GB1586417A

GB1586417A – Method of and apparatus for the inductive measurment of fluid flow
– Google Patents

GB1586417A – Method of and apparatus for the inductive measurment of fluid flow
– Google Patents
Method of and apparatus for the inductive measurment of fluid flow

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Publication number
GB1586417A

GB1586417A
GB23515/78A
GB2351578A
GB1586417A
GB 1586417 A
GB1586417 A
GB 1586417A
GB 23515/78 A
GB23515/78 A
GB 23515/78A
GB 2351578 A
GB2351578 A
GB 2351578A
GB 1586417 A
GB1586417 A
GB 1586417A
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GB
United Kingdom
Prior art keywords
magnetic field
voltage
compensation
time interval
amplifier
Prior art date
1977-10-05
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)

Expired

Application number
GB23515/78A
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)

Endress and Hauser Flowtec AG

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Flowtec AG
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
1977-10-05
Filing date
1978-05-26
Publication date
1981-03-18

1978-05-26
Application filed by Flowtec AG
filed
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Flowtec AG

1981-03-18
Publication of GB1586417A
publication
Critical
patent/GB1586417A/en

Status
Expired
legal-status
Critical
Current

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Classifications

G—PHYSICS

G01—MEASURING; TESTING

G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME

G01F1/00—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow

G01F1/56—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects

G01F1/58—Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters

G01F1/60—Circuits therefor

Description

PATENT SPECIFICATION
( 21) Application No 23515/78 ( 22) Filed 26 May 1978 ( 31) Convention Application No 2744845 ( 32) Filed 5 Oc / A ( 35) ( 44) Fed Rep of Germany (DE) Complete Specification Published 18 Mar 1981 ( 51) INT CL 3 ( 52) ( 11) 1 586 417 ( 19) t 1977 in GOIF 1/60 Index at Acceptance Gi N 19 A 3 19 F 7 B 19 H 2 A ( 54) IMPROVED METHOD OF AND APPARATUS FOR THE INDUCTIVE MEASUREMENT OF FLUID FLOW ( 71) We, FLOWTEC AG, a Swiss company of Sternenhofstrasse 21 a, 4153 Reinach BL 1, Switzerland, do hereby declare the invention, for which we pray that a patent may be granted to us, and the method by which it is to be performed, to be particularly described in and by the follow-
ing statement:-
This invention relates to a method for inductive measurement of fluid flow using a periodically reversed magnetic field, in which the work signal is derived by sampling and holding the signal voltage at equal but oppositely poled values of induction of magnetic field and the difference between the stored sample values is formed The invention also relates to apparatus for carrying out this measurement.
In magnetic induction fluid flow measurements there exists the problem that the measured voltage denotive of the fluid flow has superimposed upon it a disturbing direct voltage (asymmetric voltage), which has its origin in different electro-chemical equilibrium potentials The disturbing voltage may attain values which are substantially greater than the measured voltage.
In addition there may also be superimposed upon the measured voltage alternating current components which originate from the mains and have frequencies which correspond to the mains frequency or its harmonics.
In the known methods of the kind initially described the magnetic field is periodically changed between two equal values of induction of opposite signs Use is made of the fact that the measured voltage changes its polarity with the magnetic field while the asymmetrical voltage retains its polarity.
There is thus attained by sampling at the one induction value the sum of the measured and asymmetrical voltage and by sampling at the other induction value the difference of the asymmetrical voltage minus the measured voltage From the difference between the two stored sampling values there is thus obtained a measurement signal free from asymmetrical voltages This method however makes the assumption that the asymmetrical voltage does not alter within the measurement cycle, since otherwise the alteration appears as an error in measurement In addition the asymmetrical voltage must not assume too large a value, since otherwise the linear range of the measurement amplifier may be exceeded.
Also for large values of the asymmetrical voltage great demands are made on the accuracy of the difference-forming circuits, since any error directly affects the measured value obtained as the difference.
It is also known, instead of a magnetic field reversed between two opposite values of induction to employ a unidirectional field periodically turned on and off In this case with the magnetic field switched off the asymmetrical voltage is sampled and stored and with the magnetic field turned on the sum of the measurement and asymmetrical voltages is likewise sampled and stored.
