IP Library Granted Patent US 8,473,224
Granted Patent B2
US 8,473,224 · App. 13/420,054 · Granted Jun 25, 2013

Compensating for frequency change in flowmeters

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Quick Facts
Patent No.
US 8,473,224
App. No.
13/420,054
Granted
Jun 25, 2013
Kind
B2
Abstract

Motion is induced in a conduit that contains a fluid. The motion is induced such that the conduit oscillates in a first mode of vibration and a second mode of vibration. The first mode of vibration has a corresponding first frequency of vibration and the second mode of vibration has a corresponding second frequency of vibration. At least one of the first frequency of vibration or the second frequency of vibration is determined. A phase difference between the motion of the conduit at a first point of the conduit and the motion of the conduit at a second point of the conduit is determined. A quantity based on the phase difference and the determined frequency is determined. The quantity includes a ratio between the first frequency during a zero-flow condition and the second frequency during the zero-flow condition. A property of the fluid is determined based on the quantity.

Claims (146)

1. A flowmeter transmitter comprising:

at least one processing device; and

a storage device, the storage device storing instructions for causing the at least one processing device to:

induce motion in a conduit such that the conduit oscillates in a first mode of vibration and a second mode of vibration, the first mode of vibration having a corresponding first frequency of vibration and the second mode of vibration having a corresponding second frequency of vibration, wherein the conduit contains fluid;

determine at least one of the first frequency of vibration or the second frequency of vibration;

calculate a property of the fluid based on the first frequency of vibration and the second frequency of vibration, wherein the first frequency is determined based on the second frequency by calculating:

ω

1

2

=

ω

2

2

(

E

2

+

(

E

2

-

D

2

)

t

2

)

2

(

E

2

+

(

D

4

-

E

4

)

t

2

ω

2

2

)

(

D

2

+

(

D

4

-

E

4

)

(

1

+

t

2

)

ω

2

2

)

where ω 1 is the first frequency, ω 2 is the second frequency,

t

2

=

k

tan

2

(

φ

2

)

where φ is the phase difference k, D 2 , D 4 , E 2 , and E 4 are calibration constants related to physical properties of the conduit,

determine an augmented temperature, wherein the augmented temperature is calculated using:

T f *=T f −k td1 ( T f −T m ),

where T f , is the temperature of the fluid contained in the flowtube, T 0 is a reference temperature and the ambient temperature or flowtube temperature is T m , and k td2 is an empirically determined constant that is specific to the flowtube;

update calibration constants E 2 , and E 4 using augmented temperature, wherein E is calculated using:

E 2 =E 20 (1 +E ( T f *−T 0 ))

E 4 =E 40 (1 +F ( T f *−T 0 )),

determine a density compensated for effects of mass flow rate on frequencies by the calculation:

ρ

0

=

1

2

(

D

4

+

E

4

+

4

D

2

E

2

ω

1

2

ω

2

2

+

(

D

4

-

E

4

)

2

)

,

where D 2 , D 4 , E 2 , and E 4 are calibration constants, and ω 1 is the Coriolis mode frequency, and ω 2 is the driven mode frequency.

2. The transmitter of claim 1 , wherein the property includes a density of the fluid contained in the conduit.

3. The transmitter of claim 2 , wherein the storage device further stores instructions for causing the at least one processing device to:

determine density calibration constants based on physical properties of the conduit;

determine a reference temperature;

determine a first temperature that influences the first mode of vibration;

determine a second temperature that influences the second mode of vibration;

compensate the density calibration constants based on the first temperature, the second temperature, and the reference temperature;

wherein determining the property includes determining the density based the compensated density calibration constants.

4. The transmitter of claim 1 , wherein:

the first mode is a Coriolis mode, and

the second mode is a driven mode.

Assignments (2)
CHANGE OF NAME Recorded Jul 31, 2017
From: INVENSYS SYSTEMS, INC.
To: SCHNEIDER ELECTRIC SYSTEMS USA, INC.
Reel/Frame 043379/0925 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 7, 2012
From: TOMBS, MICAEL S., MR.
To: INVENSYS SYSTEMS, INC.
Reel/Frame 028333/0953 →