial double straight pipe (double vibrating pipe) equipped with a balance weight at the center of the outer tube to make the natural frequency equal to the natural frequency of the inner tube.

[0005]

The coaxial double straight pipe type Coriolis flowmeter is configured such that the external piping and the inner tube are coaxially connected, so that foreign matter adhering to the inner wall can be easily removed. There is an advantage that the installation space is reduced by only slightly increasing the outer shape with respect to the external piping. But,
The fluid to be measured flows through the inner tube of the coaxial double straight pipe,
In general, the fluids to be measured are diverse, and it is assumed that the temperature and density are different from each other.Therefore, the natural frequency changes due to the physical properties of these fluids to be measured. Change. Therefore, in the coaxial double straight tube type Coriolis flowmeter, it is necessary to correct an instrumental difference caused by the physical properties of the fluid to be measured.

The present invention has been made in view of the above-mentioned circumstances, and substantially eliminates the instrumental error of a coaxial double straight pipe type Coriolis flowmeter caused by a change in the temperature or density of a fluid to be measured. In addition, in order to perform correction of each instrumental error caused by the above-mentioned temperature and density, each instrumental error correction amount is determined based on a measured value of a fluid which has been calibrated and standardized in advance, and is always compared with the measured value. Accordingly, it is an object of the present invention to provide a mass flow meter computing device capable of easily correcting instrumental differences.

[0007]

According to a first aspect of the present invention, there is provided a coaxial double straight tube comprising an inner tube through which a fluid to be measured flows, and an outer tube having both ends fixed to the outside of the inner tube. A double vibrating tube attached to the outer tube with a balance weight having a weight that makes the natural frequency of the outer tube equal to the natural frequency of the inner tube; and Driving means for driving, a pair of sensors for detecting a phase displacement proportional to the Coriolis force acting on the double vibrating tube by the driving, and a mass flow rate of a Coriolis flow meter for obtaining a mass flow rate based on an output of the sensor In the meter converter, the inner tube and the outer tube have temperature detecting means for detecting the temperatures of the inner tube and the outer tube, respectively, Temperature correction means for correcting an instrumental difference based on a temperature change of the inner tube, temperature difference correcting means for correcting an instrumental difference based on a temperature difference between the inner tube and the outer tube, and Resonance frequency correction means for correcting an instrumental difference due to a frequency difference between a resonance frequency of the heavy vibration tube and a previously known resonance frequency of the double vibration tube when flowing a fluid having a reference density, wherein the temperature correction is performed. Means, a temperature difference correcting means, and an instrumental error correction means for adding the instrumental error correction amounts of the resonance frequency correcting means, and correcting the instrumental error based on the added instrumental error correction amount.

[0008]

DETAILED DESCRIPTION OF THE INVENTION According to the first aspect of the present invention, the inner tube is thermally deformed due to a change in the temperature of the fluid to be measured due to the instrumental difference of the coaxial double straight tube type Coriolis flowmeter. It is classified into an instrumental error correction amount of 1, a second instrumental error correction amount caused by a temperature difference between the inner tube and the outer tube, and a third instrumental error correction amount by a frequency difference of a resonance frequency based on a density change of the fluid to be measured. The first instrumental error correction amount is obtained by multiplying a temperature difference between a reference temperature (for example, 0 ° C.) and a temperature at the time of measurement of the inner tube by a predetermined correction coefficient per 1 ° C. The second instrumental error correction amount is an instrumental error correction amount caused by a predetermined temperature difference between the inner tube and the outer tube, and the third instrumental error correction amount is the amount of the fluid to be measured flowing through the inner tube. The instrumental error correction amount caused by the difference in density The instrument difference correction amount caused by the frequency difference between the corrected and standardized resonance frequency of the fluid and the resonance frequency of the measured fluid, and the instrument difference caused by the temperature difference between the temperature of the measured fluid and a reference temperature (for example, 0 ° C.). The correction amount and the combined instrumental difference amount are defined as the first instrumental difference correction amount and the second
And the third instrumental error correction amount is added to perform the instrumental error correction.

