In-line testing of hollow bodies with a pressure difference once a given pressure has been reached

Abstract: Plastic bottles (1) are inline tested in that a predetermined volume (29) is loaded with a predetermined pressure of gas, said predetermined volume (29) is sealingly connected to the interior of the bottle (1) and the pressure resulting in the composite volume of predetermined volume and of said bottle to be tested is measured as indication whether the bottle accords with a rated volume or not.

Description: The present invention relates to testing of hollow bodies. In the packaging of certain foodstuffs such as sweeteners and coffee or also medications such as, for example, effervescent tablets, it is essential that the packaging containers are sealed tight against the environment in order to prevent the packaged goods from becoming contaminated by, for example, atmospheric humidity. The goods are sometimes packed in containers such as bottles, cans or pouches. These containers are generally dimensionally stable or flexible hollow bodies which are fitted with lids or closable sections which can be opened, but which in the closed state are intended to tightly seal the interior of the hollow body. Various procedures, for example welding, are used in the manufacture of such containers. In addition to the tightness of such hollow bodies, also the rigidity of the walls of the dimensionally stable containers, especially in the area of junction points, is an essential criterion determining their usability. Excessively rigid or excessively weak sections such as weld seams, may result in cracks forming when the container is in use, for example, in areas where parts of different rigidity are joined. A testing method and apparatus for flexible hollow bodies is known from the EP-A1-0 313 678. Thereby, such bodies are provided within a test chamber and there is applied a positive or negative pressure to the test chamber as an initial pressure value. Although very accurate tests may be performed by monitoring the behaviour of the pressure in the test. chamber, this known technique has several drawbacks: using a test cavity results in a relatively slow test procedure not suited for fast in-line tests, using a difference measurement of pressures may further slow down the procedure by flow times of gas, applying positive or negative pressure to apply a pressure difference across the wall of such bodies is often not equally advantageous. General volume or leak testing of plastic bottles in a production line is further known from the EP-0 295 371. One object of the present invention is to avoid disadvantages as those mentioned and to create a testing method for such hollow bodies as well as a corresponding apparatus for testing such hollow bodies in a simple fast and greatly reliable manner. This is solved with claim 1 or claim 2, wherein a delimitation is in intended against US-A-2 784 373. A method is proposed wherein the hollow body is placed in a test chamber and is subjected to a positive or negative pressure difference between the internal pressure of the hollow body and the pressure in the test chamber, whereby conclusions can be drawn regarding the tightness of the hollow body or its change in volume from the behaviour of the pressure in the test chamber. When such a hollow body, which is optionally and preferably filled, is introduced into a test chamber and the chamber is filled with a test gas, preferably air, or the hollow body is directly filled with test gas - without making use of a test chamber -, such gas having a positive or negative pressure difference relative to the internal or external pressure of the hollow body respectively, a pressure equalization will take place between internal and external pressure of the hollow body depending on the tightness or leakage of the hollow body. The rate at which this equalization process takes place is a measure of the magnitude of any leakage that is present. Similarly, any increase or decrease in the volume of the hollow body will exert an effect which is a measure of the elasticity of the walls of the hollow body. The volume will increase when the pressure difference is directed outwards from the hollow body and it will decrease when the pressure difference is directed towards the interior of the hollow body. To easily and rapidly apply a predetermined pressure, practically as the initial pressure to the test chamber or the interior of the body, after sealing off the pressurized chamber containing the hollow body or the body itself, in order to derive the above mentioned criteria from the pressure curve, a reference chamber is inventively pressurized to a given pressure and then joined to the test chamber or body in order to produce the pressure difference. The pressure in the test chamber or body is then derived from the pressure level set in the reference chamber and the volume ratio of