METHOD FOR MEASURING ABSORBENT HYGIENE PRODUCTS

Abstract

A method for measuring absorbent hygiene products comprises placing absorbent bodies on a web and moving the web through at least one microwave resonator. Values of a shift in a resonance frequency and a spreading of the resonance frequency are measured using the at least one microwave resonator to continuously determine the shift in the resonance frequency and the spreading of the resonance frequency. At least one of moisture and density of the plurality of absorbent bodies is determined based on the measured values of the shift in the resonance frequency and a spreading of the resonance frequency. Empty values for each of the measured values of the shift in the resonance frequency and the spreading of the resonance frequency are determined and subtracted from the measured values of the shift in the resonance frequency and the spreading of the resonance frequency to evaluate the measured values.

Claims

1-11. (canceled)

12. A method for measuring absorbent hygiene products, the method comprising: placing a plurality of absorbent bodies on a continuous web, wherein the absorbent bodies are spaced from each other; moving the continuous web through at least one microwave resonator; measuring values of a shift in a resonance frequency and a spreading of the resonance frequency using the at least one microwave resonator to continuously determine the shift in the resonance frequency and the spreading of the resonance frequency; determining at least one of moisture and density of the plurality of absorbent bodies based on the measured values of the shift in the resonance frequency and a spreading of the resonance frequency; determining empty values for each of the measured values of the shift in the resonance frequency and the spreading of the resonance frequency by continuously determining a local minimum value and averaging the local minimum value with a plurality of past values of local minima; and subtracting the empty values from the measured values of the shift in the resonance frequency and the spreading of the resonance frequency to evaluate the measured values of the shift in the resonance frequency and the spreading of the resonance frequency.

13. The method according to claim 12, further comprising determining a position of the local minimum for one of measured values of the shift in the resonance frequency and the spreading of the resonance frequency, and determining a value of the local minimum in the determined position the other of the measured values of the shift in the resonance frequency and the spreading of the resonance frequency.

14. The method according to claim 12, wherein the local minimum value is determined for each of the measured values of the shift in the resonance frequency and the spreading of the resonance frequency.

15. The method according to claim 12, wherein a predetermined number of past local minima are averaged.

16. The method according to claim 12, further comprising at least two microwave resonators positioned at an offset from each other in a transverse and longitudinal direction relative to a direction of transport of the continuous web and configured to measure the continuous web over its width.

17. The method according to claim 16, wherein each of the at least two microwave resonators averages its measured values of the shift in the resonance frequency and the spreading of the resonance frequency in the transverse direction and corrects its averaged measured values of the shift in the resonance frequency and the spreading of the resonance frequency by the offset of the at least two microwave resonators relative to each other in the direction of transport.

18. The method according to claim 17, wherein each of the at least two microwave resonators comprises a measuring range with a homogeneous field distribution, and wherein the at least two microwave resonators are positioned transverse to the transport direction such that the continuous web is covered by measuring ranges with a homogeneous field distribution.

19. The method according to claim 12, wherein the density of an absorbent body is determined by a summation of a measured shift in the resonance frequency and a measured spreading of the resonance frequency.

20. The method according to claim 12, wherein the moisture of an absorbent body is determined by a summation of a measured shift in the resonance frequency and a measured spreading of the resonance frequency.

21. The method according to claim 19, wherein the summed values of the measured shift in the resonance frequency and a measured spreading of the resonance frequency are divided by a number of summands.

22. The method according to claim 20, wherein the summed values of the measured shift in the resonance frequency and a measured spreading of the resonance frequency are divided by a number of summands.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0013] The method according to the invention will be further explained below with reference to an exemplary embodiment. In the following:

[0014] FIG. 1 shows the basic design of a diaper machine and possible positions of a microwave resonator;

[0015] FIG. 2 shows signals of a diaper sheet where the spacing of the diaper cores is less than a sensor diameter;

[0016] FIG. 3 shows signals of a diaper sheet where the spacing of the diaper cores is greater than the diaper diameter;

[0017] FIG. 4 shows a schematic view of the field distribution in a fork resonator in a longitudinal direction; and

[0018] FIG. 5 shows an arrangement of two forked sensors for a web-shaped measured material.

