This application is the United States national phase of International Application No. PCT/EP2014/067309 filed Aug. 13, 2014, and claims priority to German Patent Application No. 10 2013 216 450.5 filed Aug. 20, 2013, the disclosures of which are hereby incorporated in their entirety by reference.
The invention relates to a test leak device for testing and calibrating a gas leak detector.
Test leaks include a housing filled with a test gas and are provided with a leak with a predetermined known leakage rate, with which the test gas escapes to the outside. The functionality or the precision of the gas leak detector can be tested by measuring the gas escaping from the test leak.
EP 0 742 894 B1 describes a test leak provided with a capillary that achieves a comparatively low leakage rate of 10−7 mbar·l/s or more. Such capillaries cannot be made infinitely small, since they would then become occluded due to air humidity and thus be useless. Up to the present day, it has been impossible to achieve leakage rates of 10−12 mbar·l/s or less with known test leaks. Such leakage rates are required to test leak test devices for very small leaks.
It is an object of the invention to provide a test leak with a low leakage rate in the region of 10−12 mbar·l/s.
The test leak device of the present invention includes a container filled with a gas with at least 10% atmospheric air. The remaining proportion of the gas may be nitrogen, for instance. The container wall is penetrated by at least one capillary. The capillary should have a leakage rate in the range of about 10−5 mbar·l/s to 10−7 mbar·l/s and preferably 10−6 mbar·l/s. Atmospheric air does not cause an occlusion of the capillary and typically has a proportion of helium and a proportion of argon. Helium and argon are typical test gases used in gas leak detection. The proportion of helium in the air in the container should be in a range from three to seven ppm and preferably about 3.5 to 5.5 ppm. A particularly proportion of helium is about 5 ppm. In the present description the term “about” means a respective deviation of ±10%. The proportion of argon in the air in the container should be in a range from 0.1 to 2% and preferably about 0.8 to 1.2%. A particularly advantageous proportion of argon is about 1%.
Filling the test leak container with atmospheric air further makes a separate filling nozzle at the test leak obsolete, which nozzle would increase the outer dimensions and make it more difficult to use in small test chambers.
It is particularly advantageous if the container is a cylinder with a cover on a front end side or with an end cap. The end cap is penetrated by the capillary. The cylinder should not exceed a length of 5 cm and a diameter of about 1 cm. The capillary may be guided within the cylinder along the central axis thereof. It is particularly advantageous if the container is made of glass and the end cap is made of a metal. Such a container may also be used in particularly small test chambers and can be filled in a simple manner. Filling is performed simply by removing the end cap and by the gas flowing into the container together with the atmospheric air. The cylindrical test leak container has a small surface area and may be evacuated in a simple manner in a test chamber due to the absence of gaps or recesses.
The gas in the container should have a relative air humidity of less than 50% and preferably less than 40% so as to avoid occlusion of the capillary by air humidity.
An embodiment will be explained hereunder with reference to the drawing.
The test leak device 10 includes a cylindrical container 12 of glass with a closed bottom 14 at one end face and an open end at the opposite end face. The open end is tightly closed with an end cap 16 of metal. A capillary 18 is guided through the metal cap 16 along the longitudinal central axis of the cylinder 12.
The container 12 is filled with atmospheric air 20 having a proportion of helium of 5 ppm and a proportion of argon of 1%. The capillary 18 has a leakage rate of 10−6 mbar·l/s. The humidity of the air is about 40%. For the test leak device 10, this results in an effective gas flow of:
1·10−6 mbar·l/s·5 ppm=5·10−12 mbar·l/s for helium and
1·10−6 mbar·l/s·1%=1·10−8 mbar·l/s for argon.
While an embodiment of the test leak device 10 is provided in the foregoing description, those skilled in the art may make modifications and alterations to this embodiment without departing from the scope and spirit of the disclosure. Accordingly, the foregoing description is intended to be illustrative rather than restrictive. The invention described hereinabove is defined by the appended claims and all changes to the invention that fall within the meaning and the range of equivalency of the claims are to be embraced within their scope.
Number | Date | Country | Kind |
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10 2013 216 450 | Aug 2013 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2014/067309 | 8/13/2014 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2015/024831 | 2/26/2015 | WO | A |
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Entry |
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International Search Report, PCT/EP2014/067309, dated Nov. 19, 2014, 3 pages. |
Written Opinion International Search Authority, PCT/EP2014/067309, dated Nov. 19, 2014, 8 pages. |
Number | Date | Country | |
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20160195448 A1 | Jul 2016 | US |