the two chambers, i.e. reference chamber to test chamber or reference chamber to interior volume of the body. Thereby, a simple and fast test method for the volume of the body most suited for fast in-line testing of bottles is created. Further, to create a defined reference pressure for the purpose of evaluating the internal pressure of the test chamber or of the body and in order to be able to perform the evaluation on the basis of a pressure difference measurement, the chamber or the interior of the body is connected with a reference pressure system prior to evaluation. Then the reference pressure system is disconnected from the chamber or body and its pressure is the reference pressure for subsequent evaluation of the chamber or body pressure. Furthermore, by carrying out the evaluation of the chamber or body pressure at a particular point in time, the process of the evaluation becomes extremely simple. At a given point in time a check is carried out to ascertain whether the ACTUAL chamber or body pressure corresponds to the DESIRED chamber or body pressure which has been selected in advance, for example, for tight hollow bodies or bodies of rated volume. If the ACTUAL test pressure is compared at two or more points in time, or even continuously in time, with DESIRED pressure values for two or more points in time or with a DESIRED pressure-time curve, then especially in the case of very small leaks or volume deviations the resolving power of the evaluation process is increased, for example, by integrating the comparative result or the DESIRED-ACTUAL difference. Furthermore, pre-selected DESIRED pressure values or DESIRED pressure curves are preferentially stored when carrying out the test mentioned above, they are compared with the recorded ACTUAL values in order to determine whether a hollow body should, for example, be rejected because of excessive leakage or volume or because it has excessively stiff or excessively elastic wall sections. Pressure generating elements are preferably linked through at least one first shut-off member with a reference chamber, with the reference chamber being, in turn, connected through at least one second shut-off member with the test chamber or directly the interior of the body. The pressure-recording elements may comprise at least one pressure difference sensor having one input directly linked with the test chamber or body and a second input connected in parallel with the test chamber or body by way of a further reference chamber which is closable by way of a shut-off device or by way of a storage device. A control unit is provided by which the shut-off device or store control is closed or enabled, respectively, once a given pressure is reached in the test chamber or body in order to store a reference pressure value for pressure value difference forming means, to which also the actual pressure value from the test chamber or from the body is led. Thus storage means are provided for data corresponding to at least one DESIRED pressure or at least one DESIRED PRESSURE CURVE, with the pressure recording element and the storage means being connected to a comparator arrangement as difference forming means in order to compare the behaviour of the pressure in the test chamber or body. In lieu of providing a pressure difference sensor arrangement, it is possible for the pressure difference signal to be electronically formed whereby pressure values prevailing in the test chamber or body are tapped off at different points in time using the first pressure value as reference pressure value in comparing the second pressure value with the first pressure value and electronically generating a pressure difference value signal. Thus, in order to test at least one of tightness of a hollow body or a change in volume of the hollow body or volume thereof, the hollow body is exposed to one of a positive or negative differential pressure difference between an internal pressure of the hollow body and the pressure in the test chamber. For flexible bodies, as plastic bottles, there is applied an interior pressure greater than the external. The pressure prevailing in the test chamber or body is tapped off and a signal is generated in accordance with a difference of pressure. values between tapped off pressures at two subsequent points in time, with a determination of at least one of the tightness, change of volume or volume of the hollow body being determined from the generated signal. For volume testing it is advantageous to store a first pressure value from the reference chamber at a first time and to compare it, at a second point in time, with the pressure resulting from pressure equalization in reference chamber and test chamber or interior of the body. The pressure tapped off at the first of the points in time or signal generated in accordance with the tapped off pressure at the first point in time is stored as mentioned. The