Measurement device and method for analyzing a sample gas by infrared absorption spectroscopy

• US 9,541,497 B2
• Filed: 12/21/2010
• Issued: 01/10/2017
• Est. Priority Date: 12/24/2009
• Status: Active Grant

• Current Assignee: Humedics GmbH (Advanced Biological Laboratories SA)
• Original Assignee: Humedics GmbH (Advanced Biological Laboratories SA)
• Inventors: Heyne, Karsten, Rubin, Tom
• Primary Examiner(s): Cheng, Jacqueline
• Assistant Examiner(s): Agahi, Puya
• Application Number:
  US13/143,074
• Publication Number:
  US 20110270113A1
• Time in Patent Office: 2,212 Days
• Field of Search: 600/529, 600/531, 600/532, 600/538, 600/539, 600/540, 600/543
• US Class Current: 1/1
• CPC Class Codes: A61B 5/082 Evaluation by breath analysis, e.g. determination of the chemical composition of exhaled breath A61B5/083, A61B5/091 take precedence
• CPC Class Codes: A61B 5/0836 Measuring rate of CO2 production
• CPC Class Codes: A61B 5/087 Measuring breath flow
• CPC Class Codes: A61M 16/12 by mixing different gases
• CPC Class Codes: A61M 2230/432 partial CO2 pressure (P-CO2)
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis
• CPC Class Codes: G01N 21/39 using tunable lasers
• CPC Class Codes: G01N 2800/085 Liver diseases, e.g. portal hypertension, fibrosis, cirrhosis, bilirubin

Abstract

A measurement device and a method for analyzing a sample gas by infrared absorption spectroscopy are described. The measurement device comprises a narrowband laser having a line width of less than 0.2 cm⁻¹ and being smaller than a width of an infrared absorption line to be measured of a sample gas. The measurement device is suited and can be arranged to measure the respiratory gas of a human or animal as sample gas, wherein the respiratory gas exchanges in the measurement chamber only by the respiration of the human or animal, and the respiratory resistance of the measurement device is less than 60 mbar.

Claims

1. A measurement device for analyzing a sample gas by infrared absorption spectroscopy, comprising:

an ante-chamber configured to homogenize the sample gas to be analyzed,

a measurement chamber arranged to receive homogenized sample gas from the ante-chamber,

a laser being arranged in relation to the measurement chamber such that light being emitted from the laser radiates through the measurement chamber, wherein the light being emitted from the laser has a frequency in a range of from 2.498*10⁷ MHz to 1.499*10⁸ MHz,

a detection device detecting the light being emitted from the laser and radiated through the measurement chamber, and

an evaluation unit evaluating signals generated by the detection device regarding a light absorption occurred in the measurement chamber, wherein

the ante-chamber has a single inlet through which the sample gas enters the ante-chamber and at least two branchings of different length and diameter through which parts of the sample gas pass through, wherein the sample gas from the single inlet is separated into the parts of the sample gas by the at least two branchings and the parts of the sample gas are brought together again after the at least two branchings, a total cross section of the at least two branchings being equal to or greater than a cross-section of a single tube that delivers the homogenized sample gas from the ante-chamber to the measurement chamber, wherein

the laser is a narrowband emitting laser having a line width of less than 0.2 cm<sup>−

1</sup> and being smaller than or equal to a width of an infrared absorption line to be measured of the homogenized sample gas, wherein

the laser is designed and arranged such that the laser frequency is varied periodically within a defined spectral range having a width of between 0.5 cm<sup>−

1</sup> and 60 cm<sup>−

1</sup>, wherein the laser frequency and its variation are chosen such that at least two infrared absorption lines to be measured of the homogenized sample gas lie in the defined spectral range, wherein

the evaluation unit is designed and arranged to determine a ratio of two isotopes of the homogenized sample gas on the basis of the light absorptions occurring at two absorption lines, wherein

the detection device is designed and arranged such that it detects the light being emitted from the laser and radiated through the measurement chamber in such a time-resolved manner that the light absorption can be determined frequency-resolved within the defined spectral range, wherein

the detection device carries out a single absorption measurement within 10<sup>−

5</sup> s or faster, wherein

the measurement device is suited and can be arranged to measure the respiratory gas of a human or animal as sample gas, wherein

the measurement chamber has an open construction devoid of obstructions which could hinder the flow of the homogenized sample gas, wherein the measurement device has a constant cross section for the sample gas flowing through so that a laminar flow of sample gas is established in the measurement device, wherein

the respiratory gas exchanges in the measurement chamber only by the respiration of the human or animal, and wherein

the respiratory resistance of the measurement device is less than 60 mbar.

