Method and apparatus for determining parameters of a gas or plasma flow

• US 6,023,329 A
• Filed: 07/20/1998
• Issued: 02/08/2000
• Est. Priority Date: 07/20/1998
• Status: Expired due to Fees

• Current Assignee: Ole Trinks, Walter Beck
• Original Assignee: Ole Trinks, Walter Beck
• Inventors: Beck, Walter, Trinks, Ole
• Primary Examiner(s): Font, Frank G.
• Assistant Examiner(s): STAFIRA, MICHAEL PATRICK
• Application Number:
  US09/119,335
• Time in Patent Office: 568 Days
• Field of Search: 356/311, 356/316, 356/300, 356/319, 356/320, 356/345, 356/346, 356/432, 356/433, 356/434, 356/435, 356/436, 356/437, 356/438, 356/442
• US Class Current: 356/311
• CPC Class Codes: G01J 3/42 Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry beam switching arrangements G01J3/08
• CPC Class Codes: G01N 21/3103 Atomic absorption analysis
• CPC Class Codes: G01P 5/26 by measuring the direct influence of the streaming fluid on the properties of a detecting optical wave
• CPC Class Codes: H05H 1/0037 by spectrometry

Abstract

A method and an apparatus determines at least one parameter of a material flow. The parameter is for example temperature, pressure or velocity of the gas or plasma flow. The material flow is either a gas or a plasma flow. The method and the apparatus are utilizing atomic absorption spectroscopy and feed a Rubidium compound into the gas or plasma flow, in which the Rubidium compound dissociates into Rubidium atoms. The Rubidium atoms are stimulated with a first laser beam and a first transmitted laser intensity is detected. First absorption lines are determined from the first transmitted laser intensity. Rubidium atoms are stimulated with a second laser beam, a second transmitted reference laser intensity is detected and second reference absorption lines are determined from the second transmitted reference laser intensity. Finally, at least one parameter of the gas or plasma flow is determined from the comparison of the first absorption lines and the second reference absorption lines of the Rubidium atoms.

Claims

1. A method for determining at least one parameter of a gas or plasma flow, said method being based on atomic absorption spectroscopy, said method comprising the steps of:

feeding a Rubidium compound into the gas or plasma flow, in which the Rubidium compound dissociates into Rubidium atoms;

stimulating the Rubidium atoms with a first laser beam;

detecting a first transmitted laser intensity;

determining first absorption lines from the first transmitted laser intensity;

stimulating Rubidium atoms with a second laser beam;

detecting a second transmitted reference laser intensity;

determining second reference absorption lines from the second transmitted reference laser intensity; and

determining at least one parameter of the gas or plasma flow from the comparison of the first absorption lines and the second reference absorption lines of the Rubidium atoms.

2. The method of claim 1, further comprising the step of:

feeding a Rubidium compound into a reference cell containing a gas or plasma of defined pressure and temperature in which the Rubidium compound dissociates into Rubidium atoms prior to said step of stimulating the Rubidium atoms with a first laser beam.

3. The method of claim 1, wherein the Rubidium atoms are stimulated with the second laser beam in a substantially perpendicular orientation relative to a main flow direction of the Rubidium atoms.

4. The method of claim 1, wherein the Rubidium compound comprises a salt.

5. The method of claim 1, wherein the Rubidium compound comprises Rubidium nitrate.

6. The method of claim 1, wherein the step of stimulating the Rubidium atoms with a first laser beam is accomplished by directing the laser beam toward the Rubidium atoms in a substantially perpendicular orientation relative to a main flow direction of the Rubidium atoms.

7. The method of claim 1, wherein one parameter is temperature.

8. The method of claim 1, wherein one parameter is pressure.

9. The method of claim 1, wherein the steps of stimulating the Rubidium atoms with the first and second laser beam are accomplished by sweeping the laser to scan a relevant frequency range of approximately 780.15 nm to 780.35 nm including a D₂ resonant transition of Rubidium atoms at a wavelength of 780.2 nm.

10. A method for determining flow velocity of a gas or plasma flow, said method being based on atomic absorption spectroscopy, said method comprising the steps of:

feeding a Rubidium compound into the gas or plasma flow, in which the Rubidium compound dissociates into Rubidium atoms;

directing a first laser beam of a diode laser toward the Rubidium atoms such that the first laser beam is directed in a substantially perpendicular orientation relative to a main flow direction of the Rubidium atoms;

stimulating the Rubidium atoms with the first laser beam in a frequency range including a D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm;

detecting a first transmitted laser intensity;

determining a first absorption line from the first transmitted laser intensity;

directing a second laser beam of a diode laser toward the Rubidium atoms such that the second laser beam is directed in a non perpendicular orientation relative to the main flow direction of the Rubidium atoms;

stimulating the Rubidium atoms with the second laser beam in a frequency range including the D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm;

detecting a second transmitted laser intensity;

determining a second absorption line from the second transmitted laser intensity;

acquiring a Doppler shifted and broadened absorption line of the first and second transmitted laser intensities;

feeding a Rubidium compound into a reference cell containing a gas or plasma of defined velocity, in which the Rubidium compound dissociates into Rubidium atoms;

stimulating the Rubidium atoms with a third laser beam;

detecting the third transmitted laser intensity;

determining the third absorption line from the third transmitted laser intensity; and

determining flow velocity of the gas or plasma flow from the shift in the acquired Doppler shifted and broadened first and second absorption line with respect to the third absorption line of the Rubidium atoms, wherein the magnitude of the shift is directly proportional to the flow velocity of the gas or plasma flow.

