Method and apparatus for measuring stable isotopes

• US 4,684,805 A
• Filed: 08/21/1985
• Issued: 08/04/1987
• Est. Priority Date: 08/21/1985
• Status: Expired due to Term

• Current Assignee: General Motors Auto OOO (General Motors Company)
• Original Assignee: General Motors Corporation (Motors Liquidation Co. GUC Trust)
• Inventors: Shu-Ti Lee, Peter, Partin, Dale L., Majkowski, Richard F.
• Primary Examiner(s): Church, Craig E.
• Assistant Examiner(s): Freeman, John C.
• Application Number:
  US06/767,742
• Time in Patent Office: 713 Days
• Field of Search: 250/339, 250/341, 250/344-345, 250/373, 250/343, 250/346, 356/434-435, 356/440, 356/320, 356/413
• US Class Current: 250/343
• CPC Class Codes: G01N 2021/1746 Method using tracers
• CPC Class Codes: G01N 21/39 using tunable lasers
• CPC Class Codes: G01N 2201/0662 Comparing measurements on two or more paths in one sample

Abstract

Spectroscopic measurements of stable isotopes are performed using a tunable lead salt diode laser. The design of the system is based upon the optimization of isotopic spectral lines from two different path lengths in an absorption cell using a single gaseous sample. A short path cell to measure the more abundant species and a long path cell to measure the less abundant species are used. A micrometer adjustment of a path length is used for equalizing spectral line intensities to obtain a measure of isotope enrichment or of absolute isotopic concentration.

Claims

1. The method of measuring different concentrations of isotopes in a sample comprising the steps of;

transmitting monochromatic radiation through the sample in at least two different path lengths, which comprise at least one short path length and at least one long path length, and sweeping the radiation frequency over absorption lines of the isotopes being measured,

detecting the intensities of spectral lines in the different paths to measure more abundant isotopes in the short path lengths and less abundant isotopes in the long path lengths,

adjusting the relative path lengths to obtain a non-saturated spectral line intensity for each isotope being measured, measuring the relative path lengths, and determining the concentrations of the isotopes from the relative path lengths and the detected spectral line intensities.

2. The method of measuring different concentrations of stable isotopes in a gaseous sample comprising the steps of;

transmitting monochromatic radiation through the sample in at least two different path lengths, which comprise at least one short path length and at least one long path length, and

sweeping the radiation frequency over absorption lines of the isotopes being measured,

detecting the intensities of spectral lines in the different paths to measure more abundant isotopes in the short path lengths and less abundant isotopes in the long path lengths,

adjusting at least one path length to equalize the detected intensities, measuring the relative path lengths, and

determining the concentrations of the isotopes from the relative path lengths and/or the detected spectral line intensities.

3. The method of measuring different concentrations of stable isotopes in a gaseous sample comprising the steps of;

introducing a reference gas into a cell,

transmitting monochromatic radiation through the reference gas in at least two different path lengths, which comprise at least one short path length and at least one long path length, and sweeping the radiation frequency over absorption lines of the isotopes being measured,

detecting the intensities of spectral lines in the different paths to measure more abundant isotopes in the short path lengths and less abundant isotopes in the long path lengths,

equalizing the detected intensities, removing the reference gas from the cell introducing the sample gas into the cell,

repeating the transmitting and detecting steps, and

adjusting the length of at least one of the paths to equalize the detected intensities for the sample gas, so that the amount of the adjustment represents the isotope enrichment in the sample.

4. Apparatus for measuring different concentrations of stable isotopes in a gaseous sample comprising;

a tunable source of monochromatic radiation for scanning radiation through a frequency band,

a sample cell arrangement having at least two optical paths through the same sample, the paths having different lengths in a ratio generally corresponding to the inverse ratio of the isotope concentrations,

means for transmitting radiation from the source through the paths,

detector means for sensing the spectral line intensity of each of isotope,

means for adjusting at least one path length by measured amounts to adjust the line intensity of the corresponding path, and

circuitry responsive to the detector means for determining isotope concentration from the path lengths and/or the respective line intensities.

5. Apparatus for measuring isotope enrichment in different concentrations of stable isotopes in a gaseous sample comprising;

a tunable source of monochromatic radiation for scanning the frequency through a band,

a sample cell arrangement having at least two optical paths through the same sample, the paths having different lengths in a ratio generally corresponding to the inverse ratio of the isotope concentrations,

means for transmitting radiation from the source through the paths,

detector means for measuring the spectral line intensity of an isotope in each optical path, and

means for adjusting the relative path lengths by measured amounts to equalize the measured line intensities, so that the amount of adjustment for a sample gas relative to a reference gas is a measure of isotope enrichment.

6. Apparatus for measuring different concentrations of stable isotopes in a gaseous sample comprising;

a tunable source of monochromatic radiation for scanning radiation through a frequency band,

a sample cell arrangement having at least two optical paths through the same sample, the paths having different lengths in ratio generally corresponding to the inverse ratio of the isotope concentrations,

means for transmitting radiation from the source through the paths,

detector means for measuring the spectral line intensity of each isotope,

means for adjusting at least one of the path lengths for equalizing the line intensities, and

circuitry responsive to the detector means for comparing the line intensities for indicating equality of line intensities for different path lengths.

7. Apparatus for measuring different concentrations of stable isotopes in a gaseous sample comprising;

a tunable source of monochromatic radiation for scanning radiation through a frequency band,

a sample cell arrangement having at least two optical paths through the same sample, the paths having different lengths in a ratio generally corresponding to the inverse ratio of the isotope concentrations,

means for transmitting radiation from the source through the paths,

detector means for measuring the spectral line intensity of each isotope, and

micrometer adjustment means for precisely adjusting at least one of the path lengths for varying the line intensities, so that isotope concentrations can be accurately determined from measured path lengths and line intensities.

8. The method of measuring the isotopic ratio of different concentrations of stable isotopes in a gaseous sample comprising the steps of;

transmitting monochromatic radiation through at least two different length paths in the absence of gas, detecting the transmitted radiation in each path and electronically equalizing the detectected signals,

admitting sample gas into the paths,

transmitting the radiation through the paths and sweeping the radiation frequency over absorption lines of the isotopes being measured,

detecting the intensities of spectral lines in the different paths to measure more abundant isotopes in short path lengths and less abundant isotopes in long path lengths,

adjusting at least one path length to equalize the detected intensities, measuring the relative path lengths and

calculating the absolute isotopic ratio from the relative path lengths, the absorption coefficients and the Beer-Lambert law.