The present invention specifically relates to the pneumatic and electronic application of a pneumatic leak meter based on absolute pressure drop measurement having the peculiarity of compensating for ambient variations such as ambient temperature and temperature of the measured part, as well as mechanical deformations of the component being tested caused by the pressure being applied.
According to the detailed classification in standard EN1779, the instruments used for leak testing fall into two basic categories, namely:
In the field of air/air ATE instrumentation, two types of measurement systems based on pressure drop measurement predominantly come into consideration, namely those based on absolute pressure drop measurement of the test part and those based on differential pressure drop measurement of the test part.
Both systems calculate the leak rate by measuring pressure decay over time, which can be expressed by the following function:
Leak=dp/dt
Meters of the “absolute pressure drop” type calculate the leak by analysing the “direct” pressure decay, i.e. after completion of the filling/pressurization phase, the branch being measured is isolated hermetically using a leak-free valve, enabling the equipment to analyse any possible pressure drop of the object being tested.
Meters of the “differential pressure drop” type perform a similar measurement, but compare the pressure decay of the object being tested with a hermetic sample volume referred to as “reference part”.
Unlike absolute pressure drop systems, differential pressure drop systems use a second differential pressure transducer, and the whole pneumatic circuit is more complex due to the low sensitivity (or resolution accuracy) of past pressure sensors. Indeed, a characteristic of the pressure drop over time (dp/dt) is that the smaller the appreciable difference in pressure (dp), the greater the sensitivity, speed and accuracy of the measurement.
For this reason, as early as in the 1970s, it was possible to produce differential pressure drop meters with a resolution capability of tenths of Pascals, which was not achievable at the time using absolute pressure drop systems.
Furthermore, as a result of the use of differential transducers, the processing and management electronics of this equipment was, at the time, extremely simplified, the measurement having no offset and being indeed “central zero”.
Conversely, and in parallel with the development of industrial force and weight measurements, the quality of pressure measurements and pressure transducers has improved significantly over the years, such that today it is possible to obtain the same measurement resolution, even with very high offset values, as is the case with leak measurements of the “absolute pressure drop” type.
The application of microprocessors and related calculation and compensation algorithms have led, over time, to performances of measurements of the “absolute pressure drop” type that are more than comparable with measurements of the “differential pressure drop” type, thereby simplifying the pneumatic sections and improving the overall reliability of the measurement systems.
There nonetheless remains an intrinsic benefit in circuitry of the “differential” type, which is related to the partial (or apparent) common-mode compensation of the measurements; in fact, all pressure decay measurement systems implies the Gay-Lussac law of ideal gases:
pV=nRT
from which it can be inferred that thermal variances of the environment or of the test part cause errors and drift in the measurement.
For this reason, differential pressure drop meters enable compensation, precisely by virtue of the common-mode elision of two components being measured (namely the part being tested and the reference part) under the same thermal conditions.
It is clear, however, that the volume variances caused by expansions of the two components being tested in turn cause measurement errors. Indeed, in a differential pressure drop system, commonly intended for industrial production, with a high operating frequency, the mechanical expansion of the component being tested is understood to be limited to the measurement operation only, while the mechanical stress on the reference sample part will accumulate for the entire usage time of the equipment to an indefinite number of times, ultimately leading to a continuous drift of the behaviour between the two parts—typically—after just 15/30 minutes of work at steady regime.
Similarly, as a result of the continuous pressurization and emptying of the single reference sample part, there is an increasing thermal accumulation that triggers endogenous thermal effects, thereby partially nullifying the effect of thermal compensation.
In practice, empirical surveys have shown that a metal component with a volume of 300 cc subjected to a relative pressure of 2 bar requires at least 20 minutes in order to restore the conditions of elasticity and rest temperature, namely return to a repeatability margin of 10% compared to the first test carried out.
For this reason, the concept of apparent repeatability has been introduced, over time, in the use of differential pressure drop meters, namely the phenomenon of good repeatability when taking repeated measurements on the same component, measurement stability that is not however maintained during practical use in production.
As a partial solution to the foregoing, manufacturers have devised different variants of algorithms designed to integrate and average, over time, the trends in tests considered to be “good”, namely measurements falling within limits of acceptability, and to use this data to obtain an average trend of what is considered to be the “sample part”.
The limitations of all of these analysis systems can be found in the basic incongruity of the concept, namely that the components measured from time to time are not quality standards but rather parts with intrinsic variability.
The practical reason for the unreliability of the aforementioned algorithms can be found in the complexity of the error accumulated during the measurements. In fact, in addition to a temperature and expansion drift, practical application also involves possible elastic phenomena of the systems providing connection to the component being measured, vibrations, and spurious movements during testing.
