Gas concentration and flow rate sensor

• US 5,343,760 A
• Filed: 07/09/1992
• Issued: 09/06/1994
• Est. Priority Date: 07/09/1992
• Status: Expired due to Fees

• Current Assignee: General Motors Corporation (Motors Liquidation Co. GUC Trust)
• Original Assignee: General Motors Corporation (Motors Liquidation Co. GUC Trust)
• Inventors: Kenty, Joseph L., Sultan, Michel F., O'Rourke, Michael J.
• Primary Examiner(s): Chilcot, Jr., Richard E.
• Assistant Examiner(s): PATEL, HARSHAD R
• Application Number:
  US07/910,913
• Time in Patent Office: 789 Days
• Field of Search: 73/861.18, 73/861.21, 73/861.04, 73/24.01, 73/24.05
• US Class Current: 73/861.04
• CPC Class Codes: F02D 41/0045 Estimating, calculating or determining the purging rate, amount, flow or concentration
• CPC Class Codes: G01F 1/666 by detecting noise and sounds generated by the flowing fluid
• CPC Class Codes: G01F 1/74 Devices for measuring flow of a fluid or flow of a fluent solid material in suspension in another fluid
• CPC Class Codes: G01N 2291/0212 Binary gases
• CPC Class Codes: G01N 2291/02809 Concentration of a compound, e.g. measured by a surface mass change
• CPC Class Codes: G01N 2291/02836 Flow rate, liquid level
• CPC Class Codes: G01N 29/036 by measuring frequency or resonance of acoustic waves

Abstract

A gas vapor sensor indicates the relative concentrations and flow rate of a gas mixture. Acoustic noise is generated within a closed chamber by the gas mixture flowing therethrough or by ambient noise sources. The chamber has a fundamental resonant frequency which varies with the vapor concentration. Acoustic frequency components of the noise corresponding to the resonant frequency of the chamber are sharply reinforced and dominate the acoustic spectrum within the chamber. The spectrum is detected and frequency filtered by a pair of dissimilar parallel filters to produce two attenuated outputs. The difference between the attenuated outputs indicates the resonant frequency and is a measure of the vapor concentration. The strength of the acoustic spectrum together with the measured vapor concentration indicates the flow rate of the mixture.

Claims

1. A sensor for detecting concentrations of a gas mixture comprising:

a chamber bounding the gas mixture, the chamber having a fundamental resonant acoustic frequency varying with the gas concentrations of the mixture therein;

means for detecting acoustic noise in said chamber and producing therefrom a spectrum signal; and

means for measuring the fundamental resonant frequency of said chamber from said spectrum signal, said measured fundamental resonant frequency being a measure of the gas concentrations.

3. A sensor as claimed in claim 1 or 2 wherein the means for measuring the fundamental resonant frequency comprises:

first and second frequency filters, each filter having a respective input, output and response curve, each of said response curves having a slope different from the other from a predetermined lowest fundamental resonant frequency to be measured to a predetermined highest fundamental resonant frequency to be measured, both of said filters being commonly coupled to the spectrum signal at their respective inputs; and

means for measuring a normalized difference between the outputs of the filters, said normalized difference being a measure of the fundamental resonant frequency.

4. A sensor as claimed in claim 3 further comprising:

means for sensing the temperature of the gas mixture within the chamber; and

means responsive to said sensed temperature for shifting the response curve of each respective filter to compensate for deviations in the fundamental resonant frequency of the chamber which result from changes in the temperature of the gas mixture within the chamber from a calibration temperature, whereby the measured fundamental resonant frequency is a temperature insenstive measure of the gas concentrations of the mixture.

5. A sensor as claimed in claim 3 wherein the frequency filters are band-pass filters, one of the band-pass filters having a central frequency substantially corresponding to a predetermined lowest fundamental resonant frequency to be measured and the other band-pass filter having a central frequency substantially corresponding to a predetermined highest fundamental resonant frequency to be measured.

6. A sensor as claimed in claim 5 wherein each response curve slope is monotonic from the predetermined lowest fundamental resonant frequency to be measured to the predetermined highest fundamental resonant frequency to be measured.

7. A sensor as claimed in claim 6 wherein the means for measuring the normalized difference comprises:

means for measuring the difference between the respective outputs of the frequency filters;

means for measuring the sum of the respective outputs of the frequency filters; and

means for measuring the ratio of said difference to said sum, said measured ratio being a measure of said normalized difference.

8. A sensor as claimed in claim 3 wherein each response curve slope is monotonic from the predetermined lowest fundamental resonant frequency to be measured to the predetermined highest fundamental resonant frequency to be measured.

9. A sensor as claimed in claim 8 wherein the means for measuring the normalized difference comprises:

means for measuring the difference between the respective outputs of the frequency filters;

means for measuring the sum of the respective outputs of the frequency filters; and

means for measuring the ratio of said difference to said sum, said measured ratio being a measure of said normalized difference.

2. A sensor for simultaneously detecting concentrations and flow rates of a gas mixture comprising:

a chamber through which the gas mixture flows, the chamber having an inlet and an outlet and a fundamental resonant acoustic frequency varying with the gas concentrations of the mixture therein;

means for detecting acoustic noise in said chamber and producing therefrom a spectrum signal;

means for measuring the fundamental resonant frequency of said chamber from said spectrum signal, said measured fundamental resonant frequency being a measure of the gas concentrations; and

means for measuring the strength of said spectrum signal, said measured strength being a measure of the gas mixture flow rate corresponding to said gas concentrations.

10. A method for simultaneously detecting concentrations and flow rates of a gas mixture comprising:

passing the gas mixture through a chamber having an inlet and an outlet and a fundamental resonant acoustic frequency varying with the relative gas concentration of the mixture therein;

detecting acoustic noise in said chamber and producing therefrom a spectrum signal;

measuring the strength of said spectrum signal;

filtering said spectrum signal through a pair of parallel filters to produce a pair of attenuated outputs; and

measuring the ratio of the difference between the pair of attenuated outputs to the sum of the pair of attenuated outputs, said measured ratio being a measure of the gas concentrations and said measured strength of the spectrum signal being a measure of the gas mixture flow rate corresponding to said gas concentrations.