Non-dispersive optical determination of gas concentration

• US 4,500,207 A
• Filed: 11/08/1982
• Issued: 02/19/1985
• Est. Priority Date: 11/14/1981
• Status: Expired due to Fees

• Current Assignee: Ferranti Limited
• Original Assignee: Ferranti Limited
• Inventors: Maiden, Adrian J.
• Primary Examiner(s): EVANS, FANNIE L
• Application Number:
  US06/440,040
• Time in Patent Office: 834 Days
• Field of Search: 250/343, 356/51, 356/434, 356/437, 356/409
• US Class Current: 356/409
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis
• CPC Class Codes: G01N 21/3518 Devices using gas filter correlation techniques; Devices using gas pressure modulation techniques

Abstract

Apparatus (FIG. 1) for non-dispersive optical determination of the concentration of an identifiable gas, such as a hydrocarbon, in a mixture such as atmospheric air comprises a sample chamber 13 to contain a sample of the mixture, a source 21 of IR radiation at a wavelength absorbed by the gas beamed through the sample chamber to a detector 22 and transducer means to change the gas pressure within the chamber to determine the change in radiation intensity detected at different pressures. One wall of the sample chamber is formed by a flexible diaphragm 25 driven by a voice-coil type transducer 26 whereby the pressure is switched repetitively between the values above and below atmospheric. Atmospheric gas is admitted to the chamber by a porous plug 24 which restricts flow to a low level permitting a pressure change in the chamber. Absorption by the gas relates the intensity of source radiation I_S and measured radiation I_M by I_M oc I_S ·e^-α o.sup.·g·p·x where x is the radiation path length through the sample, α_o is a constant, p the total pressure of the gas mixture and g the concentration of the hydrocarbon gas. By measuring intensity at different pressure involving a change Δp and a fractional change in intensity of measured radiation ΔI/I, the gas concentration g is determined by applying the relationship:- g=-ΔI/(I·Δp·α_o ·x).

Claims

1. Apparatus for non-dispersive optical determination of the concentration of an identifiable gas in an atmosphere comprising a sample chamber arranged to communicate with the atmosphere by flow limiting means in the form of a plug of porous material operable to limit the rate of gas flow between the chamber and atmosphere to a value whereby after a pressure change is induced in the chamber and for a time period thereafter there is no substantial restoration of gas pressure within the sample chamber towards atmospheric, transducer means operable to change the pressure of the gas mixture in the sample chamber by a predetermined amount between first and second pressures, a source of a beam of radiation at a wavelength absorbed by the identifiable gas only of the mixture, window means by which the radiation is passed through the sample chamber, a detector responsive to radiation at said wavelength after passage through the sample chamber to produce a signal related to the intensity level of the radiation detected, and signal processing means operable to derive a signal representing the fractional change in intensity (Δ

I/I) of the detected radiation due to the pressure change in the sample chamber and calculate from said derived signal, the chamber pressure change (Δ

p), radiation path length through the gas mixture (x) and an absorption constant characteristic of the specific gas (α

_o), a representation of the gas concentration g in accordance with the formula

space="preserve" listing-type="equation">g=-Δ

I/(I·

Δ

pα

.sub.o ·

x).

2. Apparatus as claimed in claim 1 in which the plug is formed of stainless steel.

3. Apparatus as claimed in claim 1 in which source is arranged to emit a beam modulated in intensity.

4. Apparatus as claimed in claim 3 in which the beam is 100 percent modulated by permitting radiation emitted by the source to pass through the sample chamber only intermittently.

5. Apparatus as claimed in claim 4 in which the beam is modulated by switching on and off repetitively the power supply to the source.

6. Apparatus as claimed in of claim 1 in which the transducer means is arranged to modulate the gas pressure within the sample chamber between two values at each of which the intensity of radiation passed through the sample chamber is detected.

7. Apparatus as claimed in claim 6 in which the transducer is arranged to change the pressure periodically between values equally above and below atmosphere pressure.

8. Apparatus as claimed in claim 1 in which the transducer means includes a diaphragm forming part of the wall of the sample chamber and movable to change the volume of the chamber to change the pressure of the gas therein and drive means operable to move at least part of the diaphragm.

9. Apparatus as claimed in claim 8 in which the transducer drive means comprises an electromagnetic voice-coil-like assembly fixed to the diaphragm and movable in a magnetic field by a drive signal applied thereto to produce a pressure change in the chamber in accordance with the magnitude of the drive signal and the impedance of the transducer means.

10. Apparatus as claimed in claim 9 in which the transducer means includes monitor means operable to monitor displacement of the diaphragm in response to a drive signal to provide a correction to the drive signal to effect a demanded diaphragm displacement.

11. A method of non-dispersive optical determination of the concentration of an identifiable gas in the atmosphere comprising holding a sample of the atmospheric gas mixture in a sample chamber in communication with the atmosphere by means of a porous plug operable to limit the rate of gas flow between the atmosphere and the sample chamber to a level at which a pressure change may be effected and radiation intensities measured before any significant flow of gas through the plug restores the pressure within the chamber to atmospheric, passing radiation at a wavelength absorbed by the identifiable gas through the sample chamber, detecting the intensity of radiation at said wavelength received after passage through the chamber with the gas mixture at a first pressure, changing the pressure in the chamber by a predetermined amount (Δ

p) to a second pressure, detecting the intensity of radiation at said wavelength after passage through the chamber with the gas mixture at the second pressure, determining the fractional change in intensity of detected radiation (Δ

I/I) consequent upon the change of gas pressure, and calculating the value of the gas concentration g of the identifiable gas in accordance with the formula;

space="preserve" listing-type="equation">g=-Δ

I/(I·

Δ

p·

α

.sub.o ·

x)

where x is the path length of the radiation through the sample and α

_o is an absorption coefficient constant for the identifiable gas.

12. A method as claimed in claim 11 in which the pressure is changed repetitively between two alternate values disposed about atmospheric pressure and one measurement of gas concentration is made subsequent to each pressure change.

13. A method as claimed in claim 11 or claim 12 in which the sample chamber pressure is changed by changing the volume of the sample chamber while maintaining the mass of gas therein substantially constant.