DETAILED DESCRIPTION OF THE INVENTION

[0019] FIG. 1 shows a schematic view of the overall design of a diaper machine 10. The machine 10 possesses a continuous web 12 consisting of a polyethylene outer sleeve that continuously runs through the machine at a high speed in order to produce a diaper. At periodic intervals, diaper cores are applied in a section 14 of the machine. The applied diaper cores consist of absorbent pads and are positioned on the web 12 that is passing through. The schematically portrayed detection apparatuses 18 and 20 are conventionally operating detection apparatuses that for example optically monitor the web and the applied diaper core. A microwave resonator 22, 24, 26 is positioned along the production process in order to repeatedly measure mass and moisture of the diapers and the web 12. Depending on the position of the microwave resonator along the web 12, the microwave measured values for the mass and moisture can be measured and monitored in various stages of production.

[0020] A single-use or disposable diaper consists of an outer sleeve of polyethylene (PE) and an absorbent body that generally consists of a cellulose material which is enriched with a super absorber (polymer salts). The amount of liquid can be bound by the absorbent body several times its own volume, and the liquid can be held even upon exertion of pressure.

[0021] In the production of diapers, an endless web 12 of the polyethylene outer sleeve is provided at periodic intervals in the diaper machine 10 with a permeable cover layer with the absorbent bodies. In this case, the absorbent bodies consist of a mixture of cellulose and powdered super absorber (SAP=superabsorbent polymer material).

[0022] For quality control in production, it is desirable to measure the overall mass and/or density profile of the diaper cores using microwave resonators. A series of suggestions for positioning the microwave resonators in a diaper machine is known from WO 2014/170796 A1. An approach for evaluating the measured values in order to achieve reliable and precise results is not known.

[0023] With a microwave resonator, a shift in the resonance frequency A and a spreading of the resonance curve B is measured as a consequence of the dielectric properties of the specimen to be investigated. The measured values are formed as a difference between the values of the filled and empty resonator. The resonance frequency shift A in Hz is:

A=f.sub.0f.sub.m,

wherein f.sub.0 indicates the resonance frequency of the empty resonator in Hz, and f.sub.m indicates the resonance frequency of the filled resonator in Hz. The increase in the peak width at half maximum of the resonance B in Hz is employed for the spreading of the resonance curve. The following applies:

B=w.sub.mw.sub.0,

wherein w.sub.0 designates the peak width at half maximum of the resonance of the empty resonator in Hz, and w.sub.m designates the peak width at half maximum of the resonance of the filled resonator in Hz.

[0024] From the above approach, it is clear that information on the resonance parameters of the empty resonator belongs to each measurement. The empty resonance values change as the temperature changes and as the resonator becomes soiled. In order to suppress the influence of the empty resonance values on the measured values, the following measures are taken in practice: [0025] In laboratory measurements, there is a measurement of the current empty resonance values for each recorded measured value. [0026] In process measurements in which the empty resonance values can only be measured rarely, the sensor is encapsulated and regulated to a constant temperature. In addition, the sensor is regularly cleaned with compressed air.

[0027] In the case of portioned units that are embedded in an endless, non-metal support material, the case is described as a procedure in DE 10 2009 004 457 A1 in which the distances of the portioned units in the support material is greater than the diameter of the employed microwave resonator. This ensures that the sensor only detects the support material between the portioned units. The known evaluation requires only the support material, i.e., the web without the portioned unit, to be located within the measuring range at periodic intervals. This means that the spacing of the portioned unit must be greater than the employed measuring field.

[0028] When used in the diaper machine, the spacing between two diaper cores is frequently smaller than the diameter of the sensor. Accordingly, at no time is only the support material by itself located in the sensor. This means that the sensor always contains measuring signals from the diaper package to a certain extent. Nonetheless, it was found that periodic signal minima arise between the cores along the web when diaper cores are used. The invention is based on the insight that when detecting these minima, the signals can be calculated based on the difference between the measured values A and B and the measured values of the respective local minima A.sub.min and B.sub.min instead of an empty adjustment. It is accordingly possible to compensate for all temperature influences on the sensor as well as signal fluctuations from soiling without an empty adjustment (as is known from the prior art).

[0029] The evaluation algorithm according to the invention for the microwave resonators is especially suitable for spacings between diaper cores that are less than the measuring range of the microwave resonators. Of course, the evaluation according to the invention using the local minima values and their moving average can also be used when the spacings between the diaper cores is greater than the employed measuring field due to a particular configuration of the diaper machine. The method according to the invention can accordingly be used universally independent of the spacing of the diaper cores.

