EP2457067A1

EP2457067A1 - Vibratory transducer and measuring device comprising such a transducer

Info

Publication number: EP2457067A1
Application number: EP10726082A
Authority: EP
Inventors: Christian Schütze; Christof Huber; Vivek Kumar
Original assignee: Endress and Hauser Flowtec AG; Flowtec AG
Current assignee: Endress and Hauser Flowtec AG
Priority date: 2009-07-24
Filing date: 2010-06-22
Publication date: 2012-05-30
Also published as: CN102472652B; DE102009028007A1; US20110023624A1; US8113064B2; WO2011009684A1; CN102472652A

Abstract

The invention relates to a transducer, in particular also for the use in a Coriolis mass-flow measuring device, comprising at least one measuring tube (10), which is at least temporarily vibrating during operation, for guiding flowing medium, and a sensor array (50) serving to detect vibrations of the measuring tube (10). The measuring tube extends between a first measuring tube end on the inlet side and a second measuring tube end on the outlet side, having a vibration length (L₁₀) and performing vibrations about a pivoting axis that is parallel or coincident to an virtual connecting axis which imaginarily connects the two ends of the measuring tube, for example in a bending vibration mode. The sensor array generates a first primary transducer signal representing vibrations of the measuring tube (10) by means of a first vibration sensor (51) disposed on the measuring tube (10), and generates a second primary transducer signal representing vibrations of the measuring tube (10) by means of a second vibration sensor (52) disposed on the measuring tube (10) at a distance from the first vibration sensor (51), wherein the length of an area extending between the first and second vibration sensor of the first measuring tube (10) defines a measuring length (L₅₀) of the transducer. In a transducer according to the invention, the vibration sensors of the sensor array are placed in the transducer in such a way that a sensitivity (S_IST) of the transducer, with respect to a theoretical sensitivity at a measuring length (L₁₀ = L₅₀) that maximally corresponds to the vibration length, as well as a signal amplitude (A_IST) of the primary signals, effectively obtained during operation and with respect to a theoretically maximal possible signal amplitude (A_MAX) at the location of a maximal vibration amplitude, meet the condition (I).

Description

Vibration-type transducers and measuring instrument with such a transducer

The invention relates to a transducer of the vibration type with at least one in operation about a vibration axis, such as in a bending vibration mode, oscillating measuring tube for guiding flowing medium, such as a gas and / or a liquid, and a detection of vibrations of the measuring tube serving sensor assembly, the Vibrations of the at least one measuring tube representing primary signals supplies. Furthermore, the invention relates to, for example, as a compact meter and / or a Coriolis Massedurchfluß- meter trained measuring device, for flowable media, with such a transducer and an electrically coupled with this meter electronics for processing supplied by the transducer primary signals and Generation of measured values.

In industrial metrology, esp. Also in connection with the control and monitoring of automated process engineering processes, often used for the determination of characteristic variables of in a process line, such as a pipeline, flowing media, such as liquids and / or gases, measuring systems the by means of a transducer of the vibration type and a connected thereto, usually housed in a separate electronics housing, meter electronics with a driver and evaluation, in the flowing medium reaction forces, for example

Coriolis forces, induce and derived from these the at least one measure,

for example, a mass flow rate, a density, a viscosity or another

Produce process parameters, correspondingly representative measurement signal.

Such - often by means of an in-line meter in compact design with integrated

Measuring transducers, such as a Coriolis mass flow meter, formed - measuring systems have long been known and have proven themselves in industrial use. Examples of such measuring systems with a transducer of the vibration type or even individual components thereof, are e.g. in EP-A 317 340, EP-A 848 234, JP-A 8-13631 1, JP-A 9-015015, US-A 2007/01 19264, US-A 2007/0119265, the US-A 2007/0151370, US-A 2007/0151371, US-A

2007/0186685, US-A 2008/0034893, US-A 2008/0141789, US-A 47 38 144, US-A 47 77 833, US-A 47 77 833, US-A 48 01 897, US-A 48 23 614, US-A 48 79 911, US-A 50 09 109, US-A 50 24 104, US-A 50 50 439, US-A 52 91 792, US-A 53 01 557, US-A 53 98 554, US-A 57 34 112, US-A 54 76 013, US-A 55 31 126, US-A 56 02 345, US-A A 56 91 485, US-A 57 96 010, US-A 57 31 527, US-A 57 96 011, US-A 57 96 012, US-A 58 04 741, US-A 58 69 770, US-A 59 45 609, US-A 59 79 246, US-A 60 47 457, US-A 60 92 429, US-A 60 73 495, US-A 63 1 11 36 , US-B 62 23 605, US-B 63 30 832, US-B 63 97 685, US-B 65 57 422, US-B 66 51 513, US-B 66 66 098, US-B 66 91 583, US-B 67 76 052, US-B 67 99 476, US-B 68 40 109, US-B 68 83 387, US-B 69 20 798, US-B 70 17 424, US-B 70 40 179, US-B 70 73 396, US-B 70 77 014, US-B 70 80 564, US-B 72 OO 503, the US-B 72 16 550, US-B 72 99 699, US-B 73 18 356, US-B 73 60 451, US-B 73 92 709, WO-A OO 14 485, WO-A 01 02 816, WO-A 07/130024, WO-A 08/013545, WO-A 08/07 7574, WO-A 99/28708, WO-A 99 40 394 or WO-A 96 / 02812 described.

Each of the transducers shown therein comprises at least one substantially straight or at least one, for example U-shaped or V-shaped, curved measuring tube, for example made of

Stainless steel, titanium, zirconium or tantalum, for guiding the, possibly also extremely cold or extremely hot, medium. In order to generate through the medium flowing through with influenced waveforms that is vibrated between an inlet side first Meßrohrende and an outlet side second Meßrohrende with a vibration length extending at least one measuring tube during operation of the measuring system about an imaginary connecting the two ends imaginary axis of vibration, esp flexural mode.

For exciting vibrations of at least one measuring tube have transducers from

Vibration type, therefore, further includes an electrical drive signal generated in operation by one of the mentioned driver circuits of the meter electronics and conditioned accordingly, e.g. a regulated current, driven exciter arrangement which excites the at least one measuring tube by means of at least one in operation of a current flowing directly to the measuring tube electro-mechanical, esp. Electro-dynamic vibration exciter to mechanical vibrations, such as bending vibrations, and extent supplied by the meter electronics in the transducer electrical power into mechanical

Movements implemented. Furthermore, such transducers comprise a sensor arrangement with at least two, esp. Electro-dynamic and / or identical, vibration sensors for at least selectively detecting inlet-side and Auslaßseitiger oscillations of the at least one measuring tube, esp. Those in Coriolis mode, and for generating of to be detected

Process parameters, such as mass flow rate, total mass flow or density, affected sensor electrical signals as primary signals of the transducer.

As an excited waveform - the so-called drive or Nutzmode - is usually chosen in transducers with curved, eg U-, V- or Ω-like, measuring tube that natural mode in which the measuring tube at least partially at a lowest natural resonant frequency by an imaginary Longitudinal axis of the transducer oscillates in the manner of a cantilever clamped at one end, whereby in the medium flowing from the mass flow dependent Coriolis forces are induced. These in turn cause the excited vibrations of Nutzmodes, in the case of curved measuring tubes so pendulum-like boom vibrations, to the same frequency bending vibrations according to at least one also natural second mode of vibration, the so-called Coriolis mode superimposed. In transducers with a curved measuring tube, these Coriolis force-forced cantilever oscillations in Coriolis mode usually correspond to those natural vibration modes in which the measuring tube also executes torsional vibrations about an imaginary torsional vibration axis oriented perpendicular to the longitudinal axis. In the case of transducers with a straight measuring tube, on the other hand, such a useful mode is often selected for generating mass flow-dependent Coriolis forces, in which the measuring tube carries out bending oscillations substantially in a single imaginary plane of vibration, so that the oscillations in the Coriolis mode are correspondingly designed as bending vibrations of the same oscillation frequency that are coplanar with the useful mode oscillations are. The two Meßrohrenden are so far defined by those single two nodes, the utility and Coriolis are common. In the case of a curved measuring tube, the oscillating length thus more practically corresponds to a stretched length of an axis extending between the two aforementioned nodes, essentially

free-swinging pipe section of the respective measuring tube.

Due to the superimposition of useful and Coriolis mode, the means of the sensor arrangement on the inlet side and outlet side detected vibrations of the vibrating measuring tube on a dependent on the mass flow, measurable phase difference. Usually the measuring tubes are made of such, e.g. used in Coriolis Massedurchflußmessem, transducer in operation at a momentary natural resonant frequency of the selected mode for the mode of vibration, esp. At constant-controlled oscillation amplitude, excited. Since this resonant frequency is particularly dependent on the instantaneous density of the medium, can by means of

commercially available Coriolis mass flow meter in addition to the mass flow additionally the density of flowing media are measured. Further, it is also possible, as shown for example in US-B 66 51 513 or US-B 70 80 564, by means of transducers of the vibration type, to directly measure the viscosity of the medium flowing through, for example based on an excitation power required for the excitation of the vibrations ,

For transducers with two measuring tubes, these are usually integrated into the process line via an inlet-side distributor element extending between the measuring tubes and an inlet-side connecting flange and via an outlet-side distributor element extending between the measuring tubes and an outlet-side connecting flange. In transducers with a single measuring tube, the latter usually communicates via an inlet side opening essentially straight connecting pipe segment and an outlet side opening substantially straight connecting pipe segment with the process line. Furthermore, each of the transducers shown with a single measuring tube each comprising at least one one-piece or multi-part executed, for example, tube, box or plate, counter-oscillator, which is coupled to form a first coupling zone inlet side to the measuring tube and the outlet side to form a second coupling zone the measuring tube is coupled, and in operation essentially rests or opposite to the measuring tube, ie the same frequency and antiphase, oscillates. The inner part of the transducer formed by means of measuring tube and counteroscillator is usually held solely by means of two connecting pipe pieces, via which the measuring tube in operation with the process line, held in a protective transducer housing, esp. In a vibration of the inner part relative to the measuring tube enabling manner. Both

For example, in US-A 52 91 792, US-A 57 96 010, US-A 59 45 609, US-B 70 77 014, US-A 2007/01 19264, WO-A 01 02 816 or the transducer shown in WO-A 99 40 394 with a single, substantially straight measuring tube are the latter and the

Gegenschwinger, as usual in conventional transducers, each other in

essentially aligned coaxially. In marketable transducers of the aforementioned type is usually also the counteroscillator substantially tubular and formed as a substantially straight hollow cylinder, which is arranged in the transducer so that the measuring tube is at least partially encased by the counteroscillator. As materials for such counter-oscillators, esp. Also when using titanium, tantalum or zirconium for the measuring tube, usually

relatively inexpensive steel grades, such as mild steel or free-cutting steel used.