The invention is directed to providing a method with which the electro-chemical disturbing voltages in the inductive measurement of fluid flow may be automatically compensated in a simple manner and at little cost, if they alter within the measurement cycle in which no electro-chemical voltages are formed with the fluid stationary and in which over-driving of the amplifier by too-large an asymmetrical voltage is prevented.
Accordingly the method of the invention comprises, forming between each two successive magnetic field impulses of opposite polarity an interval in which the magnetic field is zero, generating in a compensating time interval in each magnetic field interval at a constant time interval preceding the next sampling of the signal voltage a 1 586 417 compensation voltage which reduces to zero the signal voltage in the compensating time interval, the compensating value voltage generated in the compensating time interval being stored and employed up to the next compensation time interval.
The method according to the invention depends on the fact that a time variant asymmetrical voltage, if a linear alteration is assumed, starting from the value zero at the end of the compensation time interval always assumes the same value by the time the next sampling interval is reached The signal voltages sampled in cyclic succession for the opposed values of induction thus always contain the same component of asymmetrical voltage, which is eliminated when the difference between the two signals is formed.
Since in addition the asymmetrical voltage does not attain excessive values between two compensation time intervals, which are separated by a time interval which corresponds to half of the measuring cycle, no over-driving of the amplifier through the asymmetrical voltage can occur Since in the method according to the invention periodic reversal of the magnetic field is employed, the advantage is retained that with stationary fluids no electro-chemical voltages are formed, as is the case when a wholly unidirectional field is employed or when a unidirectional field is switched on and off.
Since in addition the component of the asymmetrical voltage in each sampled value is small as compared with the measurement voltage component, the forming of the difference between successive signals requires only limited accuracy.
A further substantial advantage of the method according to the invention consists in that for the same sensitivity, a lower power consumption is required in comparison to the known method with reversed unidirectional feel or a unidirectional field which is switched on and off, because of the intervals in which the magnetic field is zero.
Apparatus according to the invention for inductive flow measurement of an electrically conductive fluid flowing in a pipe, includes a magnetic field generator which generates a periodically reversed magnetic field passing through the pipe perpendicular to, the direction of flow, two electrodes arranged within the pipe which are connected with signal inputs of a measuring amplifier, sample and hold circuits which are connected to the output of the mcasuring amplifier and which are controlled by a control arrangement so that they sample the output voltage of the measuring amplifier at mutually equal values of induction in opposite polarity, and store the sample values until the next sampling, and a circuit arrangement for forming the difference of the two stored induction values and wherein the magnetic field generator is so controlled that between any two successive magnetic field impulses of opposite polarity there exists an interval in which the induction is zero, and that a compensation input of the measuring amplifier is connected with the output of a storage control circuit which, during compensation time intervals each occurring at a constant time interval before the next subsequent sampling of the signal voltage is connected with the output of the measuring amplifier so as to form a compensating voltage value which controls the output voltage of the measuring amplifier to the value zero and which maintains this compensation voltage value at the compensation input of the measuring amplifier until the next compensation time interval.
An advantageous extension of the arrangement according to the invention consists in that the control circuit forms the compensation voltage value by integration of the output voltage of the measuring amplifier existing in the compensation time interval, and that the duration of the compensation time interval is equal to one period of the mains frequency of a multiple thereof This extension allows the disturbing alternating components of the mains frequency or one of its harmonics, as well as in case of need also alternating components of which the frequency is a fraction of the mains frequency, to be automatically eliminated Preferred features and advantages of the invention will be apparent from the following description of embodiment thereof, given with reference to the accompanying drawings in which:
