Coriolis densimeter having substantially increased noise immunity

• US 4,996,871 A
• Filed: 03/09/1990
• Issued: 03/05/1991
• Est. Priority Date: 06/02/1989
• Status: Expired due to Term

• Current Assignee: Micro Motion Incorporated (Emerson Electric Company)
• Original Assignee: Micro Motion Incorporated (Emerson Electric Company)
• Inventors: Romano, Paul
• Primary Examiner(s): Goldstein, Herbert
• Application Number:
  US07/490,099
• Time in Patent Office: 361 Days
• Field of Search: 73/861.38, 73/32 A, 73/861.37
• US Class Current: 73/32.00A
• CPC Class Codes: G01F 1/8431 electronic circuits
• CPC Class Codes: G01F 1/8436 signal processing
• CPC Class Codes: G01F 1/8477 with multiple measuring conduits
• CPC Class Codes: G01F 15/024 involving digital counting

Abstract

Apparatus and accompanying methods for use therein for a Coriolis mass flow rate meter which is substantially immune to noise, and more particularly, to such a meter that is substantially unaffected by noise that occurs at substantially any frequency different from a fundamental frequency at which the flow tube(s) in the meter vibrate. Specifically, the meter relies on measuring mass flow rate by determining the phase difference that occurs between real and imaginary components of the discrete fourier transform (DFT) of both the left and right velocity sensor waveforms evaluated at the fundamental frequency at which the flow tubes vibrate. The fundamental frequency is located, during an initialization operation, by providing a power spectrum, determined through use of the DFT of one of the sensor signals and then selecting that frequency at which the magnitude of the power spectrum reaches a maximum value. In addition, the frequency at which both velocity sensor signals is sampled is readjusted in response to any change in the phase of one of the velocity sensor signals, as transformed using the DFT, in order to assure that the sampling frequency always remains substantially equal to a pre-defined integer multiple of the fundamental frequency. Furthermore, the meter, through use of the numerical value of any such phase change, also provides a density indication which is also substantially immune to such noise.

Claims

1. Apparatus for measuring density of a fluid passing through a Coriolis meter, wherein said meter utilizes a flow conduit having a sensor associated therewith for providing a sensor signal indicative of movement of said flow conduit, said apparatus comprising:

means for driving the flow conduit in a sinusoidal vibratory pattern and at a resonant frequency thereof while said fluid flows therethrough;

means for sampling said sensor signal at a sampling frequency to yield a sampled sensor signal;

means for undertaking initialization comprising;

means for setting the sampling frequency to an initial pre-defined value;

means for producing, in response the sensor signal sampled at said initial value, a power spectrum for a pre-selected sequence of frequencies contained within said sampled sensor signal and selecting a particular one of said frequencies in said sequence at which said power spectrum reaches a maximum value as being a fundamental frequency at which said conduit is resonantly vibrating;

means for setting the sampling frequency to a second sampling frequency value, equal to a pre-defined integer multiple of said one frequency, for initial use during density measurement; and

means for obtaining a base-line density value for said fluid;

means for undertaking a density measurement comprising;

means for transforming said sensor signal using a pre-defined transformation from a time domain to a frequency domain so as to yield a frequency value, wherein said frequency value is produced by evaluating said transformation at the fundamental frequency for said sampled sensor signal;

means for ascertaining in response to said frequency value a phase value associated therewith;

means for providing a density value in response to the base-line density value and the ascertained phase value; and

means for varying the sampling frequency, in response to the ascertained phase value, in order to compensate for a change in the fundamental frequency caused by a substantially simultaneously occurring variation in density of the fluid flowing through the meter, whereby the sampling frequency substantially remains at the pre-defined integer multiple of the fundamental frequency.

2. The apparatus in claim 1 wherein the transformation is a Fourier, Discrete Fourier, Fast Fourier, Hanning or Hilbert transform.

3. The apparatus in claim 2 wherein said density value providing means comprises means for generating the density value as being substantially equal to the sum of the base-line density value and a product of the ascertained phase value multiplied by a pre-defined constant.

4. The apparatus in claim 3 wherein said producing and selecting means comprises:

means for transforming said sampled sensor signal using the pre-defined transformation into the frequency value;

first means for determining a magnitude of the frequency value produced by the transformation at each successive frequency in a series of frequencies occurring at a first resolution within a pre-defined range and situated within said sequence;

means for locating, in response to said first determining means, a first frequency within said series and occurring at said first resolution at which the magnitude of the frequency value reaches a maximum value;

second means for determining the magnitude of the frequency value for each successive frequency in a second series of frequencies occurring at a second resolution and situated within a band of frequencies centered at said first located frequency and extending to corresponding limit frequencies situated on respective sides thereof as defined by said first resolution, wherein said second resolution is higher than said first resolution; and

means for locating, in response to said second determining means, a second frequency occurring at said second resolution at which the magnitude of the frequency value reaches a maximum magnitude and selecting said second located frequency as said fundamental frequency.