FIG. 1 is a diagram for explaining a mass flow meter converter according to the present invention. In the figure, 1 is an inner tube, 2
Is an outer tube, 3 and 4 are annular flanges, 5 is a shaker,
6, 7 are sensors, 8 is a balance weight, 9a and 9b are temperature sensors, 10 is a coaxial double vibrating tube (hereinafter, referred to as a double vibrating tube), 20 is a drive circuit, 30 is a resonance frequency detecting circuit, and 40 is a resonant frequency detecting circuit. Instrument error correction circuit, 50 is a mass flow calculation circuit, 5
1 is an output terminal, 60 is a mass flow meter converter. The double vibration tube 10 includes an inner tube 1, an outer tube 2, and a balance weight 8. The inner tube 1
A straight pipe around the axis 0-0 through which the fluid to be measured flows,
The outer tube 2 has annular flanges 3 and 4 at both ends,
It is coaxially fixed to the axis 0-0 via the annular flanges 3 and 4 outside the inner tube 1 to form a coaxial double straight pipe. The balance weight 8 is fixed to the center of the outer wall of the outer tube 2. The balance weight 8 is a weight for making the natural frequency of the outer tube 2 equal to the natural frequency of the inner tube 1.

The weight of the balance weight 8 is adjusted in accordance with the determined natural frequency including the weight of the vibrator 5 for driving the double vibrating tube 10 and the weights of the sensors 6 and 7. A temperature sensor 9a for detecting the temperature of the inner tube 1 is mounted on the outer wall of the inner tube 1 of the double vibrating tube 10, and a temperature sensor 9b for detecting the temperature of the outer tube 2 is mounted on the outer wall of the outer tube 2. The outer tube 2 is connected to the instrument difference correction circuit 40 through a through hole (not shown) or a connection terminal (not shown).

The vibrator 5 includes, for example, a coil 5a provided on the outer tube 2 and a core 5b provided coaxially with the coil 5a on the inner tube 1. The coil 5a is connected to one of the sensors (described later). In FIG. 1, the signal from the sensor 6) is driven by the driving circuit 20 to drive the double vibration tube 10 including the inner tube 1 and the outer tube 2 at a resonance frequency of a constant amplitude.

The sensors 6 and 7 are of the same standard, and are installed at symmetric positions with respect to the vibrator 5 on a double straight pipe.
For example, the coils 6a, 7a provided on the outer tube 2
And magnets 6b and 7b provided on the inner tube 1 coaxially with the coils 6a and 7a, both of which are connected to the mass flow calculation circuit 50 and detected from the relative velocity displacement between the inner tube 1 and the outer tube 2. A phase signal at the position is detected and a mass flow is determined from the phase difference signal.

The mass flow meter converter 60 is connected to the drive circuit 20.
And a resonance frequency detection circuit 30, an instrument difference correction circuit 40, and a mass flow rate calculation circuit 50.

The drive circuit 20 drives the vibrator 5 to vibrate the double vibrating tube 10 at a resonance frequency of a constant amplitude as described above. For example, a resonance drive system in which a signal from the sensor 6 is detected and amplified to form a closed lube for driving the vibrator 5 is formed. The resonance frequency varies greatly depending on the density, temperature, and installation state of the fluid to be measured. This is a large factor that determines the instrumental difference correction according to the present invention, and is detected by the resonance frequency detection circuit 30.