The excitation arrangement of transducers of the type in question usually has at least one electrodynamic and / or differentially acting on the at least one measuring tube and the optionally present counteroscillator or possibly existing other measuring tube

Vibration generator, while the sensor arrangement an inlet side, usually also electrodynamic, vibration sensor and at least one to substantially

identical outlet-side vibration sensor comprises. Such electrodynamic and / or differential vibration exciter commercially available transducers of the vibration type are at least temporarily by a current - in transducers with a measuring tube and a counteroscillator coupled thereto mostly fixed to the latter - magnetic coil and interacting with the at least one magnetic coil, esp. In this immersed, serving as an anchor rather elongated, esp. Rod-shaped, permanent magnet formed, which is fixed according to the measuring tube to be moved. The permanent magnet and serving as excitation coil magnetic coil are usually aligned so that they are in the

essentially coaxial. In addition, in conventional transducers, the exciter assembly is usually designed and placed in the transducer that it acts substantially centrally on the at least one measuring tube. Here is the vibration generator and insofar the

Exciter arrangement, as shown for example in the US-A 57 96 010, US-B 68 40 109, US-B 70 77 014 or US-B 70 17 424 proposed transducers, usually at least selectively along an imaginary central Peripheral line of the measuring tube fixed to the outside of this.

For most commercially available transducers of the vibration type, the vibration sensors of the sensor arrangement, as already indicated, at least to the extent substantially identical trained as the at least one vibration exciter, as they work on the same principle of action. Accordingly, the vibration sensors of such a sensor arrangement are usually each formed by means of a fixed to the measuring tube a magnetic permanent magnet armature and at least one cooperating with the armature, penetrated by the magnetic field and at least temporarily acted upon by an induced measuring voltage coil which, if present, usually on the counter-oscillator, otherwise fixed to one of the measuring tubes. Each of the aforementioned coils is also connected by means of at least one pair of electrical leads with the aforementioned operating and evaluation of the in-line measuring device, which usually on the shortest possible paths from the coils on the

Counteroscillator are guided to the converter housing.

The meter electronics of commercially available in-line meters of the aforementioned type usually have a digital measured values in real time, for example, by means of a digital signal processor (DSP) formed microcomputer. This includes, in addition to at least one corresponding processor and associated peripheral circuitry components, e.g. A / D converters and D / A converters, mostly corresponding volatile and non-volatile ones

Data storage for holding also from internally determined and / or externally transmitted to the respective InLine meter digital measurement or operating data, such as relevant for the measurement, serving as a reference chemical and / or physical properties of the medium to be measured. In addition to the microcomputer and the control of the transducer enabling driver circuit, the meter electronics also usually has a conditioning of the measuring transducer supplied by the measuring signals for the microcomputer realizing input circuit, the formation of said measurement and evaluation of the meter electronics with the microcomputer accordingly is interconnected. Based on the measurement signals provided by the transducer and / or transducer signals controlling the transducer electronics, the microcomputer determines the desired primary measurements, such as an instantaneous mass flow rate of the medium flowing through the transducer and / or a total mass flow rate Corresponds to mass of the medium that has flowed through the transducer for a given period of time, and provides it in real time.

Since conventional measuring systems of the type in question are usually designed as independent measuring devices which are to be integrated in a, for example, a filling process controlling and / or formed by programmable logic controllers (PLC), higher-level electronic data processing system, for example via 2-wire or via 4- Wire line, the respective meter electronics modern in-line measuring instruments of the type in question usually also a corresponding, the transmission or reception of measurement and / or operating data enabling communication circuit, for example, inform a in the industrial measurement and automation technology established digital output, an established 4-2OmA Current signal output, a bus interface compliant with NAMUR Recommendation NE43: 1994 and / or the PROFIBUS standard IEC 61 158 or an industry standard interface circuit. In addition, in the meter electronics and the internal supply of the in-line meter with electrical energy ensuring supply circuit is provided, the required energy via 4-wire or by means of, for example, as 4-2OmA current loop with meter-side load modulation trained , 2-wire cable from

electronic data processing system and / or from an internal energy storage relates.

Like u.a. in the above-mentioned EP-A 848 234 or WO-A 96/02812 removable, is formed in by means of a transducer of the vibration type measuring system for achieving the desired, not least also expected, high accuracy of positioning of the

Vibration sensors relative to selected nodes of the vibration for the purpose of measuring the primary measured variable mass flow excited vibrations of the measuring tube or the measuring tubes attach a special importance. According to EP-A 848 234 or WO-A 99/28708 also a low sensitivity to disturbances, about inform external vibrations, and insofar high measurement accuracy for measuring systems of the type in question would be achieved, for example, by the fact that the vibration sensors respectively as close as possible to nodes of the above-mentioned Nutzmodes be placed, whereby its share of the respectively detected by means of the sensor arrangement vibration and as far as possible at the respective primary signal is kept as low. In conventional conventional measuring systems of the type in question, esp. Even in such only with centrally acting on the measuring tube vibration exciter, the vibration sensors of the sensor arrangement in order to achieve the highest possible

Sensitivity to the primary measured variables, in particular the mass flow or the

Mass flow rate, at the same time the lowest possible sensitivity to any disturbances and sufficiently high signal-to-noise ratio of the primary signals in the range of the excited oscillation frequency typically placed in the transducer so that a length of a extending between the first vibration sensor and the second vibration sensor portion of the measuring tube corresponding Meßlänge of the transducer is more than 65% of the vibration length. In the case of curved measuring tubes, the measuring length corresponds to an extended length of the tube between the two vibration sensors, essentially free-swinging pipe section of the respective measuring tube.

However, studies on different measuring systems of the type in question have shown that a disadvantage of positioning the vibration sensors in the aforementioned manner is that to achieve a sufficient for the desired high measurement accuracy oscillation amplitude of 10-15μm at the location of the vibration sensors for the respective

Measuring system relatively large maximum vibration amplitudes for the excited vibrations in Nutzmode of about 30μm in the middle of the measuring tube are required, and thus a comparatively high, possibly far more than 10OmW amounting, electric power in the Exciter arrangement must be implemented, this to a special extent even at low

Rather bad.

Last but not least, also in in-line meters whose meter electronics, e.g. also proposed in the aforementioned US-B 67 99 476 or US-B 72 00 503, in operation only by means of both the Meßdaten- and the energy transfer serving 2-wire connection, for example, a 4-20mA current loop, with a However, both the constantly available and the maximum permissible electrical power is known to be limited, depending on the used or from a safety point of view allowed power supply to about 40-15OmW or 1W, so that may u In operation, sufficient electrical power is not always available for the excitation arrangement in order to be able to always provide the actually required signal-to-noise ratio or the required signal-to-noise ratio. For the case mentioned, that the in-line measuring device is supplied externally with electrical energy by means of a 4-2 oM current loop and also outputs the measured values by setting a proportional current strength of the current flowing in the current loop, the measuring system as a whole reverses the less electrical power and, to that extent, the less electrical exciter power available for the transducer, the more that would actually be needed for the desired high measurement accuracy. Moreover, there is a further disadvantage of high maximum vibration amplitudes in that it can increasingly provoke disturbing external vibrations and, as a result, the overall failure rate of the measuring system increases accordingly.

An object of the invention is therefore to improve the efficiency of transducers of the vibration type, with the current excitation in their respective exciter in operation fed electrical excitation power or excitation energy in primary signals are ultimately improved so that on the one hand, the primary signals, esp. Their respective Coriolis mode Representing signal components, with the lowest possible maximum amplitude of the measuring tubes and thus with low electrical excitation power the highest possible signal to noise ratio and the highest possible signal-to-noise ratio and on the other hand, the sensor array and the extent of the transducer as a whole, a sufficiently high sensitivity to the having sensing primary measures, esp. The mass flow rate and / or the totalized mass flow.

To solve the problem, the invention consists in a transducer of the vibration type, which transducer

at least one first measuring tube for guiding flowing medium, for example a gas and / or a liquid, which measuring tube is located between an inlet-side first

Meßrohrende and an outlet side second Meßrohrende extends with a swing length and in operation by an imaginary to the two Meßrohrenden imaginary connecting imaginary Connecting axis parallel or coincident vibration axis, for example, in a bending vibration mode, oscillates; such as

a sensor arrangement for detecting vibrations of the measuring tube with a measuring tube, for example, on the inlet side, arranged, for example, electrodynamic, first vibration sensor, which provides a vibration of the measuring tube representing the first primary signal of the transducer, and a spaced from the first vibration sensor on the measuring tube, for example on the outlet side, arranged , for example electrodynamic, second

Vibration sensor, which provides a vibration of the measuring tube representative second primary signal of the transducer, esp. Simultaneously to the first primary signal, comprising, wherein a length of a extending between the first vibration sensor and the second vibration sensor portion of the first measuring tube defines a measuring length of the transducer. The first vibration sensor of the sensor arrangement and the second vibration sensor of the sensor arrangement are also placed in the transducer that a sensitivity S _{IST of} the transducer, with a measured variable to be detected, esp. A mass flow rate m of a medium flowing through the transducer into a corresponding signal size of first and / or second primary signal, in particular a signal amplitude and / or a phase angle or a phase difference between the two primary signals, is converted, based on a theoretical sensitivity at a maximum length corresponding to the oscillation length, as well as a signal amplitude, Asr actually achieved in operation , the primary signals, relative to one at the location maximum

Vibration amplitude theoretically maximum possible signal amplitude, A _MAX , the condition

A S '

gl meet _- i ^I ^ij ₌ j ^ H_ _[ax so that 9Ϊ substantially or at least approximately

A-MAX ^ MAX

is maximum.

Moreover, the invention consists in a, for example, as a compact meter and / or a Coriolis mass flow meter trained, measuring device for flowable, esp. Fluid, media, such a transducer and a device electrically coupled with namely measuring instrument electronics for processing of primary signals supplied by the transducer and for generating measured values.

According to a first embodiment of the transducer of the invention, the at least one measuring tube is partially, esp. Within the itself between the first vibration sensor and the second

Vibration sensor extending area, arcuate, esp. Circular arc, formed.

According to a second embodiment of the transducer of the invention it is provided that the

Measuring tube is at least formed within the extending between the first vibration sensor and the second vibration sensor area substantially V-shaped. According to a third embodiment of the transducer of the invention it is provided that the measuring tube has a caliber which is more than 1 mm, in particular more than 5 mm. Further developing this embodiment of the invention is further provided that the caliber of the measuring tube is more than 50 mm, for example, more than 60 mm, and that the measuring length of the transducer less than 65% of the vibration length, for example, more than 40% of the vibration length , corresponds. Alternatively, the caliber of the measuring tube more than 15 mm, for example, more than 20 mm, and / or less than 50 mm, for example, less than 40 mm, amount, and the measuring length of the transducer thereby also less than 55% of the vibration length , In particular, the first measuring tube advantageously further dimensioned and the vibration sensors be placed so that a Meßlänge to caliber ratio of the transducer, defined by a ratio of the measuring length of the transducer to the caliber of the measuring tube, less than 10, esp. Smaller than 5, is.