generated difference pressure signal may advantageously be compared with a predetermined value and a conclusion may be reached indicating a lack of tightness of the hollow body as the result of such comparison or deviation from a rated volume. Control means in accordance with the present invention include a means for outputting a start signal for the time control means once a preselected value is reached within reference chamber and/or the test chamber or the body so as to initiate a control of two subsequent points in time. The reference signal source may be adapted to output a reference signal varying in time. The method and apparatus of the present invention is extremely advantageously used for flexible hollow bodies such as coffee packages and especially for in-line testing of plastic bottles. As can readily be appreciated, since only one chamber, that is, a test chamber generally, is positively or negatively pressure loaded and since it is this one chamber from which the pressure measurements are tapped, the test chamber may well be the interior of the container itself in situations where open containers such as, for example, said plastic bottles are to be tested. More particularly, an apparatus may be provided for at least one of testing tightness of a hollow body and a detecting of a change in the volume and of detecting volume of the hollow body, especially plastic bottle, caused by pressure stresses applied to the walls of the hollow body wherein a pressure generating means applies a positive pressure to an interior of the hollow body relative to a pressure surrounding the exterior of the hollow body with pressure difference sensors being provided with two pressure difference inputs both connected to the interior of the hollow body, and with one of the inputs being connected to the hollow body by a shut-off valve means. A second of line from one of the pressure inputs to the shut-off valve means may directly act as pressure storage or further reference chamber. The hollow body is utilized as the test chamber, a pressure medium is introduced into the hollow body so as to apply a pressure to the hollow body different from an external pressure of the hollow body, with the hollow body being connected to a pressure difference sensor by first and second inputs, with a valve connecting the hollow body to the first input of the pressure difference sensor being closed so as to provide a reference pressure value for the pressure difference sensor, with the pressure of the hollow body then being detected over a period of time at the second input of the pressure difference sensor. The reference pressure and the detected pressure are compared to provide information on the tightness of the hollow body. The pressure in the hollow body may also be held constant over a given period of time by introducing further pressure medium or releasing pressure medium from the hollow body, with the amount of pressure medium introduced or removed from the hollow body over a given time period being evaluated to provide information as to the tightness of the hollow body. The above and other objects, features, and advantages of the present invention will become more apparent from the following description when taken in connection with the accompanying drawings. Fig. 1 is a functional block diagram of the fundamental structure of an apparatus. Fig. 2a is a graphical illustration of the internal pressure in the hollow body and the internal pressure in the test chamber over time, given a pressure difference between the test chamber and the interior of the hollow body which is directed towards the interior of the hollow body and given fully rigid and tight walls of the hollow body on the one hand, and body walls which are tight but yield under the applied pressure stresses; Fib. 2b is a graphical illustration similar to fig. 2a depicting different leakage rates of the hollow body; Fig. 3 shows, on the basis of the depiction in fig. 1, an apparatus in which the test chamber pressure is held constant and the controlled variable is evaluated; Fig. 4 shows, on the basis of the depiction in fig. 1, a preferred embodiment of the pressure-recording system in which the pressure is measured as pressure difference; Fig. 5 shows, on the basis of the depiction in fig. 1 or fig. 4, a preferred embodiment of the apparatus for applying pressure to the test chamber as well as a time control apparatus for controlling the time of the individual phases of the method; and Fig. 5a is a schematic view of yet another apparatus wherein a generated pressure signal difference, based on two different pressure values in a test chamber of the apparatus at two subsequent points in time, is electronically effected. Figs. 6 to 8 are schematic views of further embodiments wherein the container itself forms a test chamber. Referring now to the drawings wherein like reference numerals are used throughout