[0030] Another advantage when using minimum detection is that, in the known evaluation method according to the prior art, the diaper sheet must be moved into a predefined position relative to the sensor when the measuring process starts i.e., the region between two diaper cores must for example be located in the sensor. In this position, the first empty adjustment is performed that is then the basis for the following periodic empty adjustments. This procedure is discarded when using minimum detection since sensor empty adjustment is not needed when using this method.

[0031] The method that is known from EP 1 467 191 A1 for measuring capsules/tablets also always requires the conveyor belt to be without capsules or tablets to measure an empty adjustment between two tablets to be measured.

[0032] FIG. 3 shows the signal characteristic of the resonance frequency shift A in which the distance between two diaper cores in the transport direction is greater than the extent of the measuring range in the transport direction. In this measuring situation, minimum values 28, 30, 32, 34 occur at periodic intervals between the diaper cores in which only the web 12 is located within the measuring range. It is clearly discernible that the measured values for a configuration in which the web passes through the microwave resonator without a diaper core are nearly constant and accordingly change appropriately for an empty adjustment of the signal values.

[0033] The behavior of the measured variables, in particular in the minimum range, changes significantly in FIG. 2. In this case, the distance between two diaper cores is less than the measuring range of a microwave resonator. In FIG. 2, it is discernible that the local minimum values 36 to 48 fluctuate significantly from each other. Accordingly, for example the local minimum values 40 and 42 differ from each other nearly by 1 MHz. The extent of the fluctuation becomes clear when it is considered here that the fluctuation is nearly 100% of the local minimum 40.

[0034] The minimum values portrayed in FIG. 2 fluctuate so strongly due to the measuring setup that a reliable evaluation by a simple empty adjustment, or respectively subtracting the signal values, only yields a very imprecise measured value. A measurement of the minima at a fixed machine cycle is also not possible.

[0035] In order to minimize the influence of the individually occurring variations in the minimum values 36-48, it is proposed according to the invention to form a moving average over the signal minima and use them to form the difference. A moving average A.sub.min.sub._.sub.AV is therefore used to form the difference while forming a signal. The moving average is:

A.sub.min.sub._.sub.AV=(A.sub.min.sub._.sub.1+A.sub.min.sub._.sub.2+ . . . +A.sub.min.sub._.sub.N)/N

wherein {A.sub.min.sub._.sub.i} designates the last local minima for the resonance frequency shift A. The moving average formed in this manner is used to form the difference so that the following value is used as measured variable A:

A=A.sub.coreA.sub.min.sub._.sub.AV,

wherein A.sub.core is the measured A value for the diaper core. The same procedure is used for the B values.

[0036] In addition to the above-described arithmetic averaging for the A values, other types of averaging can also be used. In particular, it may also be of interest to use weighted averages where measured values that lie further in the past are given less weight in the measurement than minimum values just recorded.

[0037] The measured variables A, B determined with the assistance of the microwave resonators can be evaluated in different ways. Since super absorbers are used as a very hydrophilic material in the production of diapers, in particular the determination of the moisture, or respectively a moisture profile, is also particularly relevant for the diaper core. It is also relevant to determine the overall mass and a density profile for the diapers from the measured variables A, B.

[0038] The overall mass of the diaper cores is obtained by adding or integrating the measuring signals A, B over the respective diaper core. If the integral value is divided by the number of individual measurements M, the mass of the diaper core can thus be determined using the following calibration equation:

Mass.sub.diapercore=a.sub.1.Math.Int(A)/M+a.sub.2.Math.Int(B)/M+a.sub.3,

where the function Int stands for the integral or the sum of the values, and M describes the number of the measurement over the diaper core. The parameters a.sub.1, a.sub.2 and a.sub.3 can be established when calibrating for the subsequent procedure. The moisture contained in the diaper can correspondingly be obtained by evaluating the moisture values with B/A. The parameters a.sub.1, a.sub.2, a.sub.3 are dependent on the length of the diaper core, but independent of the diaper speed, i.e., the production speed.

[0039] In determining the overall mass of the diaper cores, it is in principle also possible to determine the mass depending on the integral of the microwave measured values. This is expressed as follows:

Mass=a.sub.1.Math.Int(A)+a.sub.2.Math.Int(B)+a.sub.3,

where a.sub.1, a.sub.2 and a.sub.3 are parameters that are determined by a calibration. It is interesting in this case that the calibration can only be performed for one production speed since the value of the integral depends on the speed. It is theoretically possible to include the speed with which the diaper is moved through the sensor in the calibration equation.

[0040] In practice, it has been revealed that the approach of considering the average of the integrals (Int(A)/M, Int(B)/M) yields more precise results since the average of the integrals only depends on the length of the diaper cores which fluctuates very little.