According to a fourth embodiment of the transducer of the invention it is provided that the measuring tube is an inlet-side first straight tube segment with a in the direction of the first

Coupling zone pointing directional vector having imaginary longitudinal axis and an outlet-side second straight pipe segment having a pointing in the direction of the second coupling zone directional imaginary longitudinal axis, and that the two straight pipe segments, for example, to form an at least partially substantially V-shaped or U-shaped measuring tube , are aligned with each other so that the direction vector of the imaginary longitudinal axis of the first straight tube segment and the direction vector of the imaginary longitudinal axis of the second straight tube segment form an angle, esp., So that the angle less than 170 °, for example, less than 160 °, and / or more than 10 °,

for example, more than 20 °, is. At least in the event that the same angle is less than 100 °, it is further provided that the first vibration sensor of the sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer such that a measuring length-to-oscillation length ratio is defined by a ratio of the measuring length to

Oscillation length, less than or equal to 0.6, esp. Also such that the Meßlänge-to-Schwinglänge- ratio is greater than 0.3. At least in the event that the same angle is more than 100 °, for example, more than 115 °, is further provided that the first vibration sensor of the

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that the Meßlänge-to-swing length ratio is less than or equal to 0.62, esp. Also such that the Meßlänge-to-swing length ratio is greater than 0.45.

The fourth embodiment of the invention is further provided that the two straight pipe segments by means of an arcuate, for example circular arc,

Pipe segments are interconnected, esp. Such that the arcuate pipe segment measured from the center line of average pipe bend radius R, which is less than 500 mm, for example, less than 300 mm, and that the measuring tube, but at least the arcuate tubular segment, a Pipe wall thickness less than 7 mm, for example, less than 3 mm. Advantageously, the first measuring tube is further dimensioned so that the area moment of inertia of a cross section of the measuring tube is at least 40mm ⁴ , for example, more than 150mm ⁴ , esp. Such that a

Area of inertia to Meßlänge ratio ho / L ₅ o of the transducer, defined by a ratio of namely area moment of inertia to the measuring length of the transducer, more than 40mm ³ , for example, more than 100mm ³ , is. Alternatively or in addition to this, the arcuate tube segment can also be designed such that a tube bend radius-to-tube outer radius ratio, defined by a ratio of the tube bend radius through a tube outer radius of the arcuate tube segment, less than 60, for example, less than 50, and / or more than 3, for example, more than 4, is; This in particular also for the case that the first vibration sensor of the sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge-to-swing length ratio, defined by a ratio of the Meßlänge to the vibration length is greater than 0.4.

According to a fifth embodiment of the transducer of the invention it is provided that the first vibration sensor and the second vibration sensor are identical to one another.

According to a sixth embodiment of the transducer of the invention, this further comprises an inlet side on the measuring tube to form a first coupling zone and on the measuring tube to form a second coupling zone, esp. Oscillating in operation substantially opposite phase to the measuring tube and / or parallel thereto, counteroscillator, wherein the first coupling zone defines an inlet-side first end of the measuring tube and the second coupling zone defines an outlet-side second end of the measuring tube. This embodiment of the invention further forming is further provided in particular that both the first vibration sensor and the second vibration sensor are placed in the transducer so that each of the

Vibration sensors, for example, predominantly or exclusively, vibrations of the measuring tube relative to the counteroscillator, for example, differentially detect; and / or that measuring tube and counteroscillator oscillate in phase opposition to each other during operation at least on a common oscillation frequency; and / or that both the first primary signal and the second

Primary signal, for example, the same, represent oscillatory movements of the at least one measuring tube relative to the counteroscillator; and / or that the, and / or identical, vibration sensors vibration of at least one, and / or U- or V-shaped, measuring tube and, and / or U-shaped or V-shaped counter-oscillator, for example, simultaneously and / or differentially, to capture.

According to a seventh embodiment of the transducer of the invention it is provided that the first vibration sensor equidistant from a center of the measuring tube is placed in the transducer, as the second vibration sensor. According to an eighth embodiment of the transducer of the invention this further comprises two to form a first coupling zone inlet side by means of a, for example plate-shaped, first coupler element and forming a second coupling zone on the outlet side by means of a, for example plate-shaped, second coupler element mechanically interconnected, for example during operation substantially in opposite phase to each other oscillating and / or mutually parallel and / or identical in terms of shape and material, measuring tubes, wherein the first coupling zone in each case an inlet-side first end of each of the measuring tube and the second

Coupling zone each define an outlet side second end of each of the measuring tubes. Further developing this embodiment of the invention is further provided that each of the two measuring tubes in each case communicates with a first distributor element of the measuring transducer on the inlet side and with a second distributor element of the measuring transducer on the outlet side. Alternatively or in addition to this embodiment of the invention is further provided that the two measuring tubes oscillate in phase opposition to each other at least at a common oscillation frequency, and / or that both supplied by the first vibration sensor first primary signal of the transducer and that supplied by the second vibration sensor second primary signal of the transducer oscillations of the measuring tubes relative to each other, for example, to each other in opposite phase oscillations of the measuring tubes represent.

According to a ninth embodiment of the transducer of the invention, this further comprises at least one, especially one, in operation, for example, in an area of half the oscillation length, acting on the measuring tube, for example electrodynamic,

Vibration generator having exciter arrangement for vibrating the at least one measuring tube, for example in a bending mode in which it is at least partially

Performs bending oscillations around the imaginary axis of vibration. Further developing this embodiment of the invention is further provided in particular that the at least one measuring tube is excited at least temporarily in a Nutzmode by means of the excitation device, in which it, for example, predominantly or exclusively, bending vibrations about the imaginary axis of vibration, for example with a single and / or with a lowest

Resonant frequency of the measuring tube, performs, esp. Such that each of the primary signals of the

Transducer each one, for example, dominant and / or with the Nutzmode

corresponding, signal component with one of the bending vibrations in Nutzmode and / or one, for example, lowest, resonant frequency of the at least one measuring tube

having corresponding signal frequency. Alternatively or in addition to this is with this

Embodiment of the invention further provided that the first vibration sensor equidistant from the at least one vibration exciter spaced in the transducer is placed as the second vibration sensor. According to a tenth embodiment of the transducer of the invention it is provided that the measuring tube made of metal, esp. At least partially made of stainless steel, titanium, tantalum, or zirconium, is produced.

According to an eleventh embodiment of the transducer of the invention it is provided that the

Sensor arrangement otherwise has no additional vibration sensors in addition to the first and second vibration sensor.

According to a twelfth embodiment of the measuring transducer of the invention, it is further provided that the measuring length of the measuring transducer corresponding to the length of the region of the measuring tube extending between the first vibration sensor and the second vibration sensor is less than 65%, in particular less than 55%, the vibration length and more than 25%, in particular more than 30%, of

Oscillation length corresponds.

According to a first embodiment of the measuring device of the invention it is provided that the Meßgerät- electronics at least temporarily, both by means of the first primary signal and by means of the second primary signal, esp. Based on existing between the first primary signal and the second primary signal phase difference, a, esp. digital, mass flow rate measurement that currently represents a mass flow rate, m, of fluid flowing through the transducer.

According to a second embodiment of the measuring device of the invention it is provided that the measuring device electronics in operation repeatedly generates a phase difference value which currently represents the phase difference existing between the first primary signal and the second primary signal.

According to a third embodiment of the measuring device of the invention this further comprises a, in particular in operation with the evaluation circuit communicating, with the transducer electrically coupled, at least one of whose exciter device controlling exciter signal supplying driver circuit.

According to a fourth embodiment of the measuring device of the invention, it is provided that the measuring device electronics can be electrically connected to an external electronic data processing system by means of a two-wire connection, in particular as a 4-20 mA current loop.

According to a fifth embodiment of the measuring device of the invention, it is provided that the evaluation circuit at least temporarily generated by means of at least one of the primary signals, a digital, density measured value, which currently represents a density, p, of medium flowing through the transducer. According to a sixth embodiment of the measuring device of the invention, it is provided that the evaluation circuit generates, at least temporarily, by means of at least one of the primary signals, a digital, viscosity measured value which represents a viscosity, η, of medium flowing through the measuring transducer.

A basic idea of the invention is that of the selective detection of the

Oscillation movements of the at least one measuring tube, in particular those oscillations in the

Coriolis mode, serving vibration sensors in comparison to conventional transducers of the vibration type closer to the location of maximum vibration amplitude of the vibrations of the vibration

Nutzmodes - ie closer to at least one vibration exciter or closer to the center of the at least one measuring tube - to place, so as to achieve a good compromise between sufficiently high sensitivity, with each of the measured variable to be detected, such as the

Mass flow rate of the medium flowing through the transducer ultimately in a

corresponding signal magnitude of the respective primary signals, e.g. a signal amplitude, a signal difference and / or a phase angle or a phase difference between the two primary signals, is converted, on the one hand and sufficiently high signal amplitude and, consequently, sufficiently high signal-to-noise ratio of the primary signals of the transducer to achieve. The invention is based on the surprising finding that not only a high sensitivity - achievable by a high gauge length - decisive for the

Measuring accuracy of measuring systems of the type in question is, but in particular, the highest possible signal amplitude of the primary signals - achieved by the smallest possible Meßlänge. As a result, there is an optimum measuring length for vibration-type transducers in the event that a total product is maximally possible, that of an actual sensitivity S / sr of the transducer relative to a (theoretically) maximum possible sensitivity S _MAX , ie that sensitivity , with the oscillation length of the measuring tube of identical, maximum measuring length, and an actually achievable in the operation signal amplitude A _iS τ of the primary signals at the place of

Vibration sensors relative to the (theoretically) maximum possible signal amplitude A _MAX at the location of maximum oscillation amplitude, typically in the range of the vibration exciter or in the range of half the oscillation length, is formed, that is as a result the condition: is satisfied, ie that the function 9Ϊ maximized or at least approximately maximum.

An advantage of the invention is, inter alia, that even while maintaining established circuit architectures and technologies for Meßsignalaufbereitung and evaluation highly accurate measurement of the mass flow rate or the mass flow rate is also possible with very low excitation power and / or at very low mass flow rates. in the As a result, the measuring range of measuring systems of the type in question can be expanded as a whole. Another advantage of the transducer according to the invention is also to be seen in that are particularly suitable for use in small-power of less than 1W and / or by means of 4-20mA current loop operated measuring systems.

The invention and further advantageous embodiments thereof are explained in more detail below with reference to exemplary embodiments, which are illustrated in the figures of the drawing. Identical parts are provided in all figures with the same reference numerals; if it requires the clarity or it appears otherwise useful, is omitted reference numerals already mentioned in subsequent figures. Further advantageous embodiments or developments, esp. Combinations initially only individually explained aspects of the invention will become apparent from the figures of the drawing as well as the dependent claims per se.