the various view to designate like parts and, more particularly, to fig. 1, according to this figure, a hollow body 1 which is to be tested for tightness such as, for example, leaks, or to determine whether its volume changes as a result of pressure stress and elastic deformation of its walls is placed in a test chamber 3, for example, through an opening which is tightly closable by a lid 5. An internal pressure p il , which normally corresponds to the ambient pressure p u , exists in the interior of the hollow body 1. Once the test chamber 3 has been hermetically sealed, it is pressurized by connecting a source of pressure medium 7 to the test chamber 3. The pressure medium used is a gas, preferentially, air and, as a result, a positive or negative differential pressure is generated inside the test chamber 3, with the reference to the internal pressure p i1 inside the hollow chamber 1. The pressure inside the test chamber 3 is designated p 3 in fig. 1. Then the pressure system, consisting of the test chamber 3 and the hollow body 1 to be tested, is separated from the source of pressure medium 7 by means of, for example, a shut-off valve 9 and allowed to stand by itself. If the hollow body 1 is tight to the gas used and if its walls are so rigid that forces resulting from the pressure difference between p 3 and p i1 acting on the walls do not bring about any substantial deformations, then using a pressure sensor, which could be a mechanical/electrical converter, for example, a piezo-electric pressure sensor, as shown in diagrammatic form at 11 in fig. 1, an output signal s(p 3 ) is recorded qualitatively and depicted in fig. 2a. Fig. 2a presents a qualitative plot over time t of the pressure in the test chamber 3 corresponding to the signal s(p 3 ), and also of the internal pressure p i1 in the hollow body 1. Up to the time t 1 , for example, until the hollow body 1 is introduced into the test chamber 3 and the latter is tightly closed by means of the cover 5, p 3 and p i1 are identical to the ambient pressure p u . At time t 1 , the process of pressurizing the test chamber 3 by the pressure medium source 7 commences and the pressure in the chamber 3 rises. In the case mentioned above, in which the hollow body has rigid and tight walls, the internal pressure p i1 remains unaffected by the change in pressure in the test chamber 3. At time t 2 , the source 7 is separated from the test chamber 3 and in the present case the test chamber pressure p 3 (a) remains at least approximately constant as does the internal pressure p i1 (a) the hollow body 1. If the walls of the hollow body 1 are not absolutely rigid in the above mentioned sense but undergo deflection inwards or outwards at least at certain points and in accordance with the applied pressure difference Δp, which may be positive or negative, then when the differential pressure is directed towards the interior of the hollow body, the qualitative curves p 3 (b) or p i1 (b) indicated by the dash-dot lines are obtained. Similar circumstances prevail when the differential pressure is directed towards the test chamber 3. As can be seen from these qualitative curves, after a shorter or longer period of time, both pressures tend asymptotically towards a different constant limit value. Fig. 2b is a plot, similar to that shown in fig. 2a, of the conditions prevailing when leaks of various size exist in the hollow body 1. Given a relatively small leak rate, the internal pressure of the hollow body 1 and the pressure between the test chamber 3 and the hollow body 1 equalize at a relatively slow rate in accordance with the qualitative curves p(c), while for larger leaks the equalization takes place at an increasingly fast rate, as shown, for example, by the curves p(d). If a DESIRED curve p 3 , for example, as shown by p 3 (b), is known to apply in general to intact, tight hollow bodies 1, taking account also of any change in volume in the hollow body 1 caused by the differential pressure stress, then at the output side of the sensor 11 it is possible to judge, by comparing the ACTUAL curve with such DESIRED curve, to what extent a tested hollow body is tight or not, or whether it should be rejected or not. For this purpose, in accordance with fig. 1, the pressure p 3 is measured, for example, with reference to the ambient atmosphere having pressure p u and, advantageously and as will be described further below, the difference between pressure p 3 and a given reference pressure is measured. As shown in fig. 3, the pressure in the test chamber 3 is held constant and the amount of pressure medium or gas added to or removed from the test chamber per unit of time, or integrated over a given period of time, is recorded as the measured variable. As shown in fig. 3, after the hollow body 1 to be tested is introduced into the test chamber 3, which is then tightly closed, the chamber is pressurized by a source