The accumulation of all of these errors, in practice, significantly limits the use of these filters since the time and level parameters are too different from one another.
In this context, the underlying technical objective of the present invention is to provide a system for measuring pneumatic leaks that overcomes the drawbacks of the prior art mentioned above, which system takes the form of a simple, robust and reliable solution.
This and other objectives are achieved thanks to the features of the invention as set forth in the independent and dependent claims, which outline preferred and/or particularly advantageous aspects of the invention.
In particular, the preferred embodiment of the present invention provides a pneumatic leak measurement system based on differential pressure drop measurement, which system comprises two absolute pressure drop measurement circuits and associated electronics to subtract the pressure values measured by the two measurement circuits one from the other.
Thanks to this solution it is therefore possible to:
More specifically, the system according to the invention relies on a traditional high-resolution absolute pressure drop meter combined with a second similar branch connected to a reference component/part, wherein the reference component/part is understood to be a quality, leak-free reference sample.
These objectives and advantages are all achieved thanks to the pneumatic leak measurement system based on absolute pressure drop measurement, with reference sample differential compensation according to the present invention, as characterized in the claims appended hereto.
This and other features of the present invention will appear more clearly from reading the following detailed description of embodiments of the invention which are presented solely by way of non-restrictive examples and illustrated by the attached drawings in which:
With particular reference to
More specifically, reference numeral 1 designates a pneumatic “filling” or pressurization section of the object 4 being measured.
Industrial air, designated by reference numeral 6 in
As shown in the diagram of
Filling or pressurization of the test object 4 is monitored over time by the pressure meter 2. In the illustrated embodiment, the pressure meter 2 is a relative pressure meter operating relative to ambient pressure, i.e. the pressure value measured by the pressure meter 2 is measured relative to ambient pressure.
The aforementioned first circuit 7 thus acts as a first absolute pressure drop measurement circuit 7 for the purpose of measuring pressure decay over time of the test object 4.
The system 100 also includes a second absolute pressure drop measurement circuit 8, similar to the first circuit 7, likewise including a dedicated pneumatic valve and a pressure meter 3 connected on the relevant pneumatic line of the circuit 8. Similarly to pressure meter 2, the pressure meter 3 is a relative pressure meter operating relative to ambient pressure.
An end portion of the measurement circuit 8, namely of the pneumatic line thereof, can be connected or not to a reference element or sample 5 as a function of the required measurement, that is:
In the asymmetrical differential measurement mode (with no reference element/sample connected to the measurement circuit 8), the electronics associated with the system 100 of
Alternatively, in the case of symmetrical measurement (with a hermetic sample/reference part 5 connected to the measurement circuit 8), the electronics associated with the system 100 of
The aforementioned method ensures that the resulting differential measurement is free from and unaffected by mechanical stress phenomena and variations in ambient temperature.
More specifically, in addition to the associated electronics, the system 100 may further provide for the management of calculations using software such that it is possible to:
To do so (and also to avoid creating unnecessary downtime in production cycles), via hardware indications of external automations, and internal logic of the instrument, the software may further manage a “reservation” and “execution” cycle of the “reference” sample part, and via percentage parameters of the totality of the measurements taken, as well as minimum and maximum times, take measurement samples at intervals of time that are long enough not to wear out the mechanical characteristics of the reference part, but frequent enough to “chase” or track ambient variations.
Sampling takes place in any case each time the system is turned on, and special “average” algorithms on the acquired points enable the different reference curves acquired to be refined over time and filtered, while avoiding any sudden and unwanted spurious effects.
Naturally, a person skilled in the art can undertake further modifications and variations to the invention described above in order to meet specific contingent applicational requirements, said variations and modifications nonetheless falling within the scope of protection defined in the subsequent claims.
Compared to a traditional differential pressure drop meter based on a differential transducer, the present invention brings the following technical improvements:
Number | Date | Country | Kind |
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01609/18 | Dec 2018 | CH | national |
Filing Document | Filing Date | Country | Kind |
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PCT/IB2019/061340 | 12/24/2019 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2020/136582 | 7/2/2020 | WO | A |
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5142483 | Basham | Aug 1992 | A |
9638559 | Zummo et al. | May 2017 | B1 |
20090132185 | Furuse | May 2009 | A1 |
20160018288 | Eckhardt | Jan 2016 | A1 |
20180259421 | Schindler | Sep 2018 | A1 |
Number | Date | Country |
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102 42 491 | May 2003 | DE |
Number | Date | Country | |
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20220057289 A1 | Feb 2022 | US |