Vibronic Sensor

Abstract

An apparatus for determining and/or monitoring at least one process variable of a medium in a container, comprising at least an oscillatable unit having at least one membrane, and at least one oscillatory element, a driving/receiving unit embodied to excite the mechanically oscillatable unit by means of an electrical, exciter signal of adjustable excitation frequency to execute oscillations in an oscillation mode corresponding to the excitation frequency and to receive mechanical oscillations from the oscillatable unit and to convert such into an electrical received signal, and an electronics unit embodied, to produce the exciter signal, and to ascertain from the received signal the at least one process variable. The membrane is connected with the driving/receiving unit. The oscillatory element has the shape of an oscillatory rod, on which a paddle is terminally formed, and the oscillatory element is secured on the membrane in an end region remote from the paddle. Mass distribution, stiffness and/or geometry of the oscillatable unit is/are selected in such a manner that at least one of the oscillation modes of the oscillatable unit higher in reference to the oscillation mode corresponding to the excitation frequency lies in the range between two neighboring whole-numbered multiples of the excitation frequency.

Claims

1-14. (canceled)

15. An apparatus for determining and/or monitoring at least one process variable of a medium in a container, comprising: a mechanically oscillatable unit having at least one membrane and at least one oscillatory element; a driving/receiving unit, which is embodied to excite said mechanically oscillatable unit by means of an electrical, exciter signal of adjustable excitation frequency to execute oscillations in an oscillation mode corresponding to the excitation frequency and to receive mechanical oscillations from said mechanically oscillatable unit and to convert such into an electrical received signal; and an electronics unit, which is embodied, based on the received signal, to produce the exciter signal, and to ascertain from the received signal the at least one process variable, wherein: said at least one membrane is connected with said driving/receiving unit; said at least one oscillatory element has the shape of an oscillatory rod, on which a paddle is terminally formed, said at least one oscillatory element is secured on said at least one membrane in an end region remote from said paddle; and mass distribution, stiffness and/or geometry of said at least one oscillatable unit is/are selected in such a manner that at least one of the oscillation modes of said at least one oscillatable unit higher in reference to the oscillatable mode corresponding to the excitation frequency lies in the range between two neighboring whole-numbered multiples of the excitation frequency.

16. The apparatus as claimed in claim 15, wherein: said oscillatable unit is an oscillatory fork.

17. The apparatus as claimed in claim 15, wherein: said paddle is composed of a predeterminable material with a density (ρ), a predeterminable area (A.sub.P) and a predeterminable thickness (d), and the product of thickness (d) and density (ρ) is as small as possible, and the area (A.sub.P) of the paddle is as large as possible.

18. The apparatus as claimed in claim 17, wherein: the area (A.sub.P) of said paddle and/or of said oscillatory rod (A.sub.S) is/are curved.

19. The apparatus as claimed in claim 15, wherein: edges of said paddle are rounded.

20. The apparatus as claimed in claim 17, wherein: the width of said paddle (b) is greatest in the middle region with reference to the longitudinal axis (L) parallel to said oscillatory rod; and said paddle in the end region remote from said membrane slopes at an angle between 20° and 55° to the longitudinal axis of said paddle.

21. The apparatus as claimed in claim 19, wherein: said paddle has a pointed end.

22. The apparatus as claimed in claim 20, wherein: said oscillatory rod has a round cross sectional area perpendicular to the longitudinal axis (L).

23. The apparatus as claimed in claim 17, wherein: the thickness of said paddle in the end region is less than in the middle region.

24. The apparatus as claimed in claim 15, wherein: the at least one process variable is a predetermined fill level of the medium, or the density of the medium or the viscosity of the medium.

25. The apparatus as claimed in claim 15, wherein: said oscillatable unit is composed of a metal, a ceramic or a synthetic material.

26. A method for manufacturing an apparatus, comprising a mechanically oscillatable unit having at least one membrane, and at least one oscillatory element; a driving/receiving unit; and an electronics unit, the method comprising the step of: varying the mass distribution, stiffness and/or geometry of the oscillatable unit for adjusting the position of the at least one higher oscillation mode of the mechanically oscillatable unit, so that the higher oscillatory mode lies in the range between two neighboring whole-numbered multiples of the excitation frequency.

27. The method as claimed in claim 26, wherein: for adjusting the position of the first higher oscillatory mode, the mass distribution in the middle region of the paddle is varied.

28. The method as claimed in claim 26, wherein: for adjusting the position of a higher oscillatory mode, especially the second higher oscillatory mode, the stiffness in the region of the membrane and the connection between membrane and oscillatory rod is varied.

Description

[0027] The invention as well as advantageous embodiments thereof will now be described in greater detail based on the appended drawing, the figures of which show as follows:

[0028] FIG. 1 a schematic view of a vibronic sensor of the state of the art,

[0029] FIG. 2 a schematic view (a) of an oscillatory fork as well as (b) the movements of an oscillatory fork in the fundamental oscillation mode as well as in the first two excited oscillation modes.