of pressure medium 7, which may be air, or in turn the chamber may be evacuated, and the internal pressure of the test chamber 3 is recorded as the controlled variable W using a pressure sensor 11. The controlled variable W is compared at a differential measuring unit 13 with the reference pressure X or with a signal corresponding to the reference pressure and the resulting control difference Δ is applied to the control input S 7 control input of the source 7. Using the latter as the regulating element, the pressure in the test chamber 3 is adjusted to the DESIRED value X which has been set at a preselector device 15. The volume of medium per unit time to be supplied by the source 7, which is the regulating element for test chamber 3, is measured by a flow sensor 17 as a signal S ΔV / Dt which is then integrated for further evaluation, for example, over a given period of time. The curves obtained for the signal S ΔV / Δt are those shown in figs. 2a and 2b. Fig. 4 shows a preferred embodiment of the method of measuring the pressure in the test chamber 3 as depicted in fig. in fig. 1. During the pressure build-up phase between times t 1 and t 2 , the test chamber is connected via a line 19 with one input E 19 of a pressure value difference sensor or unit 21, for example, a piezo-electric sensor. Via a second line 23 fittet with a shut-off valve 25, the test chamber 3 is further connected with a second input E 23 connected with a second input of the pressure difference sensor 21. At time t R as shown in fig. 2b, the shut-off valve 25 is closed so that the pressure prevailing at that time in the test chamber 3 remains built-up in the section of line 23a between shut-off valve 25 and the second input E 23 which is used as the reference pressure system. This pressure in the connecting line 23a acts as the reference pressure on the pressure difference sensor 21 since the line 19 remains open in the following measurement phase for t > t 2 , a pressure difference is measured at the pressure difference sensor 21 relative to the pressure prevailing in the test chamber at the time t R . As can be seen from fig. 2b, the time t R is adjusted on a case by case basis to give optimum measurement resolution, as indicated by t R' , t R" and resulting reference pressures p R , p R' and p R" . Proceeding from the diagram in fig. 4, fig. 5 presents an inventive embodiment of the means of pressurizing the test chamber 3. For this purpose, a test gas source such as, for example, a pump 7a, is connected via a shut-off valve 27 with a reference volume in a reference chamber 29. The reference chamber 29 is connected via a further shut-off valve 31 with the test chamber 3. Using source 7a and with valve 27 initially open and valve 31 shut, the reference chamber 29 is filled with a test gas and a pressure sensor 33 is used to measure the pressure in the reference chamber 29. Once the pressure measured by the pressure sensor 33 attains the reference pressure adjusted at a reference signal source 35, the valve 27 is closed. Next, valve 31 is opened, thus forming a communicating system between the test chamber 3 and the reference chamber 29 and the test gas pressure is equalized according to the volumes in the reference chamber 29 and the test chamber 3. Following an equalization phase corresponding to the time section t 1 , t 2 in fig. 2b, the course of the pressure difference is measured as a volume indication of body 1, using the pressure difference sensor 21 as described on the basis of fig. 4, or at a given measuring time t m , with any differences between a DESIRED pressure difference and an ACTUAL pressure difference being recorded as shown in fig. 2b. As further shown in fig. 5 the output of the pressure difference sensor 21 is fed, for example, to a comparator 37 to which, at a second input, a standard curve is supplied from a storage and output device 3, for example, a computer. The deviations of the instantaneous test result from a given DESIRED result can be delivered at any point in time at the output of the differentiator 37 and, on the basis of these deviations a decision can be made regarding the condition of the hollow body 1 that is being tested. Instead of comparing the time curves, it is also possible at any given point in time corresponding to t m to compare the ACTUAL pressure difference at the output of the pressure difference sensor 21 with DESIRED values stored in the unit 39. For this purpose, a conventional timer unit, as shown in diagrammatic form 41, is provided. When the given pressure is attained in the reference chamber 29, the timer is activated and, in accordance with preselected time intervals T, it operates the valves 31, 25 and can also set the DESIRED value at S 39 . According to this procedure, and using the arrangement described, it is possible to detect leaks or the volume reliably and rapidly over an extremely broad range. Thereby, as