In detail show:

Fig. 1a, b shows a variant of a trained as a compact meter measuring system for in

Piping flowing media in different side views;

Fig. 2a, b, another variant of a compact measuring device designed as measuring system for in

Piping flowing media in different side views;

Fig. 3 schematically in the manner of a block diagram a, esp. Also for a measuring system according to Figures 1a, 1 b, 2 a, 2 b, suitable, meter electronics connected thereto transducer of the vibration type;

Fig. 4, 5 in, partially in section and in perspective views, a variant of a, esp. For a measuring system according to Figures 1a, 1 b suitable, transducer of the vibration type;

Fig. 6, 7 in, partially cut or perspective views, a further variant of, esp. For a measuring system according to Figures 2a, 1 b suitable, transducer of the vibration type;

Fig. 8 is a schematic side view, esp. For use in one

Measuring transducer according to Figures 4 and 5 or 6 and 7 suitable, measuring tube. and

9 to 17 results of in the context of the invention, esp. Using computer-based simulation programs carried out experimental studies. 1a, 1b or 2a, 2b respectively show a variant of a process line, not shown here, such as a pipeline of an industrial plant, insertable measuring system designed, for example, as a Coriolis mass flowmeter, density measuring device, viscosity measuring device or the like for flowable, in particular fluid, media, in particular the measuring and / or monitoring of at least one physical quantity, such as a

Mass flow, a density, a viscosity, a pressure, etc., used by a medium flowing in the process line. The - realized here as an in-line measuring device in compact design - measuring system includes for this purpose a connected via an inlet end and an outlet end to the process line transducer of the vibration type, which transducer during operation

flows according to the medium to be measured, such as a low-viscosity liquid and / or a high-viscosity paste and / or a gas, and to a, in particular in the operation of externally via cable and / or supplied by means of internal energy storage with electrical energy, meter electronics ME of the measuring system is connected. This has, as shown schematically in Fig. 3 in the manner of a block diagram, serving to drive the transducer driver circuit Exe and a primary signals of the transducer MW processing,

For example, by means of a microcomputer formed and / or in operation with the driver circuit Exe communicating, evaluation circuit μC of the measuring system electrically

is connected, which supplies in operation the at least one measured variable, such as the current or a totalized mass flow, representing measured values. The driver circuit Exe and the evaluation circuit μC and other, the operation of the measuring system serving electronic components of the meter electronics, such as internal power supply circuits NRG for providing internal supply voltages U _N and / or the connection to a higher Meßdatenverarbeitungssystem and / or a communication bus COM serving a field bus, are also housed in a corresponding electronics housing 200, in particular impact-resistant and / or explosion-proof and / or hermetically sealed. For visualizing measuring system internally generated measured values and / or optionally measuring system internally generated status messages, such as an error message or an alarm on site, the measuring system further comprise at least temporarily communicating with the meter electronics display and control HMI, such as a in Electronics housing behind a window provided therein correspondingly placed LCD or TFT display and a corresponding input keyboard and / or a touch screen. Advantageously, the meter electronics ME, especially programmable and / or remotely programmable, can also be designed such that, during operation of the in-line meter, it is connected to a superordinate electronic data processing system, for example a programmable logic controller (PLC), a personal computer and / or. or a workstation, via data transmission system, such as a fieldbus system and / or wirelessly by radio, measuring and / or other operating data can exchange, such as current measurements or the control of the inline measuring device serving adjustment and / or

Diagnostic values. In this case, the meter electronics ME, for example, such an internal Have power supply circuit NRG, which in operation of a in the

Data processing system provided external power supply via the aforementioned

Field bus system is fed. In accordance with one embodiment of the invention, the meter electronics are further configured to be electrically connectable to the external electronic data processing system by means of a two-wire connection 2L configured, for example, as a 4-20 mA current loop, and supplied with electrical power thereto, and measurements can transmit to the data processing system. In the event that the in-line meter is intended for coupling to a fieldbus or other communication system, the meter electronics ME may have a corresponding communication interface COM for a

Having data communication according to one of the relevant industry standards. The electrical connection of the transducer to the mentioned meter electronics can be done by means of corresponding leads, which led out of the electronics housing 200, for example via cable bushing, and at least partially within the

Transformer housing are laid. The leads may be at least partially as electrical, at least partially formed in wrapped by an electrical insulation wires, e.g. inform of "twisted pair" cables, ribbon cables and / or

Coaxial cables. Alternatively or in addition to the connecting lines can at least in sections, by means of traces of a, especially flexible, optionally painted

Printed circuit board be formed, see. this also the aforementioned US-B 67 11 958 or US-A 53 49 872.

4 and 5 or 6 and 7, respectively, for further explanation of the invention, a first and a second embodiment for a suitable for the realization of the measuring system suitable transducers MW vibration type shown schematically. The transducer MW is generally used in a flowing medium, such as a gas and / or a liquid, mechanical

Reaction forces, e.g. Mass flow-dependent Coriolis forces, density-dependent inertial forces and / or viscosity-dependent frictional forces to produce, the measurable, esp. Sensory detectable, act back on the transducer. Derived from these reaction forces, e.g. a mass flow m, a density p and / or a viscosity η of the medium are measured. Each of the transducers comprises for this purpose in each case one arranged in a converter housing 100, the physical-electrical conversion of the at least one parameter to be measured actually acting inner part. In addition to receiving the inner member, the transducer housing 100 may also serve to secure the electronics housing 200 of the in-line meter therein

housed driver and evaluation circuit.

To guide flowing medium, the inner part of the transducer generally comprises at least a first - in the embodiment shown in FIGS. 4 and 5 - at least

partially curved measuring tube 10, which is located between an inlet side first

Meßrohrende 11 # and an outlet side second Meßrohrende 12 # with a swing length L _10th extends and vibrate to generate the aforementioned reaction forces during operation at least over its oscillation length L ₁₀ and thereby, oscillating about a static rest position, repeatedly elastically deformed. The oscillation length L ₁₀ corresponds, as shown schematically again in FIG. 8, in this case to a length of an imaginary center line or also gravity line (imaginary connecting line through the center of gravity of all cross-sectional areas of the measuring tube), ie in the case of a curved measuring tube that is an elongate line Length of the measuring tube 10.

It should be expressly noted at this point that - although the transducer in the embodiment shown in FIGS. 4 and 5 has only a single measuring tube and at least insofar in its mechanical structure as well as its operating principle in the US-B 73 60 451 or the US-B 66 66 098 proposed or even on the part of the applicant under the type designation "PROMASS H", "PROMASS P" or "PROMASS S" commercially available transducers similar - serve to implement the invention, of course, with more than one measuring tube can be similar to that shown in the aforementioned US-A 57 96 011, US-A 57 31 527, or US-B 69 20 798 or, for example, the part of the Applicant under the type designation "PROMASS E" or "PROMASS F" Commercially available transducers each with two parallel measuring tubes. Accordingly, the transducer can also at least two, for example by means of an inlet-side distributor element and an outlet-side distributor element, optionally additionally by means of at least one inlet-side coupling element and at least one outlet-side coupling element, mechanically coupled to each other and / or identical and / or curved and / or each other Have parallel, measuring tubes for guiding medium to be measured, which vibrate during operation for generating the primary signals at least temporarily, such as frequency equal to a common

Oscillation frequency, but opposite to each other in phase. According to one embodiment of the invention, the transducer, as shown schematically in FIGS. 6 and 7, therefore, in addition to the first measuring tube 10, a second measuring tube 10 'that on the inlet side by forming a first coupling zone by means of a, for example plate-shaped, first coupler element and under education a second coupling zone on the outlet side by means of a, for example plate-shaped and / or identical to the first coupler element, second coupler element with the first measuring tube 10 is mechanically connected. Also in this case, therefore, the first coupling zone each define an inlet-side first Meßrohrende 11 #, 1 1 '# each of the two measuring tubes 10, 10' and the second coupling zone each have an outlet-side second Meßrohrende 12 #, 12 '# # of the two measuring tubes 10, 10 '. Since, in the event that the inner part is formed by means of two measuring tubes, each of the two, in particular. In operation substantially opposite phase to each other oscillating and / or parallel and / or identical in terms of shape and material, measuring tubes serves to guide medium to be measured, communicates each of the two measuring tubes for another

Embodiment of this second variant of the transducer according to the invention in each case on the inlet side with an inflowing medium in two partial flows dividing common first distributor element 15 of the transducer and each outlet side with a the partial flows again merging common second distribution element 16 of the transducer, so that so both measuring tubes are flowed through during operation of the measuring system simultaneously and in parallel by medium.

As seen from the synopsis of Fign. 4 and 5 or 6 and 7 as well as Fig. 8 readily apparent, the at least one measuring tube 10 is in each case shaped so that the aforementioned center line, as quite normal in transducers of the type in question, is located in an imaginary tube plane of the transducer. According to one embodiment of the invention, the at least one measuring tube 10 is thereby vibrated during operation so that it is a vibration axis, esp. In a

Bieschwungungsmode, oscillates, which is parallel or coincident to an imaginary connecting the two Meßrohrenden 11 #, 12 # imaginary connecting axis. The at least one measuring tube 10 is further shaped and arranged in the transducer that the aforementioned

Connecting axis substantially parallel to an inlet and outlet end of the transducer imaginary connecting imaginary longitudinal axis L of the transducer extends, possibly also coincides.

Since the transducer should be used for a variety of different applications, esp. In the field of industrial measurement and automation technology, it is further provided that the at least one measuring tube has a tube inner diameter corresponding caliber D ₁₀ , the more than 1 mm, especially than 5 mm. In order to obtain a sufficiently high oscillation amplitude for the desired measurement accuracy, in particular also in flexural vibration mode, the at least one measuring tube according to one embodiment of the invention also has a

Pipe wall thickness s, which is less than 7 mm, esp. Less than 3 mm, esp. Such that an area moment of inertia I _{10 of} a cross section of the measuring tube, defined by the relationship

I ₁₀ = | D ⁴ ₀ - (D ₁₀ + s) ⁴ J, at least 40mm ⁴ , in particular more than 150mm ⁴ .

64

The at least one measuring tube 10 of the transducer, made, for example, from stainless steel, titanium, tantalum or zirconium or an alloy thereof, and to that extent also an imaginary center line of the measuring tube 10 running within lumens, may e.g. essentially U-shaped or, as also shown in FIGS. 4 and 5 or 6 and 7, be substantially V-shaped.

Accordingly, the at least one measuring tube according to a further embodiment of the invention, an inlet side first straight tube segment having an imaginary longitudinal axis having a pointing in the direction of the first coupling zone directional vector a1, and an outlet side second straight tube segment with an imaginary longitudinal axis, one in the direction of second

Coupling zone pointing direction vector a2, on. As can be readily seen from Figures 4 and 5 or 6 and 7, the two straight pipe segments, as in such

Meßrohrgeometrien quite common, connected by means of an arcuate - here a substantially circular arc-shaped - pipe segment. For the purpose of forming a compact transducer as possible of the shortest overall installation length is the arcuate Tube segment according to a further embodiment of the invention in this case also designed so that, measured from the center line, it has a mean pipe bend radius R, which is less than 500 mm, esp. Less than 300 mm. The two straight tube segments of the at least one measuring tube 10 are further aligned with each other so that, as also shown schematically in Fig. 8, the directional vector aj_ the imaginary longitudinal axis of the first straight tube segment and the direction vector a £ the imaginary longitudinal axis of the second straight tube segment an angle Θ include. The amount of the angle Θ is in the event that the two straight pipe segments are connected to each other via a circular arc-shaped pipe segment, by pipe bend radius R and the corresponding arc length B of the arcuate

Tube segment of the measuring tube determined, for example by the radian Θ = -, in radian or by

R

1 RO ⁰ R

the degree Θ =, in (old) degree. In particular, the two straight pipe segments

π R

the at least one measuring tube thereby aligned with each other so that the angle Θ is less than 170 ° and more than 10 °. According to a further embodiment of the invention, the measuring tube is further formed so that the angle Θ is less than 160 ° and / or more than 20 °. Alternatively or in addition, according to another embodiment of the invention, the arcuate pipe segment is formed so that a Rohrbogenradius-to-Rohraußenradius ratio R ', defined by a ratio of the pipe bend radius, R, by a with the measuring tube caliber D ₁₀ and the Wall thickness s corresponding outer tube radius, r = 0.5 • D ₁₀ + s, the arcuate

Pipe segment, less than 60, esp. Less than 50, and / or more than 3, esp. More than 4, is.

