Predicting and reducing noise in a vibratory meter
US-2020264024-A1 · Aug 20, 2020 · US
US12313435B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-12313435-B2 |
| Application number | US-202117995176-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 8, 2021 |
| Priority date | Mar 31, 2020 |
| Publication date | May 27, 2025 |
| Grant date | May 27, 2025 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A method for operating a Coriolis measurement device comprises the following steps: recording the measured voltages of sensors for sensing measuring tube vibrations and creating an asymmetric sequence of values by way of the amplitudes of the measured voltages for the purpose of diagnosing the Coriolis measurement device, recording at least one stabilization variable and creating a stabilized asymmetric sequence of values based on the stabilization variable, wherein the stabilization variable is one of the following variables or a first or further temporal derivative thereof: a resonant frequency of the measuring tube containing medium or a variable derived therefrom, time or phase difference between measurement signals from the first sensor and the second sensor or a variable derived therefrom, temperature of the measuring tube wall, temperature difference between two measurement points of the measuring tube wall.
Opening claim text (preview).
The invention claimed is: 1. A method for operating a Coriolis measurement device for measuring a density or a mass flow of a medium flowing through a pipeline, wherein the Coriolis measurement device comprises: at least one measuring tube for guiding the medium, each having an inlet and an outlet and a measuring tube wall enclosing a measuring tube lumen; at least one exciter for generating measuring tube vibrations, and a first sensor on the inlet side and a second sensor on the outlet side for sensing measuring tube vibrations, wherein the exciter and the sensors each have a coil device with at least one coil and a magnetic device with at least one magnet; wherein the coil device and the magnetic device of each sensor are moved relative to one another by measuring tube vibrations, during which an electrical measured voltage is induced in the coil; and an electronic circuit for operating the exciter, for sensing and evaluating the electrical measured voltages and for outputting diagnostic information, and for outputting measured values of density or mass flow; wherein the method has the following steps: diagnosing the Coriolis measurement device by: recording the measured voltages from the sensors and creating a first sequence of values using the amplitudes of the measured voltages, wherein the first sequence of values represents differences between amplitudes of signals of at least two different sensors; recording a measurement signal of at least one stabilization variable; creating a second sequence of values based on the first sequence of values as a function of the stabilization variable; wherein the stabilization variable is based on one of the following variables or a first or second temporal derivative thereof: a resonant frequency of the measuring tube containing medium or a variable derived therefrom; time or phase difference between measurement signals from the first sensor and the second sensor or a variable derived therefrom; temperature of the measuring tube wall; or temperature difference between two measurement points of the measuring tube wall; and outputting error information if a value in the second sequence of values is greater than a predetermined value. 2. The method according to claim 1 , wherein a scatter value of the measured values of the stabilization variable is determined, wherein the first sequence of values is stabilized using the scatter value; wherein the scatter value is based on a random number of values. 3. The method according to claim 2 , wherein, when a first limit value is exceeded by the scatter value a last valid measured value of the first sequence of values is used as the current value of the first sequence of values; or the first sequence of values is set to a predetermined value. 4. The method according to claim 3 , wherein the first limit value is derived from scatter values or a mean value of measured values of the stabilization variable; or wherein the first limit value is a configurable parameter. 5. The method according to claim 4 , wherein the mean value is a moving mean value with a first time window, and wherein the scatter value is a moving scatter value with a second time window; wherein the moving mean value changes with time; wherein the moving scatter value changes with time. 6. The method according to claim 5 , wherein the first time window has a duration of at least 0.2 seconds and at most 90 seconds. 7. The method according to claim 6 , wherein the second time window has a duration of at least 2 seconds and at most 150 seconds. 8. The method according to claim 3 , wherein, if the time or phase difference or a variable derived therefrom falls below a second limit value and the asymmetry exceeds a third limit value, a last valid measured value of the asymmetric sequence of values is used as the current value of the asymmetric sequence of values, or the asymmetric sequence of values is set to a predetermined value. 9. The method according to claim 2 , wherein the scatter value is determined by one of the following procedures: summing differences between adjacent measured values, summing differences of the measured values from a mean value of measured values of the stabilization variable. 10. The method according to claim 9 , wherein a distance measure A has the following relationship: A=|p1−p2|{circumflex over ( )}n, where n>0, and p1 is a measured value and p2 is a measured value or a mean of the measured value. 11. The method according to claim 8 , wherein a warning is output if an amount of the stabilized asymmetric sequence of values exceeds a fourth limit value. 12. The method according to claim 1 , wherein the Coriolis measurement device comprises at least one temperature sensor.
Indicating or recording devices · CPC title
using electrical means · CPC title
with multiple measuring conduits · CPC title
detectors · CPC title
exciters · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.