The instrument difference correction circuit 40 is a main part having essential features of the mass flow meter converter 60 according to the present invention. Assuming that one measuring tube is supported at both ends and driven at a constant amplitude, the driving frequency varies depending on the influence of thermal stress due to the temperature change of the fluid to be measured, the pressure and density, and the elastic modulus of the measuring tube material. However, also in the case of the double vibrating tube 10, the resonance frequency of the inner tube 1 is changed by the change of the temperature, pressure and density of the fluid to be measured, and furthermore, the change of the elastic modulus. Furthermore, in the case of the double vibrating tube 10, a temperature difference between the inner tube 1 and the outer tube 2 and a thermal stress difference caused by the temperature difference, and a characteristic of the inner tube 1 and the outer tube 2 due to a difference in each material and shape. When the frequency changes and the motor is driven at a constant amplitude, the amplitude ratio between the inner tube 1 and the outer tube 2 changes.

As described above, in the case of the double vibrating tube 10, a complicated vibration phenomenon appears as compared with the case of the single straight tube. In the resonance vibration system, the vibration mode of the double vibrating tube 10 is a complex vibration determined by the above-described physical properties and state quantities of the fluid to be measured and the material and shape of the double vibrating tube 10 and causes a change in instrumental difference. However, in the present invention, the instrumental difference change factors are determined by the temperature of the inner tube 1 and the inner tube 1.
Focusing on the temperature difference between the inner tube 1 and the outer tube 2 and the resonance frequency of the double vibrating tube 10, the instrumental difference generated based on the complicated vibration calculation is corrected by the first instrumental error correction amount due to the temperature change of the inner tube 1. , A second instrument difference correction amount based on a temperature difference between the inner tube 1 and the outer tube 2, and a third instrument difference correction amount based on a resonance frequency difference, and the content of the instrument error change is simplified,
The instrumental error correction amount is added to correct the instrumental error.

That is, the first instrumental error correction amount due to the temperature change of the inner tube 1 is separated from the total instrumental error on the assumption that the instrumental error is caused only by the thermal expansion of the inner tube 1 itself.
A reference temperature of the reference fluid (for example, 0 ° C.) is determined, and an instrumental error proportional to a temperature difference between the temperature of the fluid to be measured (actually measured temperature) and the reference temperature is determined. ct, the measured temperature Tx, the reference temperature Ta, a proportionality constant predetermined and K _1, which the first instrumental error correction amount Ct, and the _{Ct = K 1 (Tx-Ta} ) ... (1) It is.

The second instrumental difference correction amount Cdt based on the temperature difference Δt between the inner tube 1 and the outer tube 2 is obtained by calculating the thermal stress generated by the temperature difference between the inner tube 1 and the outer tube 2 by the load in each axial direction. The second instrumental error Cdt is a relational expression using the temperature difference Δt as a variable, and a relational expression using the temperature difference Δt as a variable. Coefficients Ka, Kb, applied to
It is determined based on Kc. That is, the second instrumental error correction amount Cdt is expressed as follows: Cdt = Ka △ t ² + Kb △ t + Kc (2)

The third instrument difference correction amount based on the resonance frequency difference Δf of the double vibrating tube 10 is such that when fluids having different densities flow through the inner tube 1, the natural frequency of the inner tube 1 is different and the natural frequency is constant. The resonance frequency, that is, the coupling frequency formed with the outer tube 2 changes, and the instrumental error caused by the change is corrected. That is, the instrumental difference caused by the density difference of the fluid to be measured flowing in the inner tube 1 is based on the amplitude ratio between the inner tube 1 and the outer tube 2 due to the density difference of the fluid to be measured. However, the instrumental difference due to the density difference of the fluid to be measured is determined by a complicated vibration calculation, and it is difficult to incorporate a circuit capable of executing this in the converter.
For this reason, in the present invention, the resulting instrumental difference is related to the resonance frequency difference Δf. Spring constant β of tube 1 and reference temperature Tw
Is proportional to the frequency difference between the calibrated and standardized frequency ft of the fluid based on the temperature difference between the measured temperature Tx and the measured fluid temperature Tx. It is determined that the error has occurred. That is, the third instrument difference correction amount Cf is:

[0020]

(Equation 1)