To minimize acting on the inner part formed by means of a single measuring tube disturbing influences as well as to reduce the part of the respective transducer to the connected process line total emitted vibration energy, the inner part of the transducer according to the embodiment shown in FIGS. 4 and 5 further comprises a mechanically with the - Here only - measuring tube 10 coupled, for example, similar to the measuring tube U- or V-shaped, counter-oscillator 20. This is, as shown in Fig. 2, laterally spaced from the measuring tube 10 in the transducer and to form a - ultimately the aforementioned first measuring tube end 11 # defining - first coupling zone inlet side and the formation of a - second aforementioned second Meßrohrende 12 # defining - second coupling zone on the outlet side fixed to the measuring tube 10. The - in this case substantially parallel to the measuring tube 10 extending, possibly also arranged coaxially to this - counteroscillator 20 is made of a tube with respect to the thermal expansion behavior compatible metal, such as steel, titanium or zirconium, and can be, for example, tubular or in be essential box-shaped also executed. As shown in Fig. 2 or, inter alia, proposed in US-B 73 60 451, the counteroscillator 20 may be formed for example by means of left and right sides of the measuring tube 10 arranged plates or also left and right side of the measuring tube 10 arranged dummy tubes. Alternatively, the counter-oscillator 20 - like as proposed in US-B 66 66 098 - also be formed by means of a single side of the measuring tube and extending parallel thereto dummy tube. As from a synopsis of Figs. 2 and 3, the counteroscillator 20 is supported in the embodiment shown here by means of at least one inlet-side first coupler 31 at the first Meßrohrende 11 # and at least one outlet side, in particular to the coupler 31 substantially identical, the second coupler 32 at the second Meßrohrende 12 #. As a coupler 31, 32, for example, simple node plates can be used here, the respective inlet side and outlet side respectively to measuring tube 10 and

Counteroscillator 20 are attached. Furthermore, as proposed in the embodiment shown in FIGS. 2 and 3, a nodal plate spaced apart from one another in the direction of the imaginary longitudinal axis L of the transducer together with protruding ends of the counteroscillator 20, respectively formed on the inlet side and outlet side, completely closed box or possibly partially open frame as a coupler 31 and serve as a coupler 32. As schematically illustrated in FIGS. 2 and 3, the measuring tube 10 is further connected via a straight first connecting tube section 11 which opens into the region of the first coupling zone on the inlet side and escpecially via an outlet side in the region of the second coupling zone

Connecting pipe piece 11 substantially identical, straight second connecting pipe piece 12 corresponding to the medium inlet and discharge - not shown here - connected process line, wherein an inlet end of the inlet side connecting pipe piece 11 practically the inlet end of the transducer and an outlet end of the outlet side connecting pipe section 12 the outlet end of Form transducer. Advantageously, the measuring tube 10 and together with the two connecting pipe pieces 11, 12 may be made in one piece, so that for their manufacture, for. a single tubular semi-finished product of a conventional material for such transducers, such as e.g. Stainless steel, titanium, zirconium, tantalum or corresponding alloys thereof. Instead of that measuring tube 10, inlet tube piece 1 1 and outlet tube 12 are each formed by segments of a single, one-piece tube, these, if necessary, but also by means of individual, subsequently assembled, e.g.

welded together, semi-finished products are produced. Im in Figs. 2 and 3 shown

Embodiment is further provided that the two connecting pipe pieces 11, 12, so aligned with each other and to one of the two coupling zones 11 #, 12 # imaginary connecting imaginary longitudinal axis L of the transducer, that here formed by counter-oscillator and measuring tube inner part, along with twists of two connecting pipe pieces 11, 12, can oscillate about the longitudinal axis L. For this, the two connecting pipe pieces 11, 12 are aligned with each other so that the substantially straight pipe segments are substantially parallel to the imaginary longitudinal axis L or to the imaginary axis of vibration of the measuring tube that the pipe segments are aligned both to the longitudinal axis L and each other substantially. Since the two connecting pipe pieces 11, 12 shown in here

Embodiment practically over its entire length away are carried out substantially straight, they are accordingly aligned overall relative to one another and to the imaginary longitudinal axis L substantially aligned. As can be further seen from FIGS. 2 and 3, this is, especially in the In comparison with the measuring tube 10, the bending and torsion-resistant transducer housing 100, in particular rigidly, is fixed to an inlet end of the inlet-side connecting tube 11 which is distal to the first coupling zone and to an outlet end of the outlet-side connecting tube 12 which is distal to the first coupling zone. In that regard, therefore, the whole - here by means of measuring tube 10 and counteroscillator 20 formed - inner part not only completely enveloped by the converter housing 100, but also supported vibrationally due to its own mass and the spring action of both connecting pipe pieces 11, 12 in the converter housing 100.

In the event that the transducer MW is releasably mounted with, for example, formed as a metallic pipe, process line, inlet side of the transducer of a first flange 13 and the outlet side, a second flange 14 are provided. The

Connecting flanges 13, 14 can, as is customary in the case of measuring transducers of the type described, also be integrated into the converter housing 100 at least partially at the end. If necessary, the connecting pipe pieces 11, 12 but also directly with the rest

Process line, e.g. by welding or brazing. In the embodiment shown in Fig. 2 and 3, the first connecting flange 13 are the inlet side

Connecting pipe section 11 formed at its inlet end and the second connecting flange 14 to the outlet side connecting pipe piece 12 at the outlet end, while in the embodiment shown in Fig. 4 and 5, the connecting flanges are connected according to the corresponding distribution elements.

For actively exciting mechanical oscillations of the at least one measuring tube 10 or the measuring tubes, each of the measuring transducers shown in FIGS. 4 to 7 further comprises a, esp.

Electrodynamic excitation arrangement 40. This serves - driven by a supplied by the driver circuit of the meter electronics and, optionally in conjunction with the evaluation circuit, suitably conditioned excitation signal, eg with a regulated current and / or a regulated voltage -jeweils , _Excited by the driver circuit electrical excitation _energy E _exc in a on the at least one measuring tube 10, for example, pulse-shaped or harmonic, acting and this in the manner described above deflecting excitation force F _exc convert. The excitation force F _exc may, as is usual with such transducers, be bidirectional or unidirectional and in the manner known in the art, for example by means of a current and / or voltage control circuit, in terms of their amplitude and, for example by means of a phase-locked loop, with regard to their Frequency are set. As an exciter assembly 40 may, for example, in a conventional manner by means of - for example, single, ie in the region of half an oscillating length L ₁₀ , on the respective measuring tube attacking, electrodynamic

Vibration generator 41 formed exciter assembly 40 serve. The vibration exciter 41 may, in the case of an inner part formed by counteroscillator and measuring tube, as indicated in FIG. 4, for example, by means of a cylindrical attached to the counter-oscillator 20

Excitation coil, which flowed during operation of a corresponding excitation current and thus is also flooded by a corresponding magnetic field, and a at least partially immersed in the exciter coil permanent magnet armature, which is fixed from the outside, esp. Centrally, on the measuring tube 10, be formed. Further excitation arrangements for oscillations of the at least one measuring tube which are also suitable for the measuring system according to the invention are described, for example, in the aforementioned US-A 57 05 754, US-A 55 31 126, US-B 62 23 605, US-B 66 66 098 or US-B 73 60 451.

According to a further embodiment of the invention, the at least one measuring tube 10 is actively excited in operation by means of the excitation arrangement at least temporarily in a Nutzmode in which it, esp. Predominantly or exclusively, bending vibrations to the mentioned imaginary

Performs vibration axis, for example, predominantly with exactly one resonance frequency of the respective or thus each formed inner part of the transducer, such as that corresponding to a bending vibration fundamental mode in which the at least one measuring tube has exactly one antinode. In particular, in this case it is further provided that the at least one measuring tube 10, as in such transducers with curved measuring tube quite common, excited by means of the excitation system to bending vibrations at an excitation frequency f _e χ _C , so that it is in the Nutzmode to the mentioned imaginary axis of oscillation - approximately in the manner of a cantilever cantilever - oscillating, at least partially auszubig according to one of its natural bending modes. The bending oscillations of the measuring tube have an inlet-side node in the region of the inlet side end of the measuring tube 11 # defining the inlet-side coupling zone and an outlet-side node in the region of the outlet-side coupling tube 12 # defining outlet-side coupling zone, so that the measuring tube with its oscillating length L ₁₀ between them both oscillation node extends substantially free swinging. If necessary, the vibrating measuring tube but also, as proposed in US-B 70 77 014 or JP-A 9-015015, by means of correspondingly in the range of the vibration length on the measuring tube additionally attacking resilient and / or electromotive coupling elements in its oscillatory movements be specifically influenced. The driver circuit may be formed, for example, as a phase-locked loop (PLL), which is used in the manner known to the expert to an excitation frequency, f _{exc of} the

Excitation signal constantly to the current natural frequency of the desired Nutzmodes

match. The construction and use of such phase-locked loops for actively exciting measuring tubes to oscillations on a mechanical natural frequency is described in detail, for example, in US Pat. No. 4,801,897. Of course, other suitable for setting the excitation _energy E _exc suitable, known to _those skilled and driver circuits, for example, according to the above-mentioned prior art, such as the aforementioned US-A 47 77 833, US-A 48 01 897, US-A 48 79 91 1, US-A 50 09 109, US-A 50 24 104, US-A 50 50 439, US-A 58 04 741, US-A 58 69 770, US-A 6073495 or US-A 63 11 1 36. Furthermore, with regard to the use of such drive circuits for vibration-type transducers, reference should be made to the measuring instrumentation provided with transmitters of the "PROMASS 83" series. Electronics, as described for example in connection with "PROMASS E", "PROMASS F", "PROMASS H", "PROMASS I"

"PROMASS P" or "PROMASS S" are offered. The driver circuit is, for example, in each case designed such that the lateral bending oscillations in the payload mode are regulated to a constant, thus also independent of the density, p, substantially independent amplitude.

To vibrate the least one measuring tube 10, the exciter assembly 40, as already mentioned, by means of an equally oscillating excitation _signal of adjustable excitation frequency, f _exc fed, so that the excitation coil of - here only on the measuring tube 10 attacking

Vibration exciter - in operation of a regulated in its amplitude accordingly

_Exciter current i _{exc is flowed} through, which required for moving the measuring tube

Magnetic field is generated. The driver or exciter _signal or its excitation current i _exc may be harmonic, multi-frequency or even rectangular, for example. The excitation frequency, f _e χ _C , required for maintaining the bending vibrations of the at least one measuring tube 10

Excitation current i _exc can be selected and adjusted in an advantageous manner in the embodiment shown in the embodiment, that the laterally oscillating measuring tube 10 oscillates at least predominantly in a bending vibration fundamental mode with a single antinode. Accordingly, according to a further embodiment of the invention, the excitation or Nutzmodefrequenz, f _exc , adjusted so that it corresponds as closely as possible to a natural frequency of bending vibrations of the measuring tube 10, esp. Of the Bieschwwingungsgrundmodes. When using an off

Stainless steel, esp. Hastelloy made measuring tube with a caliber D ₁₀ of 29 mm, a wall thickness s of about 1, 5 mm, a swing length of about 420 mm and a stretched length, measured between the two Meßrohrenden, of 305 mm, the The resonance frequency thereof corresponding to the bending vibration fundamental mode may be approximately 490 Hz, for example, at a density of practically zero, for example in the case of a measuring tube filled only with air.

