Coriolis flow meter and method of measuring mass flow rate
US-2015377673-A1 · Dec 31, 2015 · US
US10788348B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10788348-B2 |
| Application number | US-201515745040-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 27, 2015 |
| Priority date | Jul 27, 2015 |
| Publication date | Sep 29, 2020 |
| Grant date | Sep 29, 2020 |
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A method and apparatus for a flowmeter ( 5 ) is provided. The method comprises the steps of placing a material in a flow tube ( 130, 130 ′) while exciting a vibration mode of the flow tube ( 130, 130 ′). Exciting the vibration mode of the flow tube ( 130, 130 ′) comprises the steps of periodically driving a first driver ( 180 L) with a first signal and periodically driving a second driver ( 180 R) with a second signal, wherein the second driver ( 180 R) is driven essentially in phase with the first driver ( 180 L), but wherein the first driver's ( 180 L) drive amplitude modulated signal reaches a maximum amplitude when the second driver's ( 180 R) drive modulated signal reaches a minimal amplitude, and the first driver's ( 180 L) drive amplitude modulated signal reaches a minimum amplitude when the second driver's ( 180 R) drive amplitude modulated signal reaches a maximum amplitude. The method also comprises the steps of measuring the relative phase between a first pickoff ( 170 L) and a second pickoff ( 170 R) and determining a relative phase of a right eigenvector for the flow tube ( 130, 130 ′).
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We claim: 1. A method, comprising: placing a material in a flow tube while exciting a vibration mode of the flow tube, wherein exciting the vibration mode of the flow tube comprises the steps of: periodically driving a first driver with a first signal; periodically driving a second driver with a second signal, wherein the second driver is simultaneously driven essentially in phase with the first driver, wherein the first driver's drive amplitude modulated signal reaches a maximum amplitude when the second driver's drive amplitude modulated signal reaches a minimal amplitude, and the first driver's drive amplitude modulated signal reaches a minimum amplitude when the second driver's drive amplitude modulated signal reaches a maximum amplitude; measuring the relative phase between a first pickoff and a second pickoff; and determining a relative phase of a right eigenvector for the flow tube; measuring a frequency shift that occurs between when the first driver's drive amplitude modulated signal reaches a maximum amplitude and when the second driver's drive amplitude modulated signal reaches a maximum amplitude; offsetting the first signal with a phase shift; adjusting the first signal offset until the frequency shift is substantially undetectable; and determining the relative phase of the left eigenvector coefficients from the first signal offset necessary for rendering the frequency shift substantially undetectable. 2. The method of claim 1 , wherein the step of determining an actual flow of the material through the flow tube further comprises: determining an uncorrected flow of the material through the flow tube using the relative phase of the right eigenvector; and determining a zero offset for the flow of the material through the flow tube using the relative phase of the left eigenvector coefficients. 3. The method of claim 2 , further comprising: determining a material flow through the flow tube using the relative phase of the right eigenvector corrected by the zero offset. 4. The method of claim 1 , further comprising: determining the relative phase of a right eigenvector; and determining a zero offset for the flow of the material through the flow tube by weighted averaging the relative phase of the right eigenvector with the relative phase of the left eigenvector. 5. The method of claim 1 , further comprising: estimating a frequency shift caused by the driver cycling; and relating the frequency shift to flow. 6. The method of claim 5 , wherein the frequency is estimated with a frequency modulated second-order infinite impulse response adaptive notch filter. 7. The method of claim 6 , further comprising: inputting a notch filter sharpness (a) parameter into the meter electronics; inputting a notch filter modulation frequency (fm) parameter into the meter electronics; determining a notch filter adaptation rate (k) parameter based on the notch filter modulation frequency (fm) parameter and the sharpness (a) parameter; and inputting a pickoff signal into the adaptive notch filter, wherein the adaptive notch filter has a center frequency adapted to minimize filter output. 8. The method of claim 6 , wherein an output of the notch filter is demodulated at the cycling frequency. 9. The method of claim 1 , further comprising: co-locating the first driver with the first pickoff sensor; and co-locating the second driver with the second pickoff sensor. 10. The method of claim 1 , wherein the step of periodically driving the first driver with the first signal comprises sinusoidally driving the first driver, and wherein the step of periodically driving the second driver with the second signal comprises sinusoidally driving the second driver. 11. A method, comprising: simultaneously providing a first signal to the first driver and a second signal to the second driver, wherein the second driver is driven essentially in phase with the first driver; flowing a material through a flow tube while periodically exciting a vibration mode of the flow tube such that a first driver's drive amplitude modulated signal reaches a maximum amplitude when a second driver's drive amplitude modulated signal reaches a minimal amplitude, and the first driver's drive amplitude modulated signal reaches a minimum amplitude when the second driver's drive amplitude modulated signal reaches a maximum amplitude; measuring the relative motion of the vibrating flow tube; measuring a relative phase of a right eigenvector while exciting the vibration mode of the flow tube; determining the material flow through the flow tube using the relative phase of a right eigenvector corrected by a zero offset; determining a new zero offset without stopping the material flow through the flow tube using a relative phase of a left eigenvector for the flow tube; and determining the material flow through the flow tube using the relative phase of a right eigenvector corrected by the new zero offset. 12. The method of claim 11 , further comprising: co-locating the first driver with the first pickoff sensor; and co-locating the second driver with the second pickoff sensor. 13. A vibratory flowmeter ( 5 ) comprising: a flowmeter assembly ( 10 ) including one or more flow tubes ( 130 , 130 ′) and first and second pickoff sensors ( 170 L, 170 R); first and second drivers ( 180 L, 180 R) configured to vibrate the one or more flow tubes ( 130 , 130 ′); and meter electronics ( 20 ) coupled to the first and second pickoff sensors ( 170 L, 170 R) and coupled to the first and second drivers ( 180 L, 180 R), with the meter electronics ( 20 ) being configured to: simultaneously provide a first signal to the first driver ( 180 L) and a second signal to the second driver ( 180 R), wherein the second driver ( 180 R) is driven essentially in phase with the first driver ( 180 L), wherein the first driver's ( 180 L) drive amplitude modulated signal reaches a maximum amplitude when the second driver's ( 180 R) drive amplitude modulated signal reaches a minimal amplitude, and the first driver's ( 180 L) drive amplitude modulated signal reaches a minimum amplitude when the second driver's ( 180 R) drive amplitude modulated signal reaches a maximum amplitude; measure the relative phase between a first pickoff ( 170 L) and a second pickoff ( 170 R) and determine a relative phase of a right eigenvector for the flow tube; and measure a frequency shift that occurs between when the first driver's ( 180 L) drive amplitude modulated signal reaches a maximum amplitude and when the second driver's ( 180 R) drive amplitude modulated signal reaches a maximum amplitude, offset the first signal with a phase shift, adjust the first signal offset until the frequency shift is substantially undetectable, and determine the phase of the left eigenvector coefficients from the first signal offset necessary for rendering the frequency shift substantially undetectable. 14. The vibratory flowmeter ( 5 ) of claim 13 , with the meter electronics ( 20 ) being further configured to determine an uncorrected flow of a material through the one or more flow tubes ( 130 , 130 ′) using the relative phase of the right eigenvector and to determine a zero offset for the flow of the material through the one or more flow tubes ( 130 , 130 ′) using the phase of left eigenvector coefficients. 15. The vibratory flowmeter ( 5 ) of claim 14 , with the meter electronics ( 20 ) being further configured to determine a material flow through the one or more flow tubes ( 130 , 130 ′) using the relative phase of the right eigenvector corrected by the zero offset. 16. Th
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