Figure 1 shows a schematic general view of an arrangement for inductive fluid flow measurement in accordance with one invention:
Figure 2 shows a simplified block diagram of the controlled arrangements for the magnetic field coil of the arrangement of
Figure 1; Figure 3 shows the block diagram of the signal processing arrangement of the arrangement of Figure 1 l Figure 4 comprises waveform diagrams used to explain the mode of operation of the arrangement for Figures 1 to 3; and Figure 5 shows diagrams to a larger time-scale for explaining the mode of operation of the arrangement according to the invention.
Figure 1 shows schematically a pipe 1, through which an electrically conductive fluid flows perpendicular to the plane of the drawing A magnetic field coil 2, which for reasons of symmetrv consist of two equal halves arranged on either side of the pipe 1, generate within the pipe a magnetic field
B 1 B 2 passing perpendicularly to the axis of 1 586 417 the pipe Within the pipe 1 there are arranged two electrodes 3 and 4, at which an induced voltage can be tapped off, which is proportional to the mean velocity of flow of the electrically conductive fluid through the magnetic field The electrodes 3 and 4 are connected with the two inputs 5 and 6 respectively of a signal processing arrangement 7, which provides at its output 8 a signal appropriate for further processing, which is a measure of the velocity of flow.
The signal processing and control arrangement provides at two further outputs 9 and control signals which are applied to the two inputs 11 and 12 of a coil drive arrangement 13 The two coil halves 2 are connected in series to the outputs 14 and 15 of the coil drive arrangement 13.
One embodiment of the coil drive arrangement 13 is shown schematically in Figure 2 It contains four switches 16, 17, 18, 19 which are connected after the manner of a bridge circuit, the magnetic coil 2 lying in a bridge diagonal, while the other bridge diagonal is connected in series with a constant current generator 20 to a direct voltage source 21 The direct voltage source 21, which may for example provide a voltage of 24 volts, can either be a mains-fed unit or a battery.
The switches 16 to 19 which in practice are naturally electronic switches, are actuated in diagonally opposed pairs by signals applied to the input terminals 11 and 12.
If an impulse is applied to input 11 the two switches 16 and 18 are closed which lie in diametrically opposed branches of the bridge: in this case the current I delivered by the constant current generator 20 flows in the direction of the arrow Bl through the magnetic coil 2 so that this generates within the tube 1 a magnetic field Bl of which the direction is indicated in Figure 1 by the arrows shown in full line If an impulse is applied to input 12 the two switches 17 and 19 are closed so that the current I applied to the bridge circuit flows in the opposite direction through the magnetic coils 2 as is indicated by the broken-line arrow B 2: as a result the magnetic field B 2 generated in the pipe 1 has the direction indicated by the broken-line arrow The inductions Bl and B 2 have the same value but are of opposite signs When an impulse is applied to neither of the inputs 11 and 12 all the switches are opened and the magnetic field in the pipe 1 has zero induction value.
Figure 3 shows a more detailed circuit diagram of the signal processing and control arrangement 7 of Figure 1 The two input terminals 5 and 6 are the inputs of a measuring amplifier 22 constructed as a difference amplifier to which the signal voltage arising between the electrodes 3 and 4 is thus applied To the output of the measuring amplifier 22 there are connected two sample and hold circuits 23 and 24, the sample and hold circuit 23 being connected directly and the sample and hold circuit 24 by way of an inverter 25, which inverts the polarity of the output signal of the measuring amplifier 22 For simplicity it is indicated that the sample and hold circuit 23 contains a switch 51, which is closed by a signal applied to a control input 26 and then connects a storage capacitor Cl by way of a resistance R 1 with the output of the measuring amplifier 22, so that the storage capacitor Cl charges to a voltage which depends upon the output voltage of the measuring amplifier 22 The circuit elements Ri, Cl together form an integrating circuit, that integrates the output voltage of the measuring amplifier 22 during the time of closure of the switch 51 The output of the sample and hold circuit 23 is connected with the input of a buffer amplifier 28, which prevents the capacitor Cl from being discharged after the opening of the switch 51; the sampled voltage stored on the capacitor Cl thus remains available at the output of the buffer amplifier 28 until the next closure of the switch 51.