In the embodiment shown in FIGS. 4 and 5 with inner part formed by means of a measuring tube and counteroscillator, the measuring tube 10 carries out the bending oscillations actively excited by the excitation arrangement predominantly relative to the counteroscillator 20, in particular in opposite phase to one another at a common oscillation frequency. In the case of a simultaneously, for example differentially, acting on both measuring tube and counteroscillator exciter arrangement is doing

Forcibly also the counteroscillator 20 is excited to simultaneous cantilever oscillations, in such a way that it oscillates at the same frequency, but at least partially out of phase, esp. Essentially opposite phase, oscillating in the Nutzmode measuring tube 10. In particular, measuring tube 10 and counteroscillator 20 are further coordinated or excited so that they perform at least temporarily and at least partially counterparts, ie equal frequency, but substantially out of phase, bending vibrations about the longitudinal axis L during operation. The

Bending vibrations can be designed so that they are of the same modal order and thus at least at rest fluid substantially uniform; in the other case the Using two measuring tubes, these, as usual with transducers of the type in question, by means of the, esp. Differentially between the two measuring tubes 10, 10 'acting energizer arrangement actively excited so that they run during operation at least temporarily gegengleiche bending vibrations about the longitudinal axis L. In other words, the two measuring tubes 10, 10 'or measuring tube 10 and counter-oscillator 20 then each move in the manner of mutually oscillating tuning fork tines.

For the operationally provided case that the medium flows in the process line and thus the mass flow m is different from zero, also Corioliskräfte be induced by means of vibrating in the manner described above measuring tube 10 in the medium flowing. These in turn act on the measuring tube 10 and thus cause an additional, sensory detectable deformation of the same, namely essentially according to a further natural natural mode of higher modal order than the Nutzmode. A momentary expression of this so-called, the excited Nutzmode superimposed on an equal frequency

Coriolis is in this case, especially in terms of their amplitudes, depending on the instantaneous mass flow m. As Coriolis mode, as is common with such curved tube transducers, e.g. serve the natural mode of the anti-symmetric twist mode, ie those in which the measuring tube 10, as already mentioned, and torsional vibrations about a perpendicular to the

Bending vibration axis aligned imaginary torsional vibration axis that intersects the center line of the measuring tube 10 in the region of half the oscillation length L ₁₀ imaginary.

For detecting oscillations, in particular bending oscillations, of the at least one measuring tube 10, in particular also those in Coriolis mode, the measuring transducer furthermore has a corresponding sensor arrangement 50 in each case. This includes, as also schematically illustrated in FIGS. 4 to 7, a spaced from at least one vibration exciter on at least one measuring tube 10, for example, electrodynamic, first vibration sensor 51, the one

Vibrations of the measuring tube 10 representing the first primary signal Si of the transducer provides, for example, a voltage corresponding to the vibrations or corresponding to the vibrations current, and a spaced from the first vibration sensor 52 at least one measuring tube 10 arranged, esp. Electrodynamic, second vibration sensor 52, the a second vibration representative of the measuring tube 10

Primary signal S _{2 of} the transducer provides. A length of between the two, for example identical, vibration sensors extending, esp. Essentially free-vibrating, the corresponding at least one measuring tube corresponds, as shown schematically in Fig. 8, in this case a measuring length L _{50 of} the respective transducer. Each of the - typically broadband - primary signals si, S _{2 of} the transducer MW in this case has in each case one corresponding to the Nutzmode signal component with one of the current

Oscillation frequency, f _e χ _C , of the oscillating in active excited Nutzmode at least one measuring tube 10 corresponding signal frequency and one of the current mass flow of the im at least one measuring tube 10 flowing medium dependent phase shift relative to, for example by means of PLL depending on a between at least one of

Vibration _signals Si, S ₂ and the excitation current in the exciter _arrangement existing phase difference generated excitation _signal i _exc on. Even in the case of using a rather broadband excitation _signal i _exc can be assumed that the corresponding with the Nutzmode signal component of each of the primary signals other, esp. With any external interference corresponding and / or classify as noise due to the usually very high vibration quality of the transducer , Signal components predominates and so far also at least within one of a bandwidth of the Nutzmodes corresponding

Frequency domain is dominant.

In the embodiments shown here, the first vibration sensor 51 on the inlet side and the second vibration sensor 52 are arranged on the outlet side at least one measuring tube 10, esp. From at least one vibration exciter or equidistant from the center of the measuring tube 10 as the first vibration sensor. As with such, used in a designed as a Coriolis mass flow meter measuring system, transducers from

Vibration type quite common, the first vibration sensor 51 and the second

According to an embodiment of the invention, the vibration sensor 52 is further arranged in each case on a side of the measuring tube occupied by the vibration exciter 41 in the measuring transducer.

Furthermore, the second vibration sensor 52 can also be arranged on the side of the measuring tube occupied by the first vibration sensor 51 in the transducer. The

In addition, vibration sensors of the sensor arrangement can advantageously also be designed so that they provide primary signals of the same type, for example, in each case a signal voltage or a signal current. According to a further embodiment of the invention, both the first vibration sensor and the second vibration sensor are further each placed in the transducer MW, that each of the vibration sensors at least predominantly detects vibrations of at least one measuring tube 10. For the case described above, that the inner part is formed by means of a measuring tube and a counter-oscillator coupled thereto, according to a further embodiment of the invention, both the first vibration sensor and the second

Vibration sensor designed and placed in the transducer so that each of the

Vibration sensors predominantly oscillations of the measuring tube relative to the counteroscillator, for example, differentially detect, so that both the first primary signal Si and the second primary signal S ₂ , esp. Counterparts, represent oscillatory movements of at least one measuring tube 10 relative to the counteroscillator 20. For the other case described that the inner part is formed by means of two, esp. In operation gegengleich swinging, measuring tubes, according to another embodiment of the invention, both the first vibration sensor and the second vibration sensor is formed and placed in the transducer so that each of the

Vibration sensors predominantly oscillations of the first measuring tube 10 relative to the second measuring tube 10 ', for example, differentially detect, so that both the first primary signal Si as Also, the second primary signal S ₂ , esp. Opposite, represent oscillatory movements of the two measuring tubes relative to each other. According to a further embodiment of the invention, it is provided that the sensor arrangement has exactly two vibration sensors, that is to say in addition to the first and second vibration sensors no further vibration sensors, and insofar corresponds to a conventional sensor arrangement with regard to the components used.

The supplied by the sensor arrangement Schwingungsmeßsignale si, S ₂ , each one

Signal component with a current oscillation frequency, f _e χ _C , of the active excited in Nutzmode oscillating at least one measuring tube 10 corresponding signal frequency are, as shown in Fig. 3, that of the meter electronics ME and there then the measuring and Evaluating circuit μC supplied where they are first preprocessed by means of a corresponding input circuit FE, esp. Pre-amplified, filtered and digitized, to then be able to be suitably evaluated. As an input circuit FE as well as a measuring and evaluation circuit μC here used in conventional Coriolis mass flow meters for the purpose of converting the primary signals used or determination of mass flow rates and / or totalized mass flows, etc. already used and established

Circuit technologies are applied, for example, those according to the above-mentioned prior art. According to a further embodiment of the invention, the measuring and evaluating circuit μC is accordingly also realized by means of a measuring device electronics ME provided, for example by means of a digital signal processor (DSP),

Microcomputers and means implemented in this and running in it

Program codes realized. The program codes can be persistently stored, for example, in a non-volatile memory EEPROM of the microcomputer and, when it is started, loaded into a volatile memory RAM integrated, for example, in the microcomputer. Processors suitable for such applications are, for example, those of the TMS320VC33 type marketed by Texas Instruments Inc. It goes without saying that the primary signals si, S ₂ as already indicated, for processing in the microcomputer by means of corresponding analog-to-digital converter A / D of the meter electronics ME in

corresponding digital signals are to be converted, cf. For this example, the aforementioned US-B 63 11 136 or US-A 60 73 495 or the aforementioned transmitter of the series "PROMASS 83".

The measuring and evaluating circuit μC is used according to an embodiment of the invention in particular, by means of the primary signals si, S ₂ supplied by the sensor arrangement 50, for example by means of a primary signals si, S ₂ generated between the measuring tubes 10 which oscillate proportionally in useful and Coriolis mode of the first and second vibration sensors 51, 52 detected phase difference, recurring a mass flow measurement value X _m to determine the mass flow rate to be measured, m, of the medium guided by the transducer as possible exactly represented. Alternatively or in addition to the measurement and evaluation circuit, for example, derived from a current mass flow value X _m and / or a plurality of pre-sequentially generated and / or mass flow measurements, to determine a mass measured value X _M , which is a totalized Mass flow, M, currently represented. For this purpose, the evaluation circuit according to a further embodiment of the invention in operation repeatedly generates a phase difference value X _Δφ which currently represents the phase difference Δφ i existing between the first primary signal Si and the second primary signal S ₂ . Furthermore, the evaluation circuit of the measuring system according to the invention can also be used, derived from one, for example on the basis of at least one of the primary signals supplied by the sensor arrangement measured vibration frequency of lateral bending vibrations of the at least one measuring tube 10, for example, those in Nutzmode, in the person skilled in and for In a known manner additionally generate a, for example digital, density measurement value X _p , which currently represents a density to be measured, p, of the medium. As an alternative or in addition to this, the evaluation circuit, as is customary for in-line measuring devices of the type in question, may also be used, derived from the _{drive signal} i _eXc , which is also known as a measure of an apparent viscosity or a viscosity index. Density product of the medium guided in the measuring tube can serve to determine a, for example digital, viscosity measured value X _η , which currently represents a viscosity of the medium, cf. this also the US-B 70 17 424, US-B 68 40 109 or US-B 66 51 513. Incidentally, however, can be readily assumed that determined by means of the meter electronics, esp. Also any provisional, Measured values in the measuring device electronics ME are buffered at least temporarily, for example in the mentioned EEPROM memory and / or RAM memory, and can thus be kept sufficiently long for subsequent uses. The abovementioned, in particular also the arithmetic functions respectively serving the generation of the mass flow measurement value X _m or other of the aforementioned measured values, can be realized very simply, for example by means of the abovementioned microcomputer of the evaluation circuit μC or, for example, also a digital signal processor DSP provided therein be. The creation and implementation of corresponding algorithms which correspond to the above-described formulas or, for example, also reproduce the mode of operation of the mentioned amplitude or frequency control circuit for the excitation arrangement, as well as their translation in the meter electronics according to executable program codes is the person skilled in and for is familiar and therefore requires - at least in knowledge of the present invention - no more detailed explanation.

