Method for operating a Coriolis mass flowmeter

Patent metadata

Field	Value
Publication number	US-10816378-B2
Application number	US-201414566825-A
Country	US
Kind code	B2
Filing date	Dec 11, 2014
Priority date	Dec 13, 2013
Publication date	Oct 27, 2020
Grant date	Oct 27, 2020

Abstract

A method for operating a Coriolis mass flowmeter in which the interferences when calculating the medium parameters is considered by the eigenfrequency (f 01 ) of the oscillation of the measuring tube being determined in the first and second natural modes during operation of the Coriolis mass flowmeter, and at least one medium parameter ({dot over (m)}) is calculated with the aid of the oscillation measuring variable (Δt) by means of a calculation rule representing a mathematic relation between the oscillation measuring variable (Δt), the medium parameter ({dot over (m)}) and the eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first natural mode and the second natural mode, and the medium parameter ({dot over (m)}) being determined taking into consideration the current determined eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tub in the first natural mode and the second natural mode as well as the oscillation measuring variable (Δt).

First claim

What is claimed is:

1. Method for operating a Coriolis mass flowmeter having at least one electric setting device, at least one electric drive forming an oscillation generator, at least one measuring tube interacting with a medium and having at least one oscillation sensor, comprising the steps of:
using the electric setting device to provide an electric excitation signal for exciting the electric drive,
using the electric drive to excite the measuring tube into oscillation in at least one first natural mode,
detecting the excited oscillation of the measuring tube with the oscillation sensor as an oscillation measuring variable (x, {dot over (x)}, Δt)
calculating at least the mass flow of a medium through the measuring tube as one medium parameter ({dot over (m)}) with the aid of the oscillation measuring variable (Δt) by means of a calculation rule, and
reducing the influence of interferences on measured values or on medium parameters to be determined by:
determining a first eigenfrequency (f 01 ) of the oscillation of the measuring tube in the first natural mode during operation of the Coriolis mass flowmeter,
determining a second eigenfrequency (f 02 ) of the oscillation of the measuring tube in at least one second natural mode during operation of the Coriolis mass flowmeter,
wherein a calculation rule represents a mathematic relation between the oscillation measuring variable (Δt), the medium parameter ({dot over (m)}) and the first and second eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first and second natural modes,
wherein the medium parameter ({dot over (m)}) is determined taking into consideration current determined eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first and second natural modes as well as the oscillation measuring variable (Δt),
wherein the calculation rule has a term for the eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first natural mode and the second natural mode as an integral correction function f IK ,
wherein a term for the integral correction function f IK depending on the eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first natural mode and the second natural mode has the following form

1

1
-

ω
01
2

ω
02
2

wherein ω 01 is a circular eigenfrequency of the oscillation in the first natural mode and ω 02 is a circular eigenfrequency of the oscillation in the second natural mode,
wherein the eigenfrequencies are continually measured during operation of the Coriolis mass flowmeter and calculation of the mass flow as the medium parameter is continuously corrected using the integral correction function with the continuously measured eigenfrequencies,
wherein corrected measured values and characteristic variables of the flow through the measurement tube, in which the influence of interferences has been reduced, are output.

2. Method according to claim 1 , wherein at least one of the first eigenfrequency (f 01 ) of the oscillation of the measuring tube is determined in the first natural mode and the second eigenfrequency (f 02 ) of the oscillation of the measuring tube is determined in the second natural mode by specifically exciting the measuring tube in a phase-locked loop.

3. Method according to claim 2 , wherein a phase shift between a driving force of the electric drive and a velocity response ({dot over (x)}) of the measuring tube detected via the oscillation sensor is regulated using a variation of the frequency of the excitation signal at a predetermined value.

4. Method according to claim 1 , wherein the oscillation of the measuring tube is excited in the second natural mode by at least one of actively exciting the oscillation of the measuring tube in the first natural mode based on structural asymmetries and excitation tracking the eigenfrequency of the second natural mode via a phase-locked loop.

5. Method according to claim 1 , wherein the calculation rule has a term for the eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first natural mode and the second natural mode as an integral correction function f IK .

6. Method according to claim 5 , wherein the calculation rule has no further dependencies on the eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube in the first natural mode and the second natural mode.

7. Method according to claim 5 , wherein a term for the integral correction function f IK depending on the eigenfrequencies (f 01 , f 02 ) of the oscillations of the measuring tube ( 5 ) in the first natural mode and the second natural mode has the following form

1

1
-

ω

0
⁢
1

2

ω

0
⁢
2

2

wherein ω 01 is the circular eigenfrequency of the oscillation in the first natural mode and ω 02 is the circular eigenfrequency of the oscillation in the second natural mode.

8. Method according to claim 5 , wherein the integral correction function f IK is additionally dependent on spring stiffness c 2 of the measuring tube in oscillation in the second natural mode.

9. Method according to claim 6 , wherein an integral correction function f IK has the following form:

f
IK

(

T
,

Δ
⁢

⁢
T

,
P
,
σ
,

Δ
⁢

⁢
σ

,
…

⁢

)

=

K
·

1

1
-

ω
01
2

ω
02
2

·

1

Assignees

• Krohne Messtechnik Gmbh

Inventors

• Kolahi Kourosh
• Storm Ralf

Classifications

• G01F1/8436 Primary

  signal processing · CPC title