Measuring the concentration of gaseous hydrogen fluoride

• US 4,535,241 A
• Filed: 11/17/1982
• Issued: 08/13/1985
• Est. Priority Date: 04/13/1981
• Status: Expired due to Term

• Current Assignee: Australian Atomic Energy Commission A Body Corporate of Australia
• Original Assignee: Australian Atomic Energy Commission (Government of Australia)
• Inventors: Eberhardt, John E.
• Primary Examiner(s): Smith, Alfred E.
• Assistant Examiner(s): FIELDS, CAROLYN
• Application Number:
  US06/444,900
• Time in Patent Office: 1,000 Days
• Field of Search: 356/437, 250/343, 250/345, 250/346, 250/339, 250/338
• US Class Current: 250/339.13
• CPC Class Codes: G01N 2021/1704 in gases
• CPC Class Codes: G01N 21/3151 using two sources of radiation of different wavelengths G01N21/33 - G01N21/39 take precedence
• CPC Class Codes: G01N 21/39 using tunable lasers

Abstract

Method and apparatus for quantitatively determining the concentration of gaseous hydrogen fluoride in a medium containing gaseous hydrogen fluoride. The apparatus has one or two lasers (1) (2) which provides a beam (11) having two frequencies, a first frequency which is absorbed by gaseous hydrogen fluoride and a second frequency which is substantially unabsorbed by low pressure gaseous hydrogen fluoride and less absorbed than the first frequency by high pressure gaseous hyrogen fluoride or gaseous hydrogen fluoride plus other gases or vapors. Detectors (12) (15) detect the beam transmitted through the medium and calculator (18) determines the concentration from the outputs of the detectors (12) (15). The preferred lasers (1) (2) are infra red helium-neon lasers.

Claims

1. A method for quantitatively determining the concentration of gaseous hydrogen fluoride in a medium containing gaseous hydrogen fluoride, characterised in that said method comprises combining the results of (a) a measurement of the transmission or absorption of a laser beam at a first frequency corresponding to a neon 3 p₄ -2 s₂ transition through said medium containing gaseous hydrogen fluoride, and (b) a measurement of the transmission or absorption of a laser beam at a second frequency excluding said first frequency, through said medium containing gaseous hydrogen fluoride.

2. The method as defined in claim 1, characterised in that said second frequency is sufficiently removed from said first frequency not to be significantly absorbed by gaseous hydrogen fluoride and not strongly absorbed by other interfering gases or vapours in said medium.

3. The method as defined in claim 1 or claim 2 characterised in that said second frequency excluding said first frequency is between 4753 cm^-1 and 4000 cm^-1.

4. The method as defined in claim 3, characterised in that said second frequency excluding said first frequency is between 4173 cm^-1 and 4176 cm^-1.

5. The method as claimed in claim 4, characterised in that said medium is atmospheric air.

6. An apparatus for quantitatively determining the concentration of gaseous hydrogen fluoride in a medium containing gaseous hydrogen fluoride, characterised in that said apparatus comprises:

(i) a first source of laser light at a first frequency corresponding to a neon 3 p₄ -2 s₂ transition;

(ii) first detecting means associated with said first source, located remote from said first source by a suitable path length for detecting the intensity or absorption of said laser light at said first frequency;

(iii) a second source of laser light at a second frequency excluding said first frequency;

(iv) second detecting means associated wth said second source, located remote from said second source by a suitable path length for detecting the intensity or absorption of said laser light at said second frequency; and

(v) calculating means associated with the outputs of said first and second detecting means to calculate said concentration;

and wherein said medium containing gaseous hydrogen fluoride is located between said first and second sources and said first and second detecting means so that laser light from said first and second sources passes through said medium containing gaseous hydrogen fluoride to said first and second detecting means.

7. The apparatus as defined in claim 6, characterised in that said first source is a helium-neon laser.

8. The apparatus as defined in claim 7 characterised in that said helium-neon laser includes ²⁰ Ne or ²² Ne.

9. The apparatus as defined in claim 6, characterised in that said second source is a helium-neon laser in conjunction with a selective absorber.

10. The apparatus as defined in claim 9, characterised in that said helium-neon laser includes ²⁰ Ne and said selective absorber is an intra-cavity methane cell.

11. The apparatus as defined in claim 9, characterised in that said second source is a ²² Ne helium-neon laser.

12. The apparatus as defined in claim 6, characterised in that said first and second detecting means comprise a pair of detectors or a single detector for detecting and discriminating between the frequencies of said first and second sources.

13. The apparatus as defined in claim 12, characterised in that said detectors are photovolataic or photoconductive cells, bolometers or optically excited acoustic detectors.