Of course, the aforementioned formulas or other realized with the meter electronics functionalities of the measuring system can also be readily realized in whole or in part by means of corresponding discretely constructed and / or hybrid, ie mixed analog-digital, arithmetic circuits in the meter electronics ME.

In order to achieve the highest possible efficiency with the electrical excitation power or exciter _energy E _exc fed into the exciter arrangement during operation, _{it is} ultimately into the primary signals si, s ₂ or in the with the by means of the transducer to be detected each measured variable, such as the mass flow rate and / or density, corresponding signal size, such as a

Signal amplitude, a signal frequency and / or a phase angle or a phase difference between the two primary signals, etc., be converted, esp. Such that the mentioned, quasi a universal optimization function for transducers of the type in question defining,

A S

Condition 91 = - ^ - = A * S * is maximally possible, are in the inventive

A-MAX ^ MAX

Measuring system, the first vibration sensor of the sensor assembly and the second

Vibration sensor of the sensor assembly placed in the transducer so that the measuring length L _{50 of} the transducer less than 65%, esp. Less than 55%, the oscillation length L ₁₀ and more than 25%, esp. More than 30%, the oscillation length L ₁₀ , see. 9, in particular also in conjunction with FIG. 8. In other words, the two vibration sensors are optimally placed in the transducer when the actual sensitivity SIST achieved by the sensor

Transducer MW relative to - theoretically - maximum possible sensitivity SMAX, ie that sensitivity at a maximum length corresponding to the oscillation length L ₁₀ (L ₅₀ = L ₁₀ ), and actually achievable in operation signal amplitude Asr the primary signals si, S ₂ respectively at the place of Vibration sensors relative to - theoretically - maximum possible signal amplitude A _M AX at the location of maximum vibration amplitude - in this case the vibration exciter or at half the swing length L ₁₀ (L ₅₀ = 0) - maximum or at least almost maximum, which in turn surprisingly in the usual Meßrohrgeometrien in the aforementioned, but not used for the sensor positioning range between 65% and 30% of the oscillation length L _{10 is} the case; see. See also Fig. 9.

Further investigations, esp. Also by means of computer-aided simulation calculations on transducers with typical Meßrohrkonfigurationen - such as curved measuring tubes with a caliber D ₁₀ in the range between 10mm and 250mm - have also shown that - as, inter alia, from the synopsis of Fig. 10, 1 1, 12, 13, 14, 16 and 17 readily apparent - the first vibration sensor of the sensor assembly and the second vibration sensor of

Sensor arrangement as possible to be placed in the transducer, that a Meßlänge-to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length L ₅₀ to

Oscillation length L _10, the condition ξ <0.6, esp. Such that the condition ξ> 0.35 is satisfied.

By further investigations, of which individual results are shown by way of example in FIG. 10, on a large number of typical transducer configurations with an essentially V-shaped curved measuring tube, it has been found in particular that optimization of the

Measuring transducer in the above sense, the first vibration sensor of the sensor assembly and the second vibration sensor of the sensor assembly in response to the mentioned, enclosed by the two straight pipe segments angle Θ is to be placed in the transducer that the mentioned Meßlänge-to-swing length ratio, ξ = L ₅₀ / L ₁₀ , the condition ξ≤0.57 1 - 0.1 - sinl- - 30, this is especially true for such transducers with V

2

curved measuring tube, where the angle Θ is less than 100 °.

By further case studies on transducers in which the angle Θ was more than 100 °, esp. Also more than 115 °, has been determined by for different sensor positions and

Meßrohrkaliber also shown that for a variety of conventional Meßwandlerkonfigurationen with V-shaped measuring tube an optimal Meßlänge-to-swing length ratio ξ = L ₅₀ / L _{10 is} to be found in a range by the condition ξ <0.62, esp. But also the Condition ξ> 0.45, is satisfied.

As a further variable for the dimensioning of an optimal sensor position in the above sense and, consequently, an optimal measuring length or an optimal measuring length-to-oscillation length ratio, ξ, has been exemplified by further investigations, of which individual results in FIGS. 11 to 14 are, exposed to transducers with a substantially V-shaped measuring tube of the above-mentioned pipe bend radius R of the arcuate pipe segment. Accordingly, it may also be advantageous for the achievement of the highest possible efficiency of the transducer in the above sense, if for the mentioned case that the Meßlänge-to-swing length ratio, ξ = L ₅₀ / L ₁₀ less than 0.65, esp is more than 0.4, the pipe bend radius R - in dependence also on the pipe outer radius r (0.5 D ₁₀ + s) of the at least one measuring tube 10 - the condition:

R <- or satisfies the condition R '<or vice versa if the Meßlänge- ξ - 0.4 ξ - 0.4 to swing length ratio, ξ = L ₅₀ / L ₁₀ , the condition ξ <- h 0.4 or ξ≤ h 0.4

R R 'satisfied; the latter in particular for the above-mentioned case that the arcuate pipe segment is formed so that its pipe bend radius to pipe outer radius ratio R 'is less than 60 and / or more than 3.

To further improve the aforementioned efficiency of the transducer or to maximize the aforementioned optimization function 9Ϊ the at least one measuring tube are dimensioned according to a further embodiment of the invention and the vibration sensors placed in the transducer so that a Meßlänge to caliber ratio L ₅₀ / D _{10 of} the transducer, defined by a ratio of the measuring length L _{50 of} the transducer to the caliber D _{10 of} the measuring tube, less than 10, esp. Less than 5, is; esp. Such that, as also apparent from Fig. 15, the caliber D _{10 of} the at least one measuring tube is more than 15 mm, esp. More than 20 mm, and that the measuring length L _{50 of} the transducer less than 55% of Oscillation length L ₁₀ corresponds, or that in the event that the caliber D _{10 of} the measuring tube is more than 50 mm, esp. More than 60 mm, the measuring length L _{50 of} the transducer less than 65% of the oscillating length L ₁₀ , esp. But more than 40% of the vibration length L ₁₀ , corresponds; this in particular also for the above-mentioned case, that the same moment of inertia I _{10 of} the measuring tube is 40 mm ⁴ or more or the measuring tube also shaped and dimensioned and the vibration sensors are placed so that, as shown in FIG. 17, a Area of inertia to Meßlänge ratio I ₁₀ / L _{50 of} the transducer, defined by a ratio of an area moment of inertia I _{10 of} a cross section of the measuring tube to the measuring length L _{50 of} the transducer, more than 40 mm ³ , esp. More than 100 mm ³ , is ,

In view of the above-described rules for measuring tube and sensor arrangement, it is now no difficulty for the expert to optimize transducer of the type in question such that on the one hand, the primary signals at the lowest possible maximum amplitude of the at least one measuring tube or at the lowest possible electrical excitation power have a high signal-to-noise ratio and a high signal-to-noise ratio, and that, on the other hand, the transducer is nevertheless sufficiently sensitive to the primary measured quantities to be detected, in particular the mass flow rate and / or the totalized mass flow.

Claims

PATENTAN SPEECHES

A vibration-type transducer comprising:

at least a first measuring tube (10) for guiding flowing medium, esp. a gas and / or a liquid, which measuring tube (10) extends between an inlet-side first Meßrohrende and an outlet-side second Meßrohrende with a vibration length (L ₁₀ ) and in Operation oscillates about an imaginary connecting the imaginary connecting axis imaginary connecting axis parallel or coincident vibration axis, esp. In a bending vibration mode; such as

- A detecting the vibrations of at least the first measuring tube (10) serving

Sensor arrangement (50) with

- one on the measuring tube (10), esp., On the inlet side, arranged, esp. Electrodynamic, first vibration sensor (51), which provides a vibration of the first measuring tube (10) representing the first primary signal (si) of the transducer, and

a second oscillating sensor (52) arranged on the measuring tube (10) and spaced apart from the first oscillating sensor (52), the second primary signal (S ₂ ) of the measuring transducer representing vibrations of the first measuring tube (10), in particular simultaneously with the first primary signal (si);

- Wherein a length of a between the first vibration sensor and the second

Vibration sensor extending portion of the first measuring tube (10) defines a measuring length (L ₅₀ ) of the transducer, and

- Wherein the first vibration sensor of the sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer, that

a sensitivity, SIST, of the transducer, with which a measured variable to be detected, in particular a mass flow rate m, of a medium flowing through the transducer into a corresponding signal magnitude of the first and / or second primary signal, esp

Signal amplitude and / or phase angle or phase difference between the two primary signals converted, based on a theoretical sensitivity at one of the resonant length (Li ₀₎ corresponding maximum measurement length (Li ₀ = L _50), and

a signal amplitude, As ₁ , of the primary signals (SK S?) actually achieved in operation, based on a maximum maximum possible oscillation amplitude at the location

A S '

Signal amplitude, A ' _M AX', satisfy the condition 1- ς .- = Max.

^ ¹ MAX ⁰ MAX

2. Transducer according to one of the preceding claims, wherein the at least one measuring tube partially, esp. Within the itself between the first vibration sensor and the second

Vibration sensor extending portion, arcuate, esp. Circular arc, is formed.

3. Transducer according to one of the preceding claims, wherein the at least one measuring tube at least within the between the first vibration sensor and the second

Vibration-extending portion is formed substantially V-shaped.

4. Transducer according to one of the preceding claims, wherein the at least one measuring tube has a caliber (D ₁₀ ) which is more than 1 mm, esp. More than 5 mm.

5. A transducer according to claim 4, wherein the caliber (D ₁₀ ) of the measuring tube is more than 50 mm, esp. More than 60 mm, and wherein the measuring length (L ₅₀ ) of the transducer less than 65% of the oscillating length (L ₁₀ ) , in particular more than 40% of the oscillation length (L ₁₀ ), corresponds.

6. A transducer according to claim 4, wherein the caliber (D ₁₀ ) of the measuring tube is more than 15 mm, esp. More than 20 mm, and / or less than 50 mm, esp. Less than 40 mm, and wherein the measuring length ( L ₅₀ ) of the transducer corresponds to less than 55% of the oscillation length (L ₁₀ ).

7. A transducer according to any one of claims 4 to 6, wherein the first measuring tube is dimensioned and the vibration sensors are placed so that a Meßlänge to caliber ratio L ₅₀ / D _{10 of} the transducer, defined by a ratio of the Meßlänge (L ₅₀ ) of the transducer to the caliber D _{10 of} the measuring tube, less than 10, esp. Less than 5, is.

8. Transducer according to one of the preceding claims,

- wherein the measuring tube has an inlet-side first straight tube segment with a pointing in the direction of the first coupling zone directional vector (a1) imaginary longitudinal axis and an outlet-side second straight tube segment with a in the direction of the second

Has imaginary directional vector (a2) having imaginary longitudinal axis, and

- Wherein the two straight tube segments, esp. To form an at least partially substantially V-shaped or U-shaped measuring tube, are aligned with each other so that the directional vector (a1) of the imaginary longitudinal axis of the first straight tube segment and the directional vector (a2) of imaginary longitudinal axis of the second straight pipe segment an angle (Θ) include, esp., So that the angle (Θ) is less than 170 ° and more than 10 °.