2. The measurement device according to claim 1 wherein the evaluation unit is designed and arranged to determine the ratio of two isotopes in real time.

3. The measurement device according to claim 1, wherein the measurement chamber is mirror-less and light emitted from the laser passes through the measurement chamber exactly once.

4. The measurement device according to claim 3, wherein the measurement chamber has an inlet window through which the laser light enters the measurement chamber and an outlet window through which the transmitted light exits the measurement chamber.

5. The measurement device according to claim 1, wherein furthermore tempering means for tempering the measurement chamber onto a constant temperature are provided.

6. The measurement device according to claim 1, wherein the homogenized sample gas flows through the measurement chamber continuously or intermittently and wherein the measurement chamber has an open construction without valves or air flaps which would hinder the flow of the homogenized sample gas into and out of the measurement chamber.

7. The measurement device according to claim 6, wherein the measurement device is designed and arranged such that a time-resolved light detection by the detection device occurs during flowing-through of the homogenized sample gas through the measurement chamber.

8. The measurement device according to claim 1, having a spirometer detecting the volumetric flow rate of the homogenized sample gas flowing through the measurement chamber.

9. The measurement device according to claim 1, wherein the laser signal is pulsed with a pulse duration of less than 200 ns.

10. The measurement device according to claim 9, wherein the detection device is designed and arranged to be read out with a frequency that is twice as big as the frequency by which the laser emits light pulses.

11. The measurement device according to claim 1, wherein the measurement device is formed such that the light emitted from the laser is divided into two partial beams, wherein a first of the two partial beams passes through the measurement chamber and a second of the two partial beams is detected by a reference detection device, and wherein the evaluation unit evaluates the signals of the reference detection device for standardizing the signal intensity of the laser.

12. The measurement device according to claim 1, wherein the measurement device is designed and arranged to determine the ratio of the ¹³CO₂/¹²CO₂ isotope concentration in the respiratory gas of a human or animal in a time-resolved manner.

13. The measurement device according to claim 1, wherein the measurement device is designed and arranged to conduct a quantitative measurement of a metabolic parameter in the respiratory gas in real time.

14. The measurement device according to claim 1, wherein the measurement device is designed and arranged to determine the carbon dioxide concentration of the respiratory gas in the range between 0.08% and 8% in flow-through in real time.

15. A method for analyzing a sample gas by infrared absorption spectroscopy in a measurement device according to any of the preceding claims, having the steps of:

homogenizing a sample gas in an ante-chamber having a single inlet through which the sample gas enters the ante-chamber and at least two branchings of different length and diameter through which parts of the sample gas pass through, wherein the sample gas from the single inlet is separated into the parts of the sample gas by the at least two branchings and the parts of the sample gas are brought together again after the at least two branchings, a total cross section of the at least two branchings being equal to or greater than a cross-section of a single tube that delivers the homogenized sample gas from the ante-chamber to a measurement chamber,

radiating the measurement chamber with light being emitted from a narrowband laser having a line width of less than 0.2 cm<sup>−

1</sup>, and being smaller than or the width of an infrared absorption line to be measured of the homogenized sample gas being present in the measurement chamber, wherein the measurement chamber has an open construction devoid of obstructions which could hinder the flow of the homogenized sample gas, wherein the light being emitted from the laser has a frequency lying in a rage of from 2.498*10⁷ MHz to 1.499*10⁸ MHz, wherein the laser frequency is varied periodically within a defined spectral range of between 0.5 cm<sup>−

1</sup> and 60 cm<sup>−

1</sup>, and the laser frequency and its variation are chosen such that at least two infrared absorption lines to be measured of the homogenized sample gas lie in the defined spectral range,

time-resolved detecting the light emitted from the laser and radiated through the measurement chamber, wherein a single absorption measurement is carried out within 10<sup>−

5</sup> s or faster, and

evaluating the detected signals regarding a light absorption occurred in the measurement chamber, wherein the light absorption is determined frequency-resolved within the defined spectral range, wherein

a ratio of two isotopes of the homogenized sample gas on the basis of the light absorptions occurring at two absorption lines is determined, wherein

the homogenized sample gas is the respiratory gas of a human or animal,

wherein the respiratory gas is exchanged in the measurement chamber only by the respiration of the human or animal, wherein the respiratory resistance of the measurement device is less than 60 mbar, and wherein the measurement device has a constant cross section for the sample gas flowing through so that a laminar flow of sample gas is established in the measurement device.

16. The method according to claim 15, wherein the ratio of two isotopes of the homogenized sample gas is determined which have absorption lines lying within the defined spectral range.