In the same manner the sample and hold circuit 23 contains a switch 52, which is closed by a control signal applied to a control input 27, as well as a storage capacitor C 2, which together with a resistance R 2 forms an integrating circuit, that integrates the output voltage of the inverter during the time of closure of the switch 52 The charging voltage on the capacitor C 2 attained after the opening of the switch 52 remains available at the output of a buffer amplifier 29 connected to the output of the sample and hold circuit 24 until the next closure of the switch 52.
The outputs of the two buffer amplifiers 28 and 29 are connected by way of summing resistances 30 and 31 respectively with the inverting input of an operational amplifier operating as a summing amplifier, in the negative feedback circuit of which there is connected a resistor 33 in parallel with a capacitor 34 The output of the operational amplifier 32 corresponds to the output 8 of the signal processing and control arrangement 7.
The measuring amplifier 22 includes an additional compensation input 35 which is connected to the output of a storing control circuit 36 As an example it is indicated that the storing control circuit may contain an operational amplifier 37 which by means of a capacitor 38 in the ne-ative feedback circuit in conjunction with an input resistor 39 is connected as an integrator The noninverting input of the operational amplifier 37 acting as a reference input is connected to earth The input resistance 39 is con-95 1 586 417 nected in series with a switch 53 to the output of the measuring amplifier 22 It may thus be seen that if the switch 53 is closed the operational amplifier 37, develops an output voltage which is applied to the compensating input 35 of the measuring amplifier 22 and has a value such that the output voltage of the measuring amplifier 22 is controlled to the value zero When the switch 53 is open the operational amplifier 37 retains the compensation voltage value developed until the next closure of the switch 53.
A control circuit 41 controlled by a clock 40 provides at three outputs the control signals for the switches 51 i, 52, 53; two further outputs of the control circuit 41 correspond to the output 9 and 10 of Figure 1 at which there are provided the control circuits for the coil drive arrangements 13.
If the described arrangement is fed from the main, the clock 40 may have a synchronizing input 42 through which it may be synchronized bv the main supply This synchronizing arrangement may be omitted in a batterv-driven apparatus.
The mode of operation of the above described circuit will be explained with reference to Figures 4 and 5.
Diagram A of Figure 4 shows the controlled impulses at the output 9 and diagram B shows the control impulses at the output 10 of the signal processor 7 of Figure 1.
Because of the above-described mode of operation of the coil drive arrangement 13 (Figure 2) the magnetic field in pipe 1 thus assumes alternately the induction values B 1, and B 2 represented in diagram C of the Figure 4 between which there exists an interval in which the magnetic field has the induction value zero The period which is equal to the duration Tl of a measuring cycle is large compared with the period of the mains frequency: the signals may be obtained for example from the mains frequency by digital frequency division by the dividing factor 32 so that for a mains frequency of 50 Hz the measuring cycle has duration T\ 1 of 640 ms: this corresponds to a frequency of field generation of 1 5625 Hz.
In the illustrated example it is assumed that in each period the two magnetic field impulses as well as the intervals lying therebetween all have the same duration.
which in the above-given numerical example thus amounts to 160 ms.
The diagrams 51 52 and 53 illustrate the control impulses which are provided by the control circuit 41 for actuation of the switches SI 52 and 53 respectively of Figure 3.
The control impulses are substantially shorter than the control impulses of diagralms A and B generated for controlling the maognetic field and in consequence also substantial-
1 v shorter than the magnetic field impulses generated by the magnet coil 2 Preferably.
the duration of the sample control impulses 51 52 and the compensation control impulse 53 are similar in relation to the period of the mains voltage; in a preferred embodiment they amount for example to 40 ms, that is to twice the mains period For clarity diagram A of Figure 5 shows in a larger time-scale, the mutual timings of the magnetic field impulses B 1, B 2 and control impulses 51, 52, 53 for one period The sampling control impulses 51 fall within the positive magnetic field impulse Bl and the sampling control impulses 52 fall within the negative magnetic field impulses B 2 They preferably lie in the region of the trailing end of these impulses, so that relations have become stationary in the sampling time interval and possible initial oscillatory processes have subsided In the above-given numerical example each sampling control impulse 51 i 52 may commence at a time interval 100 ms after the beginning of the corresponding magnetic field impulse Bl or