5. The apparatus in claim 4 wherein said first magnitude determining means comprises:

means for successively varying a frequency index throughout the pre-defined range by an incremental value specified by said first resolution; and

means for determining the magnitude of the frequency value at each successive value of the frequency index occurring at said first resolution within said pre-defined range while maintaining the sampling frequency at a constant value.

6. The apparatus in claim 4 wherein said second magnitude determining means comprises:

means for successively varying the sampling frequency by an incremental value specified by said second resolution from the first one of the limit frequencies in said second series to the second one of the limit frequencies in said second series; and

means for determining the magnitude of the frequency value at each successive frequency in said second series.

7. A method for measuring density of a fluid passing through a Coriolis meter, wherein said meter utilizes a flow conduit having a sensor associated therewith for providing a sensor signal indicative of movement of said flow conduit, said method comprising the steps of:

driving the flow conduit in a sinusoidal vibratory pattern and at a resonant frequency thereof while said fluid flows therethrough;

sampling said sensor signal at a sampling frequency to yield a sampled sensor signal;

during initialization;

setting the sampling frequency to an initial pre-defined value;

producing, in response the sensor signal sampled at said initial value, a power spectrum for a pre-selected sequence of frequencies contained within said sampled sensor signal and selecting a particular one of said frequencies in said sequence at which said power spectrum reaches a maximum value as being a fundamental frequency at which said conduit is resonantly vibrating;

multiple of said one frequency, for initial use during density measurement; and

obtaining a base-line density value for said fluid;

during density measurement;

transforming said sensor signal using a pre-defined transformation from a time domain to a frequency domain so as to yield a frequency value, wherein said frequency value is produced by evaluating said transformation at the fundamental frequency for said sampled sensor signal;

ascertaining in response to said frequency value a phase value associated therewith;

providing a density value in response to the base-line density value and the ascertained phase value;

varying the sampling frequency, in response to the ascertained phase value, in order to compensate for a change in the fundamental frequency caused by a substantially simultaneously occurring variation in density of the fluid flowing through the meter, and

iteratively repeating the sensor signal transforming, phase value ascertaining, density value providing, and sampling frequency varying steps so as to provide a succession of density measurement values, whereby the sampling frequency that is used to produce substantially all of these density measurement values substantially remains at the pre-defined integer multiple of the fundamental frequency.

8. The method in claim 7 wherein the transformation is a Fourier, Discrete Fourier, Fast Fourier, Hanning or Hilbert transform.

9. The method in claim 8 wherein said density value providing step comprises the step of generating the density value as being substantially equal to the sum of the base-line density value and a product of the ascertained phase value multiplied by a pre-defined constant.

10. The method in claim 9 wherein said producing and selecting step comprises the steps of:

transforming said sampled sensor signal using the pre-defined transformation into the frequency value;

first determining a magnitude of the frequency value produced by the transformation at each successive frequency in a series of frequencies occurring at a first resolution within a pre-defined range and situated within said sequence;

locating, in response to said first determining step, a first frequency within said series and occurring at said first resolution at which the magnitude of the frequency value reaches a maximum value;

second determining the magnitude of the frequency value for each successive frequency in a second series of frequencies occurring at a second resolution and situated within a band of frequencies centered at said first located frequency and extending to corresponding limit frequencies situated on respective sides thereof as defined by said first resolution, wherein said second resolution is higher than said first resolution; and

locating, in response to said second determining step, a second frequency occurring at said second resolution at which the magnitude of the frequency value reaches a maximum magnitude and selecting said second located frequency as said fundamental frequency.

11. The method in claim 10 wherein said first magnitude determining step comprises the steps of:

successively varying a frequency index throughout the pre-defined range by an incremental value specified by said first resolution; and

determining the magnitude of the frequency value at each successive value of the frequency index occurring at said first resolution within said pre-defined range while maintaining the sampling frequency at a constant value.

12. The method in claim 10 wherein said second magnitude determining step comprises the steps of:

successively varying the sampling frequency by an incremental value specified by said second resolution from the first one of the limit frequencies in said second series to the second one of the limit frequencies in said second series; and

determining the magnitude of the frequency value at each successive frequency in said second series.