Method and device for optical pressure measurement of a gas in a closed container

• US 20120266681A1
• Filed: 05/10/2010
• Published: 10/25/2012
• Est. Priority Date: 05/23/2009
• Status: Active Grant

• Current Assignee: Heuft Systemtechnik GmbH
• Original Assignee: Hochschule Fuer Angewandte Wissenschaften Hamburg
• Inventors: Baumann, Bernd, Wolff, Marcus
• Granted Patent: US 8,707,790 B2
• Time in Patent Office: Days
• US Class Current: 73/705
• CPC Class Codes: G01L 11/02 by optical means

Abstract

Method for optical pressure measurement of a gas in a closed container by directing a radiation of a radiator through the container and measuring the transmitted radiation by a detector, wherein

• • the radiation of the radiator covers at least one first wavelength range in which there is an absorption of the radiation by the gas,
  • the intensity of the transmitted radiation is detected in a second wavelength range by the detector, wherein the second wavelength range overlaps at least partially with the first wavelength range, and
  • an accumulated intensity of the detected radiation in the second wavelength range is assigned to a pressure of the gas.

Claims

1. Method for optical pressure measurement of a gas in a closed container by directing a radiation of a radiator through the container and measuring the transmitted radiation by a detector, wherein:

the radiation of the radiator covers at least one first wavelength range in which there is an absorption of the radiation by the gas,

the intensity of the transmitted radiation is detected in a second wavelength range by the detector, wherein the second wavelength range overlaps at least partially with the first wavelength range, and

an accumulated intensity of the detected radiation in the second wavelength range is assigned to a pressure of the gas.

2. The method according to claim 1, wherein the radiation is directed through the gas in the gas phase.

3. The method according to claim 1, wherein the radiation is directed through the gas which is dissolved in a liquid.

4. A method according to claim 1, wherein the radiator radiates with a continuous spectrum in the first wavelength range.

5. The method according to claim 4, wherein a thermal radiator is provided as radiator, whose radiated spectrum corresponds to a Planck spectrum.

6. A method according to claim 1, wherein at least one light emitting diode is provided as radiator.

7. A method according to claim 1, wherein a laser is provided as radiator, a semiconductor laser in particular, whose radiated wavelength is modulated in the first wavelength range.

8. A method according to claim 1, wherein the second wavelength range of the detector covers also the wavelengths of the first wavelength range, in which there is an absorption by the gas.

9. A method according to claim 1, wherein the first wavelength range of the radiator is limited to the second wavelength range by one or several filters.

10. A method according to claim 1, wherein the accumulated intensity in the second wavelength range corresponds to the intensity that is summed up or integrated over the second wavelength range.

11. A method according to claim 1, wherein the value of the accumulated intensity is assigned to a pressure value via at least one predetermined characteristic curve.

12. A method according to claim 1, wherein carbon dioxide is intended as gas.

13. The method according to claim 12, wherein the radiation is directed through a closed beverage bottle.

14. A method according to claim 1, wherein the radiation is directed through a container which is filled with a protective gas.

15. A method according to claim 1, wherein the radiation is directed through a vacuum closed container.

16. A method according to claim 1, wherein the allocation of the accumulated intensity to the pressure takes place depending on the transmission spectrum of the container.

17. Device for the optical pressure measurement of a gas in a closed container, said device including:

a radiator, which generates a radiation in a first wavelength range, wherein there is an absorption of the radiation by the gas in the first wavelength range,

a detector, which detects the intensity of the radiation transmitted through the container and the gas in a second wavelength range, wherein the second wavelength range overlaps at least partially with the first wavelength range, and

with an analysing unit, which assigns a pressure value to an intensity accumulated in the second wavelength range.

18. The device according to claim 17, wherein a thermal radiator is provided, whose radiated spectrum corresponds to a Planck spectrum.

19. The device according to claim 17, wherein one or several light emitting diodes with a continuous spectrum are provided.

20. The device according to claim 17, wherein a laser is provided as radiator, a semiconductor laser in particular, whose radiation can be modulated in the first wavelength range.

21. A device according to claim 17, wherein within the second wavelength range, the detector has several switchable measurement ranges, in which the pressure value is determined for different pressure ranges of the gas.

22. A device according to claim 17, wherein the analysing unit has a characteristic curve, which assigns the pressure value to the accumulated intensity.

23. A device according to claim 17, wherein the analysing unit has plural characteristic curves depending on the transmission spectrum of the container, each one assigning the pressure value to the accumulated intensity.