[0030] FIG. 3(a) the oscillation spectrum of the oscillatory fork of a LIQUIPHANT field device in comparison with the oscillation spectrum of an oscillatory fork of the invention, and (b) the associated acoustic spectra.

[0031] FIG. 4a-b a comparison of the geometries of the oscillatory fork of a LIQUIPHANT field device and an oscillatory fork of the invention belonging to the spectra in FIG. 3

[0032] FIG. 5(a) a side view of the oscillatory fork of the invention of FIG. 4, (b) a second variant of an oscillatory fork of the invention with a paddle rounded in the end region, and (c) a third variant of an oscillatory fork of the invention with a paddle having a pointed end.

[0033] FIG. 1 shows a vibronic sensor 1. An oscillatable unit 4 in the form of an oscillatory fork extends partially into a medium 2 located in a container 3. Since this variant of the oscillatable unit is applied most frequently, the entire following description concerns, without limitation, an oscillatory fork.

[0034] The oscillatory fork is excited to execute mechanical oscillations by means of the electromechanical transducer unit 5, which is supplied with the exciter signal. The electromechanical transducer unit 5 can be, for example, a piezoelectric stack- or a bimorph drive. It is understood, however, that also other embodiments of a vibronic sensor fall within the scope of the invention. Furthermore, an electronics unit 6 is shown, by means of which the signal evaluation and/or supply of the exciter signal occurs.

[0035] FIG. 2a shows schematically an oscillatory fork, such as applied for the LIQUIPHANT field device. Shown is the membrane 7, and the oscillatory element 8 connected therewith. The oscillatory element includes two oscillatory rods 9, on the end of each of which a paddle 10 is formed. In operation, the oscillatory fork 4 executes oscillatory movements corresponding to the oscillatory mode, with which it is excited. How these movements look is shown schematically in FIG. 2b. Shown there is an oscillatory fork 4 turned by 90° relative to FIG. 2a. The arrows indicate the essential movement directions of the oscillatory fork 4 for the fundamental oscillation mode A, the first higher oscillatory mode B and the second higher oscillatory mode C. Each of the two oscillatory rods 9 behaves essentially as the bending oscillator mentioned in the introduction of the description. In the fundamental oscillation mode, the two oscillatory rods 9 oscillate with phase opposite to one another.

[0036] In FIG. 3a), finally, two oscillation spectra are shown, one for a conventional oscillatory fork in the LIQUIPHANT field device, and the second for an oscillatory fork of the invention. Both curves are normalized to whole-numbered multiples of the fundamental frequency, which corresponds to the fundamental oscillation mode. The dashed line is for the oscillation spectrum of the oscillatory fork in the LIQUIPHANT field device with the fundamental oscillation mode A at 1f.sub.0, the first higher oscillatory mode B in the vicinity of 7f.sub.0 and the second excited oscillatory mode in the vicinity of 13f.sub.0. In contrast, the first higher oscillatory mode B′ for an oscillatory fork of the invention (solid line) lies at about 6.5f.sub.0, and, thus in the range between two whole-numbered multiples of the fundamental frequency and is no longer excited by the exciter signal. The second higher oscillatory mode C′ of the oscillatory fork of the invention lies just about at 16f.sub.0, and, thus, in the region of the audible limit. The result is a clearly reduced noise emission of the oscillatory fork, such as is evident from the acoustic spectra in FIG. 3b) associated with the oscillation spectra. The decrease of the sound pressure for the first higher oscillatory mode B amounts to 32 dB(SPL) and that for the second higher oscillatory mode to 62 dB(SPL).

[0037] For manufacture of an optimized oscillatory fork of the invention, the mass distribution, the stiffness as well as the geometry were adapted by means of the finite elements method. In this regard, the mass distribution of the paddles was varied for shifting the first higher oscillatory mode B. For the second higher oscillatory mode C, in contrast, the radii in the transition region between the fork root and the membrane were varied, so that the stiffness as well as the bend line of the membrane, respectively the contact region between the oscillatory rod and the membrane, change.

[0038] For illustration, a conventional LIQUIPHANT oscillatory fork 4 and an oscillatory fork of the invention 4′ are placed alongside one another in FIG. 4. The figures, in each case, on the left represent the oscillatory fork in the LIQUIPHANT field device, while those on the right side are an embodiment of the invention. Furthermore, the reference characters, which refer to the embodiment of the invention, are provided with primes. The construction shown here is only one possible example of an oscillatory fork of the invention. There are countless other embodiments for oscillatory forks, which likewise would fall within the scope of the present invention.