was explained on the basis of fig. 2a, it is possible to detect deviations in the shape characteristics of the hollow bodies from the anticipated shape characteristics, as may happen, for example, if the wall sections are unacceptably rigid or unacceptably elastic. In the embodiments described hereinabove in connection with figs. 4 and 5, a differential sensor 21 was employed to hold a pressure value prevailing in the test chamber 3 at a first point in time occurring, for example, upon a closing of the shut-off valve 25 and thus storing the prevailing pressure value in a line section 23a of a second or connecting line 23 at one input of the differential pressure sensor 21. The pressure value prevailing at the first point in time, that is, when the shut-off valve 25 is closed, was then compared with a pressure value prevailing in the test chamber 3 at a subsequent point in time, that is, a point in time subsequent to the storing or holding of the prevailing pressure at the line section 23a. Consequently, with the above described of figs. 4 and 5, one pressure value at a first point in time and prevailing in the test chamber is taken as a reference pressure value which is compared with a second pressure value prevailing in the test chamber 3, which second pressure value prevails in the test chamber 3 at some subsequent point in time. The above described measuring technique or concept may be carried out electronically rather than by utilizing a pressure difference sensor as in the embodiments 4 and 5, with the advantage of faster test cycles as no flow and transient phases are encountered for signal transmission and storage. More particularly, as shown in fig. 5a, prevailing pressure in a test chamber 3 may be tapped directly or by a connecting line 23 arranged between the test chamber 3 and a pressure/electrical signal transducer 50 which may, for example, be an absolute pressure electrical signal transducer such as a piezo-transducer working against a reference force F. An electrical output of the transducer 50 representing the pressure prevailing in the test chamber 3 is led, as schematically shown, by way of a switch W 1 and a switch W 2 to a first storage area I of a conventional electronic storage unit 52 once the timer unit 41 activates the switch W 1 at a first point in time. The timer unit 41 may then subsequently, after a predetermined time interval, activate the switch W 1 at a point in time later than the first point of time so that the output signal of the transducer 50 is led to a second area II of the storage unit 52 upon an activation of the switch W 2 by an output signal of a conventional time lag unit 54 which may be formed as a separate component from or an integral portion of the timer unit 41. Upon storage of the electric data in the storage areas I and II of the storage unit 52 relating to the pressure prevailing in the test chamber 3 at a first point in time and to the pressure prevailing in the test chamber 3 at a second point in time, the data is output from the storage areas I, II and supplied to a conventional difference forming unit 56, wherein a signal representing the pressure differential of the two prevailing pressure values is formed and led to a conventional differentiator 37 and processed in the manner described hereinabove in connection with the embodiment of fig. 5. In all other respects, the pressure difference signal, as described hereinabove in connection with figs. 4 and 5, is processed in the same manner as the pressure difference signal from the pressure difference sensor, with the difference residing in the formation of the pressure difference signal in the embodiment of fig. 5a occurring electronically. In the embodiment of fig. 5a, a pressure value prevailing in the test chamber 3 at one point in time is the reference pressure for forming a pressure difference with respect to a pressure value prevailing in the test chamber 3 but taken at a subsequent period of time. Figs. 6 to 8 provide examples of highly advantageous embodiments respectively employing the principles of the embodiments described hereinabove in connection with figs. 4 and 5; however, the hollow body 1, fashioned as an open container such as, for example, a bottle of a bottle stream, functions as the test chamber 3 of the embodiments of figs. 4 and 5. More particularly, as shown in fig. 6, the hollow body 1 is sealed by a suitable conventional plug or latch type sealing adaptor 58 and, during a pressure build-up phase between t 1 and t 2 , the hollow body 1 is connected through the line 19 with one input E 19 of the pressure difference sensor 21. The second line 23, provided with the shut-off valve 25, connects the sealed hollow body with the second input E 23 of the pressure difference sensor 21. At the time t R , as shown in fig. 2b, the shut-off valve 25 is closed so that the pressure prevailing at that time in the hollow body 