B 2 so that it ends 20 ms before the end of the magnetic field impulse.
The compensation control impulses 53 fall within the intervals between each two successive magnetic field impulses They begin for example likewise at a time interval of 100 ms after the end of the preceding magnetic field impulse so that after the end of each compensation control impulse 53 there remains time interval of 20 ms before the beginning of the succeeding magnetic field impulse Between the end of each compensation control impulse 53 and the beginning of the next sampling control impulse 51 52 there thus exists always the same time interval of 120 ms.
Diagrams B of Figure 4 shows the wave form of the signal voltage obtained by the super position of disturbing direct voltage Us and measurement voltage U N for the case of a disturbing direct voltage Us constant with time which is assumed to be smaller than the measurement voltage Us,.
In this diagram the sampling effected by the sampling pulses 51 52 is also indicated it being assumed that the compensation circuit with the storage control circuit 36 is not present Diagram E of Figure 4 shows under the same assumptions the relations for the case of a disturbing direct voltage Us varying with time Finally Figure 4 represents the mode of operation of the comnpensation circuit for the case corresponding to diagram E For the sake of clarity the diagrams D E and F for one cycle of measurement are shown to a larger scale in Figure 5.
In the case of diagram D there exists during intervals in the magnetic field a constant disturbing direct voltage Us upon which a positive-going measurement voltage 1 586 417 UM is superimposed during the positive magnetic field pulses B 1, and a negativegoing measurement voltage UM during the magnetic field pulses B 2 Since the sampling always relates to zero level, the value sampled during the sampling 51 is Us + UM and the value sampled during the sampling pulses 52 is Us UM As a result of the inversion by the inverter 25 and the subsequent summing operation, the difference of the two sampled alues is formed:
US + UM (US UM) = 2 UM.
The disturbing direct voltage Us is thus eliminated by this difference formation.
If, on the other hand, the disturbing direct voltage Us alters with time, as is illustrated in diagram E, complete compensation of the disturbing direct voltage by differencing is no longer possible During sampling by the sampling pulses 51 a disturbing direct voltage Us, is present, so that the sampled value Us, + UM is stored.
During sampling by the sampling pulses 52 the disturbing direct voltage has increased by the amount A Us; the sampled values Us + A Us UM is thus stored The ensuing formation of the difference thus yields:
Us, + UM (US, + A Us UM) = 2 UM A Us.
The measurement is also affected by an error, which is equal to the alterations A Us of the disturbing direct voltage between the two successive samplings Diagram E of Figure 4 also allows a further disadvantageous consequence of the varying disturbing voltage to be recognised: the sum of the disturbing direct voltage and the measurement voltage can rapidly assume very large values, which exceed the linear modulation range of the measuring amplifier When this occurs measurement is no longer possible If in addition the disturbing direct is large compared with the measurement voltage, errors in the formation of the difference very greatly affect the accuracy of the measurement results obtained.
Diagram F of Figure 4 and 5 show how the phenomena described above may be avoided by the operation of the storing control circuit 36 in combination with the particular kind of field drive employed.
Each compensation control impulse 53 causes the output voltage of the measurement amplifier 22 to be regulated to zero during a compensation time interval TK which occurs shortly before the beginning of each magnetic field impulse Since this regulation is effected during the intervals in the magnetic field, it operates only on the disturbing direct voltage existing at this point in time After the end of the compensation time interval TK the disturbing direct voltage then alters in accordance with the conditions prevailing, starting from the value zero At sampling by the sampling pulse 51 it has attained a certain value A Us.
Thus in this sampling time interval the sample value A Us + UM is sampled and stored.