## EQU1 ##

Accordingly, the total instrument error ΔE is obtained by the first instrument error correction amount Ct based on the temperature of the inner tube 1 and the second instrument error correction amount Cdt based on the temperature difference Δt between the inner tube 1 and the outer tube 2. , And the instrumental error due to the density difference Δρ of the fluid to be measured is added to the third instrumental error correction amount Cf due to the resonance frequency difference Δf, and the total instrumental error output from the instrumental error correction circuit 40 is obtained. ΔE is: ΔE = Ct + Cdt + Cf (5)

The mass flow rate calculation circuit 50 obtains a phase difference signal ΔT proportional to the Coriolis force output from the sensors 6 and 7, and obtains a mass flow rate Qa proportional to the phase difference signal ΔT. Qa is obtained by correcting the instrumental error ΔE according to the equation (5). That is, assuming that the proportionality constant of the phase difference signal ΔT for obtaining the mass flow rate Qa is Ka, Qa = Ka (1 + ΔE) △ T = Ka (1 + Ct + Cdt + Cf) △ T (6) The mass flow rate Qa corrected for the difference ΔE is output.

[0024]

According to the first aspect of the present invention, the natural frequency of the outer tube 2 and the natural frequency of the inner tube 1 in the coaxial double straight tube type Coriolis flowmeter are changed by the temperature and density change of the fluid to be measured. Is changed and the instrumental error is changed by a first instrumental error correction amount C based on a simple thermal expansion of the inner tube.
t, the second instrumental difference correction amount Cdt due to the temperature difference between the inner tube 1 and the outer tube 2, and the frequency difference Δf of the calibrated and standardized fluid frequency with respect to the resonance frequency of the fluid to be measured. The total instrumental error is corrected by adding the third instrumental error correction amount Cf, and a simple, inexpensive, and high-precision mass flow rate can be obtained without performing correction using a complicated arithmetic expression. .

[Brief description of the drawings]

FIG. 1 is a diagram for explaining a mass flowmeter converter according to the present invention.

[Explanation of symbols]

DESCRIPTION OF SYMBOLS 1 ... Inner tube, 2 ... Outer tube, 3, 4 ... Annular flange, 5 ... Exciter, 6, 7 ... Sensor, 8 ... Balance weight, 9a, 9b ... Temperature sensor, 10 ... Coaxial double vibrating tube (2 Heavy vibration tube), 20: drive circuit, 30: resonance frequency detection circuit, 40: instrumental difference correction circuit, 50: mass flow calculation circuit, 51: output terminal, 60: mass flow meter converter.

Claims (1)

[Claims] 1. A coaxial double straight pipe comprising an inner tube through which a fluid to be measured flows and an outer tube having both ends fixed to the outside of the inner tube, wherein the outer tube has a natural frequency of the outer tube. A double vibrating tube to which a balance weight having a weight equal to the natural frequency of the inner tube is attached; driving means for driving the double vibrating tube at a resonance frequency of a constant amplitude; A pair of sensors for detecting a phase displacement proportional to a Coriolis force acting on the heavy vibrating tube, and a mass flowmeter converter of a Coriolis flowmeter for obtaining a mass flow rate based on an output of the sensor, wherein the inner tube and the outer tube Has temperature detecting means for detecting the temperatures of the inner tube and the outer tube, respectively, and corrects an instrumental difference based on a temperature change of the inner tube. Temperature correction means, temperature difference correction means for correcting an instrumental difference based on a temperature difference between the inner tube and the outer tube, and a resonance frequency of the double vibrating tube when the fluid to be measured flows is calibrated and standardized. Resonance frequency correction means for correcting an instrumental difference due to a frequency difference from a resonance frequency of the double vibrating tube when flowing the fluid, the temperature correction means, the temperature difference correction means, the resonance A mass flow meter converter, comprising: instrumental error correction means for adding the instrumental error correction amounts of the frequency correcting means and correcting the instrumental error based on the added instrumental error correction amount.