[0039] On the left, in each case, are representations of the oscillatory fork in the LIQUIPHANT field device and on the right an analogous representation of an oscillatory fork of the invention. Depending on the process, some features of the conventional oscillatory fork in the LIQUIPHANT field device are maintained. These relate, on the one hand, to the length a of the membrane up to the end of the paddle at 40 mm, as well as width b of the paddle at 17.2 mm. Especially, attention was paid that the switching point of the oscillatory fork, correspondingly a frequency shift at a certain immersion depth into the medium, is not changed by the changes of the mass distribution and stiffness. It is understood, however, that here also other measures can be used for the oscillatable unit 8 and especially other switching points defined. FIG. 4a) provides a perspective view of the two oscillatory forks 4, 4′. For reasons of simplification, the following description is of only one of the two paddles 10,10′. The other paddle 10,10′ is analogously embodied. While for the conventional oscillatory fork 4 (left), the oscillatory rod 9 continues along the paddle 10 as rib 11, which protrudes out from the paddle surface, in the case of the oscillatory fork 4′ of the invention (right), the paddle 10′ and the rib 11′ merge to a homogeneous unit with curved surface, in which the oscillatory rod 9′ transitions homogeneously. The outer paddle surface 12 of the oscillatory fork 4 in the LIQUIPHANT field device is planar with superimposed rib 11, while for the oscillatory fork 4′ of the invention, the outer surface of the paddle 12′ is curved and merged with the rib 11′ and, thus, a homogeneous unit is formed. As a result of this merging, also the radius 13, respectively 13′, changes at the transition between oscillatory rod 9, 9′ and paddle 10,10′, as well as the paddle upper edge contour 14, respectively 14′, which is rounded for the oscillatable unit 4′ of the invention.

[0040] FIG. 4b) shows the oscillatable units 4, 4′ in a side view. In this representation, the differences between the outer surfaces 12, 12′ of the paddles 10,10′ can be yet better appreciated. For the oscillatory fork 4 in the LIQUIPHANT field device, the outer surface is planar, and for the oscillatory fork of the invention 4′ curved. In the here shown embodiment, the inner surfaces 15,15′ of the paddles are planar both for the oscillatory fork 4 and for the oscillatory fork 4′. It is understood, however, that also the inner surface of the paddle 15′ can be curved.

[0041] A further difference between the two oscillatory forks 4, 4′ relates to the angular orientations of the oscillatory rods 9,9′ at the joints 16, 16′ with the membranes 7,7′. This change can best be given by statement of the angles a and 13, which are drawn for the oscillatory fork 4 of the LIQUIPHANT field device. These angles for the oscillatory fork 4 in the LIQUIPHANT field device are α=35.5°, and β=107.7° while for the oscillatory fork 4′ of the invention, the analogous angles are α′=29.9° and β=104.9°.

[0042] On the whole, for the shown example of an oscillatable unit 4′ of the invention, the adapting of the mass distribution in the region of the paddle 10′, which results from the merging of the rib 11′ with the paddle surface, as well as the adapting of its curvature, effects the shifting of the first higher harmonic B. The shifting of the second higher harmonic C, in contrast, results from the adapting of the radii in the region of the joint 16, 16′ with the membrane and the changed angular orientation.

[0043] FIG. 5 shows, finally, two other variants of an oscillatory fork of the invention. Again, these are individual examples, and it is understood that besides these illustrated embodiments, there are still innumerable other variants, which can be designed and which all likewise fall within the scope of the invention. Here, FIG. 5a) shows a side view of an oscillatory fork 4′ of the invention as shown in FIG. 4. The lower edge contour 15′, i.e. the end region, of the paddle, is embodied straight in the case of this variant. In contrast, FIG. 5b) shows a possible embodiment of an oscillatory fork 4″ of the invention with rounded lower edge contour 15″, and FIG. 5c) an oscillatory fork 4′ of the invention with a pointed lower end 15′″. Also, in the case of these examples, the process related measures a and b are maintained. These different geometries for the end regions 15′, 15″, 15′″ of the paddles are motivated by the resulting differences in the drop shedding behavior. Rounded edge contours, 5″ or such with a point 15′″ have advantages in this regard. On the other hand, the change of the geometry of the end regions 15″, 15′ of the paddles changes also the sensitivity of the oscillatory forks, especially the switching point, so that, depending on choice of the end region 15′,15″,15′″, the mass distribution and stiffness must be adapted anew.

LIST OF REFERENCE CHARACTERS

[0044] 1 vibronic sensor [0045] 2 medium [0046] 3 container [0047] 4 oscillatable unit in the form of an oscillatory fork [0048] 5 electromechanical transducer unit [0049] 6 electronics unit [0050] 7 membrane [0051] 8 oscillatory element [0052] 9 oscillatory rod [0053] 10 terminally formed paddle [0054] 11 rib [0055] 12 outer paddle surface of the oscillatory fork [0056] 13 radius at the transition between oscillatory rod and paddle [0057] 14 upper edge contour of the paddle [0058] 15 lower edge contour of the paddle, respectively end region [0059] 16 angular orientation of the oscillatory rods at the joint with the membrane [0060] A fundamental oscillation mode of an oscillatory fork [0061] B first higher oscillatory mode of an oscillatory fork [0062] C second higher oscillatory mode of an oscillatory fork