1 remains built-up in the section of line 23a between the shut-off valve 25 and the second input E 23 which is used as the reference pressure system. The testing is carried out in the same manner as described hereinabove in connection with the embodiment of fig. 4. As shown in fig. 7, a test gas source such as, for example, pump 7a is connected by way of a shut-off valve 27 with a reference volume in a reference chamber 29. The reference chamber 29 is connected by way of a further shut-off valve 31 with the hollow body 1 sealed by the sealing adaptor 58. With the valve 27 being in an initially open position and the valve 31 shut, the source 7a fills the reference chamber with a test gas and the pressure sensor 33 is used to measure the pressure in the reference chamber 29. Once the pressure measured by the pressure sensor 33 attains the reference pressure adjusted at the reference signal source 35, the valve 27 is closed and the valve 31 is opened thus forming a communication system between the hollow body 1 and the reference chamber 29, with the test gas pressure being equalized in accordance with the volumes in the reference chamber 29 and the hollow body 1. Following an equalization phase corresponding to the time frame t 1 , t 2 in fig. 2b, the course of the pressure difference is measured using the pressure difference sensor 21 as described hereinabove in connection with fig. 4, or at a given measuring time t m , with any differences between a DESIRED pressure difference and an ACTUAL pressure difference being recorded as shown in fig. 2b. In all other respects the embodiment of fig. 7 functions in the same manner as indicated hereinabove in connection with fig. 5. In the embodiment of fig. 8, prevailing pressure in the hollow body 1 may be tapped by the connecting line 23 arranged between the hollow body 1 and a pressure/electrical signal transducer 50 which may, for example, be an absolute pressure/electric signal transducer such as a piezo-transducer working against a reference force F. The electrical output of the transducer 50 representing the pressure prevailing in the hollow body 1 is led by way of the switch W 1 and the switch W 2 to a first storage area I of a conventional electronic storage unit 52 once the timer unit 41 activates the switch W 1 at a first point in time. The timer unit 41, after a predetermined time interval, subsequently activates the switch W 1 at a point in time later than the first point in time so that the output signal of the transducer 50 is led to the secondary II of the storage unit 52 upon an activation of the switch W 2 by an output signal of a conventional time lag unit 54 formed either as a separate component from or an integral portion of the timer unit 41. The data is processed and the testing proceeds in the same manner as described hereinabove in connection with fig. 5a.

Claims: A method for testing hollow bodies, comprising loading the interior of a body (1) or a test chamber (3) containing said body with a pressure, measuring a first pressure in said body or in said test chamber at a first point of time and electrically storing a first electrical signal representing said first pressure measured, generating and storing electrically a difference signal from said first electric signal stored and a second electric signal representing a second pressure in said body or in said chamber at a second point in time and evaluating in dependency of said difference signal, whether said hollow body is leaky or has an undesired volume behavior, characterized by in-line testing said bodies and performing said storing and generating said difference signal once a given pressure in said body or said test chamber has been reached, storing said difference signal for said evaluating electronically in an electronic storage unit with storage areas. Apparatus for testing hollow bodies, comprising means for loading said hollow bodies or a test chamber (3) for said hollow bodies with a pressure; pressure-measuring means (50) connected to said body or connected to said test chamber and generating an electric output signal; a timing unit initiating at a first point in time storing of a signal dependent on said output signal at said first point in time in an electric storage and initiating at a second point in time storing of the difference of said stored signal and said dependent signal of said output signal prevailing at said second point in time in an electric storage, characterized by said apparatus being an in-line testing apparatus and comprising a pressure-measuring means enabling said timing unit once a predetermined pressure has been reached, said electric storage for said difference signal being an electronic storage unit with storage areas.

Inventors: LEHMANN MARTIN, LEHMANN, MARTIN
Applicants: LEHMANN MARTIN, LEHMANN, MARTIN
Application year: 1991
Main classification: G01F17
IPC codes: B07C5, G01F17, G01M3