9. A transducer according to the preceding claim, wherein the measuring tube is shaped so that the angle (Θ) is less than 170 °, esp. Less than 160 °, and / or more than 10 °, esp. More than 20 °.

10. A transducer according to claim 8 or 9, wherein the measuring tube is shaped so that the angle (Θ) is less than 100 °.

11. A transducer according to the preceding claim, wherein the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition ξ <0.6 satisfied.

12. A transducer according to the preceding claim, wherein the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition ξ> 0.35 satisfied.

13. A transducer according to the preceding claim, wherein the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition : Fulfills.

14. A transducer according to claim 8 or 9, wherein the measuring tube is shaped so that the angle (Θ) is more than 50 °.

15. A transducer according to claim 8 or 9, wherein the measuring tube is shaped so that the angle (Θ) is more than 100 °, esp. More than 115 °.

16. A transducer according to the preceding claim, wherein the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition ξ <0.62 fulfilled.

17. A transducer according to the preceding claim, wherein the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition ξ> 0.45 fulfilled.

18. A transducer according to any one of claims 8 to 17, wherein the two straight pipe segments by means of an arcuate, esp. Circular arc, pipe segment are interconnected.

19. Transducer according to the preceding claim, wherein

- The arcuate tube segment measured from the center line of the middle

Pipe bend radius (R) which is less than 500 mm, in particular less than 300 mm, and

- The measuring tube has a tube wall thickness (s), which is less than 7 mm, esp. Less than 3 mm.

20. A transducer according to claim 19 in conjunction with claim 4 or one dependent therefrom, wherein the first measuring tube dimensioned and the vibration sensors are placed so that an area moment of inertia to Meßlänge ratio ho / L ₅ o of the transducer, defined by a Ratio of an area moment of inertia (I ₁₀ ) of a cross section of the measuring tube to the measuring length (L ₅₀ ) of the transducer, more than 40mm ³ , esp. More than 100mm ³ , wherein the area moment of inertia (I ₁₀ ) of the cross section of the measuring tube the condition

Iio = ^ r - ko "(D ₁₀ + s) ⁴ ].

o4

21. A transducer according to the preceding claim, wherein the first measuring tube is dimensioned so that the nämliches area moment of inertia (I ₁₀ ) of the measuring tube at least 40mm ⁴ , esp. More than 150mm ⁴ , is.

22. A transducer according to claim 19 in conjunction with claim 4 or a dependent claim,

- wherein the first vibration sensor of the sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge-to-Schwinglänge- ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the vibration length ( L ₁₀ ), less than 0.65, and

- Wherein the arcuate pipe segment is formed so that its pipe bend radius (R) the

0.5 - D _1n + s

Condition: R <- satisfied.

23. A transducer according to claim 19 in conjunction with claim 4 or a dependent claim,

- wherein the arcuate tube segment is formed so that a Rohrbogenradius to Rohraußenradius ratio (R '), defined by a ratio of the pipe bend radius (R) by a tube outer radius (r) of the arcuate tube segment, less than 60, esp. Less than 50, and / or more than 3, esp. More than 4, is, and

wherein the first vibration sensor of the sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer such that a measuring length-to-vibration length Ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ) satisfying the condition ξ≤- + 0.4.

24. A transducer according to the preceding claim, wherein the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that a Meßlänge to swing length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition ξ> 0.4 satisfied.

25. A transducer according to claim 19 in conjunction with claim 4 or a dependent claim,

- wherein the arcuate pipe segment is formed so that a Rohrbogenradius-to-Rohraßenradius ratio (R '), defined by a ratio of the pipe bend radius (R) by a pipe outer radius (r) of the arcuate pipe segment, the condition R' <fulfilled.

ξ - 0.4

26. A transducer according to claim 19 in conjunction with claim 4 or a dependent claim, wherein the arcuate tube segment is formed as well as the first

Vibration sensor of the sensor arrangement and the second vibration sensor of the

Sensor arrangement are placed in the transducer so that a Meßlänge-to-oscillating length ratio, ξ = L ₅₀ / L ₁₀ , defined by a ratio of the measuring length (L ₅₀ ) to the oscillating length (L ₁₀ ), the condition ξ <° - ⁵ - P " ^{+ S} ₊ 0.4 met.

27. A transducer according to the preceding claim, wherein the first vibration sensor of

28. A transducer according to claim 19 in conjunction with claim 4 or a dependent claim, wherein the measuring tube is formed and the first vibration sensor of

Sensor arrangement and the second vibration sensor of the sensor arrangement are placed in the transducer so that the transducer fulfills the condition - • - h 0.4> 1.

L ₅₀ v RJ

29. A transducer according to the preceding claim, wherein the measuring tube is formed as well as the first vibration sensor of the sensor arrangement and the second vibration sensor of

Sensor arrangement are placed in the transducer so that the transducer fulfills the condition--> 0.35.

30. Transducer according to one of the preceding claims, wherein the first vibration sensor and the second vibration sensor are identical to each other.

31. A transducer according to one of the preceding claims, further comprising a formation of a first coupling zone inlet side of the measuring tube and to form a second

Coupling zone on the outlet side fixed to the measuring tube, esp. In operation substantially in opposite phase to the measuring tube oscillating and / or parallel to this, counter-oscillator, wherein the first coupling zone define an inlet-side first end of the measuring tube and the second coupling zone an outlet-side second end of the measuring tube.

32. A transducer according to the preceding claim, wherein both the first vibration sensor and the second vibration sensor are placed in the transducer so that each of

Vibration sensors, in particular predominantly or exclusively, vibrations of the measuring tube relative to the counteroscillator, esp. Differentially capture.

33. A transducer according to any one of claims 31 to 32,

- Measuring tube and counteroscillator in operation at least on a common

Oscillation frequency oscillate to each other in opposite phases; and or

- Wherein both the first primary signal (si) and the second primary signal (S ₂ ), esp.

gegengleiche, oscillatory movements of the at least one measuring tube relative to

Represent backswing.

34. A transducer according to any one of claims 31 to 33, wherein the, esp.

Vibration sensors of the at least one, esp. U- or V-shaped, measuring tube and, esp. U- or V-shaped counter-oscillator, esp., Simultaneous and / or differentially detect.

35. A transducer according to one of the preceding claims, wherein the first vibration sensor equidistant from a center of the measuring tube is placed in the transducer, as the second vibration sensor.

36. A transducer according to one of the preceding claims, comprising two to form a first coupling zone inlet side by means of a, esp. Plate-shaped, first coupler element and the formation of a second coupling zone on the outlet side by means of a, esp. Plate-shaped, second Coupler element mechanically interconnected, esp. In operation substantially in phase opposition to each other and / or mutually parallel and / or identical in terms of shape and material, measuring tubes, wherein the first coupling zone in each case an inlet-side first end of each of the measuring tube and the second coupling zone in each case an outlet-side second Define end of each of the measuring tubes.

37. A transducer according to the preceding claim, wherein each of the two measuring tubes respectively communicates on the inlet side with a first distributor element of the measuring transducer and on the outlet side with a second distributor element of the measuring transducer.

38. A transducer according to claim 36 or 37,

- Wherein the two measuring tubes oscillate in phase opposition to each other at least on a common oscillation frequency; and or

- Wherein both the first vibration sensor (51) supplied first primary signal (si) of the transducer and the second vibration sensor (51) supplied second primary signal (si) of the transducer oscillations of the measuring tubes (10) relative to each other, in particular to each other in anti-phase oscillations Measuring tubes, represent.

39. A transducer according to one of the preceding claims, further comprising at least one, esp. Exactly one, in operation, esp. In a range of half the oscillation length (L ₁₀ ), acting on the measuring tube, esp. Electrodynamic, vibration exciter (41) having

Exciter arrangement (40) for vibrating the at least one measuring tube (10), esp. In a bending vibration mode in which it performs at least partially bending vibrations about the imaginary axis of vibration.

40. A transducer according to the preceding claim, wherein the at least one measuring tube is excited in operation by means of the exciter arrangement at least temporarily in a Nutzmode in which it, esp.

predominantly or exclusively, bending oscillations around the imaginary axis of vibration, esp. With a single and / or with a lowest resonant frequency of the measuring tube, performs.

41. A transducer according to the preceding claim, wherein each of the, in particular simultaneously generated, primary signals of the transducer in each case one, esp. Dominant and / or corresponding with the Nutzmode, signal component with a bending vibrations in Nutzmode and / or one, esp. Has resonant frequency of at least one measuring tube corresponding signal frequency.

42. A transducer according to any one of claims 39 to 41, wherein the first vibration sensor equidistant from the at least one vibration exciter spaced in the transducer is placed as the second vibration sensor.

43. A transducer according to one of the preceding claims, wherein the measuring tube made of metal, esp.

Stainless steel, titanium, tantalum, or zirconium.

44. Transducer according to one of the preceding claims, wherein the sensor arrangement has no further vibration sensors except the first and second vibration sensor.

45. A transducer according to one of the preceding claims, wherein the length of the extending between the first vibration sensor and the second vibration sensor portion of the first measuring tube corresponding Meßlänge (L ₅₀ ) of the transducer less than 65%, esp. Less than 55% and / or more as 25%, the oscillation length (L ₁₀ ) of the oscillation length (L ₁₀ ) corresponds.

46. Measuring device, esp. A compact meter and / or a Coriolis mass flow meter, for flowable, esp. Fluid, media, which meter a transducer according to one of the preceding claims and a device electrically coupled with namely Meßelektronik electronics for processing of primary signals supplied by the transducer and for generating measured values.

47. A meter according to the preceding claim, wherein the meter electronics at least temporarily both by means of the first primary signal (S ₁ ) and by means of the second primary signal (S ₂ ), esp. Based on a between the first primary signal (S ₁ ) and the second primary signal (S ₂ ) existing phase difference, a, esp. Digital, mass flow rate measurement (X _m ) is generated, which represents a mass flow rate, m, of flowing medium through the transducer currently.

48. Measuring device according to claim 46 or 47, wherein the measuring device electronics in operation recurrently generates a phase difference value (X ' _Δφ ), which between the first primary signal (S ₁ ) and the second primary signal (S ₂ ) existing phase difference, Δφi, currently represents.

49. Measuring device according to one of claims 46 to 48, further comprising a, in particular in operation with the evaluation circuit communicating with the transducer electrically coupled, at least one of whose exciter device controlling exciter signal supplying driver circuit.

50. Measuring device according to one of claims 46 to 49, wherein the measuring device electronics by means of a, in particular., As 4-20 mA current loop formed, two-wire connection (2L) with an external electronic data processing system is electrically connected.

51. Measuring device according to one of claims 46 to 50, wherein the evaluation circuit at least temporarily by means of at least one of the primary signals (S ₁ , S ₂ ), a, esp. Digital, density measured value (X _p ) currently representing a density, p, of medium flowing through the transducer.

52. Measuring device according to one of claims 46 to 51, wherein the evaluation circuit at least temporarily by means of at least one of the primary signals (si, S ₂ ), one, esp. Digital, viscosity measured value (X _η ) generated, the viscosity, 77 , represented by medium flowing through the transducer.

53. Use of a measuring device according to one of claims 46 to 52 for measuring a mass flow rate and / or a density and / or a viscosity and / or a pressure of a medium flowing in a process line.