Method and apparatus for the detection of a gas using photoacoustic spectroscopy

• US 5,159,411 A
• Filed: 05/08/1991
• Issued: 10/27/1992
• Est. Priority Date: 09/12/1988
• Status: Expired due to Fees

• Current Assignee: FLS Airloq A/S
• Original Assignee: FLS Airloq A/S
• Inventors: Henningsen, Jes, Hammerich, Mads, Olafsson, Ari
• Primary Examiner(s): Rosenberger, Richard A.
• Application Number:
  US07/663,852
• Time in Patent Office: 538 Days
• Field of Search: 356/432 T, 356/437, 356/432, 250/343
• US Class Current: 356/432
• CPC Class Codes: G01N 2021/1704 in gases
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids

Abstract

In a process for the detection of a first gas in a gas mixture comprising a second gas, the absorption spectre of which interferes with the absorption spectre of the first gas, a photoacoustic measurement is carried out in the presence of a third gas which in combination with the first or the second gas exhibits kinetic cooling. During measurement the gas mixture is influenced by pulsating laser light having a constant repetition frequency where the frequency of the laser light is varied gradually. The measurement comprises at least one detection of the phase of the photoacoustic signal as a function of the laser light frequency. The invention further relates to an apparatus for carrying out the invention.

Claims

1. A method for the detection of a first gas in a gas mixture through photoacoustic spectroscopy, wherein the gas mixture further comprises a second gas the absorption spectrum of which interferes with the absorption spectrum of the first gas, wherein the gas mixture is irradiated by pulsating laser light having a constant pulsation frequency and therefore a uniform wavelength during the measurement and wherein the wavelength of the laser light is varied gradually and wherein the measurement comprises at least one reading of the phase of the photoacoustic signal as a function of the uniform wavelength during measurement, characterized in that a photoacoustic measurement is carried out in the presence of a third gas in the gas mixture, said third gas being present in the gas mixture or being added to the mixture immediately before the measurement and exhibiting kinetic cooling in combination with the first or the second gas.

2. A method according to claim 1, characterized in that, during the measurement, the gas mixture is provided in a measurement chamber where the pressure is reduced as compared to the atmospheric pressure.

3. A method according to any one of claims 1 or 2, characterized in that, during measurement, the gas mixture is provided in a measurement chamber which is constructed as an acoustic resonator and in that the resonance frequency of the measurement chamber is substantially identical with the pulsation frequency of the laser light.

4. A method according to claim 3, characterized in that the measurement also comprises the reading of the amplitude of the photoacoustic signal as a function of the wavelength of the laser light.

5. A method according to claim 3, characterized in that the absorption of the gas mixture is measured both as to amplitude and phase at a minimum of one wavelength at which the first gas exhibits absorption, that the third gas is added to the gas mixture which third gas coacts with either the first or the second gas in such a way that they exhibit kinetic cooling, that the absorption of the gas mixture is measured again at the same wavelength, and that the minimum of two amplitude and phase measurements are combined to determine the absorption amplitude of the first gas.

6. A method according to any one of the claims 1-2, characterized in that the measurement also comprises the reading of the amplitude of the photoacoustic signal as a function of the wavelength of the laser light.

7. A method according to claim 6, characterized in that the absorption of the gas mixture is measured both as to amplitude and phase at a minimum of one wavelength at which the first gas exhibits absorption, that the third gas is added to the gas mixture which third gas coacts with either the first or the second gas in such a way that they exhibit kinetic cooling, that the absorption of the gas mixture is measured again at the same wavelength(s), and that the minimum of two amplitude and phase measurements are combined to determine the absorption amplitude of the first gas.

8. A method according to any one of claims 1-2, characterized in that the absorption of the gas mixture is measured both as to amplitude and phase at a minimum of one wavelength at which the first gas exhibits absorption, that the third gas is added to the gas mixture which third gas coacts with either the first or the second gas in such a way that they exhibit kinetic cooling, that the absorption of the gas mixture is measured again at the same wavelength(s), and that the minimum of two amplitude and phase measurements are combined to determine the absorption amplitude of the first gas.

9. An apparatus for carrying out the method according to claim 1 comprising in combination a laser, means for pulsation of the laser light, a measuring cell exhibiting acoustic resonance at a frequency which is substantially identical with the pulsation frequency of the laser light, a detector for the detection of the radiation passing through the measuring cell, a detector for the detection of an acoustic signal from the measuring cell, and an electronic measurement circuit for processing the signal from the detectors, characterized in that the wavelength of the laser is settable within certain wavelength intervals, and in that the electronic circuit comprises phase detection means constructed to record the phase course of the acoustic signal as a function of the wavelength of the laser within a wavelength interval over which the absorption spectrum of the gas to be measured changes measurably.