Determining the resonance parameters for mechanical oscillators

• US 8,676,543 B2
• Filed: 06/02/2010
• Issued: 03/18/2014
• Est. Priority Date: 06/23/2009
• Status: Expired due to Fees

• Current Assignee: ExxonMobil Research & Engineering Company (Exxon Mobil Corporation)
• Original Assignee: ExxonMobil Research & Engineering Company (Exxon Mobil Corporation)
• Inventors: Wolf, H. Alan, Cheng, Chung-Min, Akehurst, George, Yablon, Dalia G., Schilowitz, Alan M., Alvarez, Manuel S.
• Primary Examiner(s): Teixeira Moffat, Jonathan C.
• Assistant Examiner(s): PARK, HYUN D
• Application Number:
  US12/792,500
• Publication Number:
  US 20100324852A1
• Time in Patent Office: 1,385 Days
• Field of Search: 702/190
• US Class Current: 702/190
• CPC Class Codes: G01D 1/00 Measuring arrangements giving results other than momentary value of variable, of general application G01D3/00 takes precedence; in tariff metering apparatus G01D4/00; transducers not specially adapted for a specific variable G01D5/00
• CPC Class Codes: G01D 15/00 Component parts of recorders for measuring arrangements not specially adapted for a specific variable
• CPC Class Codes: G01H 13/00 Measuring resonant frequency
• CPC Class Codes: G01N 17/04 Corrosion probes
• CPC Class Codes: G01N 29/46 by spectral analysis, e.g. Fourier analysis or wavelet analysis spectral signal processing per se G06F17/14

Abstract

Mechanical oscillators employ the use of resonance parameters, frequency and the quality factor Q, for the measurement of corrosion or deposition. The ability of a mechanical oscillator to measure small amounts of metal loss or deposition is not only dependent upon the mechanical design but is limited by the precision in determining the resonance frequency and Q. Methods for measuring these resonance parameters with a high precision in the presence of noise are provided. The increased degree of precision improves the utility of these devices as sensitive probes for corrosion and deposition (fouling) measurement. The increased degree of precision is enabled in part by employing curve fitting consistent with modeling the mechanical oscillator as a simple harmonic oscillator. This curve fitting procedure, combined with averaging and utilizing signal processing parameters to mitigate noise effects, adds precision in measuring resonance parameters.

Claims

1. A method for determining resonance parameters, resonance frequency f and quality factor Q, for a mechanical oscillator in a service fluid environment in the presence of noise produced by the service fluid comprising:

a) estimating the resonance parameters for a mechanical oscillator in a service fluid environment based on an excitation of the mechanical oscillator by a flow of the service fluid, the estimate of the resonance parameters being determined from the steps of determining a fast Fourier transform of amplitude as a function of frequency, wherein said estimate of the resonance parameters is determined from averaging the fast Fourier transform run multiple times;

b) exciting the mechanical oscillator in the service fluid environment using a signal generator at one or more excitation frequencies selected based on the estimated resonance parameters, the service fluid environment producing noise that causes an excitation;

c) determining a response to said exciting of the mechanical oscillator at the one or more excitation frequencies; and

d) determining f and Q, using a computer, from the response with multiple measurements and curve fitting and averaging.

2. The method of claim 1 wherein the determination of step c) is accomplished with a digital computer.

3. The method of claim 1 wherein f and Q are determined from the steps of terminating the excitation at the one or more excitation frequencies produced by said signal generator so that the amplitude of said oscillator decreases from which amplitude as a function of excitation frequency is determined repeating this step so as to obtain an average value off and Q.

4. The method of claim 3 wherein f and Q are determine from a frequency sweep signal.

5. The method of claim 1 wherein f and Q are determined from the steps of terminating the excitation at the one or more excitation frequencies produced by said signal generator so that the amplitude of said oscillator decreases, obtaining f from the crossing of the amplitude of zero and Q from the decline of the amplitude, repeating the above steps to obtain an average value for f and Q.

6. The method of claim 5 wherein f and Q are determined from a ringdown signal.

7. The method of claim 1 where the one or more signal generator excitation frequencies are algorithmically selected based on the estimated resonance parameters to minimize the required number of frequencies.

8. The method of claim 1 wherein the signal generator excitation confirms or refutes peaks in the fast Fourier transform as the oscillator resonance.

9. The method of claim 1 applied recursively to determine f and Q as a function of time.