11. The method of claim 10, wherein the laser beam directed in a non perpendicular orientation is directed toward the main flow direction of the Rubidium atoms at an angle of approximately between 40 and 60 degrees.

12. An apparatus for determining at least one parameter of a gas or plasma flow, comprising:

at least one laser for stimulating Rubidium atoms flowing in a main flow direction of the gas or plasma flow with a first laser beam in a frequency range including a D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm;

at least one photo detector detecting a first transmitted laser intensity of said laser for stimulating Rubidium atoms;

wherein a first absorption line is determined from the first transmitted laser intensity;

a reference cell containing Rubidium atoms in a gas or plasma having defined pressure and temperature;

a second laser beam for stimulating Rubidium atoms in said reference cell in a frequency range including the D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm;

at least one photo detector detecting a second transmitted laser intensity of the second laser beam;

wherein a second absorption line is determined from the second transmitted laser intensity, and wherein at least one parameter of the gas or plasma flow is determined from the comparison of the first and the second absorption line.

13. The apparatus of claim 12, wherein said at least one laser is a diode laser.

14. The apparatus of claim 12, wherein the at least one laser is directed toward the Rubidium atoms such that at least one laser beam emitted from said laser would project in a direction that is substantially perpendicular to the main flow direction of the Rubidium atoms.

15. The apparatus of claim 12, wherein one parameter is temperature.

16. The apparatus of claim 12, wherein one parameter is pressure.

17. An apparatus for determining flow velocity of a gas or plasma flow, comprising:

a high enthalpy tunnel;

at least one laser for stimulating Rubidium atoms flowing in a main flow direction of the gas or plasma flow with a first laser beam in a frequency range including a D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm;

the first laser beam being directed in a perpendicular orientation relative to the main flow direction of the Rubidium atoms;

at least one photo detector detecting a first transmitted laser intensity of the first laser beam;

wherein a first absorption line is determined from the first transmitted laser intensity;

a second laser beam stimulating Rubidium atoms flowing in the main flow direction of the gas or plasma flow in a frequency range including the D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm, the second laser beam being directed in a non perpendicular orientation relative to the main flow direction of the Rubidium atoms;

at least one photo detector detecting a transmitted laser intensity of the second laser beam stimulating Rubidium atoms in said high enthalpy tunnel;

wherein a second absorption line is determined from the second transmitted laser intensity wherein a Doppler shifted and broadened absorption line of the first and second transmitted laser intensity is acquired;

a reference cell containing Rubidium atoms in a gas or plasma having a defined velocity;

a third laser beam stimulating Rubidium atoms in said reference cell in a frequency range including the D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm;

at least one photo detector detecting a third transmitted laser intensity of the third laser beam for stimulating Rubidium atoms in said reference cell;

wherein a third absorption line is determined from the third transmitted laser intensity, wherein the flow velocity of the gas or plasma flow is determined from the shift in the acquired Doppler shifted and broadened first and second absorption line with respect to the third absorption line of the Rubidium atoms in the reference cell, wherein the magnitude of the shift is directly proportional to the flow velocity of the gas or plasma flow.

18. An apparatus for determining the flow velocity of a gas or plasma flow, comprising:

means for feeding a Rubidium compound into the gas or plasma flow, in which the Rubidium compound dissociates into Rubidium atoms;

means for stimulating the Rubidium atoms with a laser beam;

means for detecting a transmitted laser intensity;

means for determining absorption lines from the transmitted laser intensity

means for stimulating the Rubidium atoms with a reference laser beam;

means for detecting a transmitted reference laser intensity;

means for determining reference absorption lines from the transmitted reference laser intensity; and

means for determining at least one parameter of the gas or plasma flow from the comparison of the absorption lines and the reference absorption lines of the Rubidium atoms.

19. The apparatus of claim 18, wherein said means for stimulating the Rubidium atoms with the reference laser beam comprise a reference cell containing a gas of defined pressure and temperature into which a Rubidium compound is fed and in which the Rubidium compound dissociates into Rubidium atoms.

20. The apparatus of claim 18, wherein the means for stimulating the Rubidium atoms with a reference laser beam stimulate the Rubidium atoms in a substantially perpendicular orientation relative to a main flow direction of the Rubidium atoms.

21. The apparatus of claim 18, wherein the Rubidium compound comprises a salt.

22. The apparatus of claim 18, wherein the Rubidium compound comprises Rubidium nitrate.

23. The apparatus of claim 18, wherein the means for stimulating the Rubidium atoms sweep for scanning a relevant frequency range of approximately 780.15 nm to 780.35 nm including the D₂ resonant transition of Rubidium atoms at a wavelength of approximately 780.2 nm.