[0041] Another feature of measuring with microwave resonators for absorbent hygiene products is that the web-shaped material may possess a large width in certain circumstances. Preferably, wide fork-type sensors are used to measure web-shaped material as for example known in the textile field from EP 1 316 630 B1. These fork-type sensors basically consist of a cylinder divided in two along its longitudinal axis through which the web-shaped material is guided. Fork-type sensors possess great field homogeneity in the direction of the cylinder, i.e., perpendicular to the transport direction of the web to be measured. It is therefore possible to precisely measure density and mass profiles in the direction of movement, wherein the sensor measures a strip transverse to the direction of movement in an integrating manner.

[0042] To achieve the aforementioned field homogeneity, the so-called basic mode E010 is operated in a fork-type sensor. If d is designated as the diameter of a cylindrical fork-type sensor and l as its length, it accordingly holds true for d/l.fwdarw.0 that the resonance frequency f.sub.0 of mode E011 increasingly approaches the basic mode E010. Given this approach, the basic mode is no longer useable for measuring in practice since effects and influences from the E011 mode which is also instigated are always manifested. Accordingly, the length of fork-type sensors is limited for physical reasons and cannot be scaled or lengthened arbitrarily. For frequencies of 2-3 GHz for example, fork-type sensors can be used at most up to a length of about 20 cm. Such a measuring width may be too small for hygiene products such as diapers for adults.

[0043] FIG. 4 shows the field strength distribution in a fork-type sensor in the direction of the cylinder axis. Three zones can be distinguished:

I. A field strength range outside of the resonance space in which the field strength decreases exponentially.
II. An inhomogeneous field strength range at the floor and cover of the cylinder structure, and
III. a homogeneous field strength range that is particularly well-suited for measuring mass and density.

[0044] An offset arrangement of the fork resonators 50, 52 portrayed in FIG. 5 makes it possible to detect the entire web-shaped measured material 54 with the homogeneous field ranges III of the two fork resonators 50, 52. The homogeneous measuring ranges III of the fork resonators 50, 52 are offset relative to each other in the transverse direction Q and in the transport direction T.

The offset V in the transport direction arising between the fork resonators 50 and 52 can be taken into consideration by a temporal offset when evaluating the measuring signals.

[0045] When using the sensors 50, 52, the mass per length unit is determined by the following four measured values:

A.sub.1,B.sub.1,A.sub.2,B.sub.2,

wherein A designates the resonance frequency shift and B the spread of the resonance, and the indices refer to the resonators 50 and 52.

[0046] The mass per length unit m in for example g/cm can be determined by the following relationship:

m=a.sub.1.Math.A.sub.1+a.sub.2.Math.A.sub.2+a.sub.3.Math.B.sub.1+a.sub.4.Math.B.sub.2+a.sub.5,

where a.sub.i designates the calibration coefficients.

[0047] At the same time, the moisture of the measured material u can be measured in %. The quotient of the microwave measured values is used for density-independent moisture measurement. As is usual, the following is defined: =B/A or =arctan(B/A). The moisture of the measured material u in % is determined using the microwave moisture values from the two resonators. Let .sub.1=arctan(B.sub.1/A.sub.1) and .sub.2=arctan(B.sub.2/A.sub.2) for the microwave resonators 50, 52. The determined moisture value u is then:

u=b.sub.1.Math..sub.1+b.sub.2.Math..sub.2+b.sub.3,

where b.sub.i designates the calibration coefficients.

[0048] Due to production tolerances of the fork-type sensors, the measurements in both fork resonators yield slightly different measured values for measured variables A and B for the same product. By test measurements of a homogeneous material, the two measured variables of the resonators 50, 52 can be set in relation to each other. When using a homogeneous material, an offset between the resonators can of course be dispensed with. One approach for evaluating measured signals can therefore be:

A.sub.1=c.sub.1.Math.A.sub.2,

B.sub.1=c.sub.2.Math.B.sub.2,

where c.sub.1 and c.sub.2 are predetermined coefficients. The advantage of previously setting the measured variables of the two microwave resonators in a constant relationship c.sub.1, c.sub.2 with each other is that fewer calibration coefficients a.sub.i must be determined for the mass and moisture values.

[0049] In principle, the above-described arrangement of the microwave resonators 50, 52 can also be expanded to more than two microwave resonators in order to measure the web to be measured with a field distribution as homogeneous as possible.