Before the subsequent negative magnetic field impulse B 2 the output voltage of the measurement amplifier 22 is again controlled to zero during a compensation time interval Ti<. Thereafter it rises again, starting from this value zero If a constant linear alteration of the disturbing direct voltage is assumed, it again attains the same value A Us at the time of sampling by the sampling control impulse 52 so that in this sampling time interval the sample value A Us UM is sampled and stored The subsequent formation of the difference between the sampled values then gives: Us + UM (AUS UM) = 2 UM it may thus be seen that the disturbing direct voltage is completely compensated; although it alters with time. It is also to be seen that the disturbing direct voltage can always have only a small value, since it is returned to zero value during each half of the measuring cycle, from which it may be perceived that it does not alter greatly in this space of time There is thus no danger of over-driving of the measurement amplifier. Finally, the disturbing direct voltage A Us to be eliminated at each formation of a signal difference always remains small in relation to the measurement voltage UM so that accuracy of the difference formation affects the accuracy of measurement only insignificantly. Because the signals sampled by the control impulses 51, 52 and 53 are always integrated over the duration of a time interval of 40 ms, that is equal to two periods of the mains frequency, the superimposed disturbing frequencies, which are a multiple of half the mains frequency ( 25 Hz), are made ineffective, since their direct current mean value is zero for the sampled signal. The choice of the very low working frequency, which is only a fraction of the mains frequency and in the example given is 1.5625 Hz for a mains frequency of 50 Hz. yields several advantages On the one hand there is, between the turning of the coil current and the sampling of the signal voltage sufficient time for initial oscillations to decay and steady conditions to result On the other hand, at such low frequencies the coils may be regarded as practically pure resistances, so that no large amount of l 20 l 25 1 586 417 reactive power is necessary. The coil currents and the magnetic fields generated by them have for simplicity been illustrated as rectangular impulses The described method is however, independent of the waveform of the coil currents and magnetic fields Even with rectangular drive pulses, because of the self-inductance of the coils, in general a more trapezoidal wave form of the coil currents will result. Claims (7) WHAT WE CLAIM IS: 1 A method for inductive flow measurement using a periodically reversed magnetic field, in which the useful signal is obtained by sampling and storing the signal voltage at equal but opposite values of induction of magnetic field and forming the difference of the stored sample values, wherein there is formed between each two successive magnetic field impulses of opposite polarity an interval of which the magnetic field is zero there being generated in a compensation time interval within each magnetic field interval at a constant timeinterval before the next subsequent sam pling of the signal voltage a compensation voltage which restores the signal voltage during the compensation time interval to zero value and that the compensation voltage value developed during the compensation time interval is stored and is employed until the next compensation time interval. 2 Apparatus for inductive flow measurement of an electrically conductive fluid flowing in a pipe including a magnetic field generator which generates a periodically reversed magnetic field passing through the pipe perpendicular to the direction of flow. two electrodes arranged within the pipe. which are connected with signal inputs of a measuring amplifier sample and hold circuits which are connected to the output of the measuring amplifier and are controlled bv a control device so that thev sample the output voltage of the measurement amplifier at mutually equal values of induction in opposite polarity, and store the sample values until the next sampling, and a circuit arrangement for forming the difference of the two stores induction values and wherein the magnetic field generator is so controlled that between anv two successive macnetic field impulses of opposite polaritv there exists an interval in which the induction value is zero and that a compensation input of the measuring amplifier is connected with the output of a storage control circuit which. during compensation time intervals each occurring at a constant timc-interval before the next subsequent sampling of the signal voltage is connected with the output of the measurement amplifier, so as to form a compensation voltace value which restores the output voltage of the measurement amplifier to the value zero and maintains this compensation voltage value at the compensation input of the measurement amplifier until the next compensation time interval. 3 Apparatus in accordance with claim 2, wherein the control circuit forms the compensation voltage value by integration of the output voltage of a measurement amplifier existing during the compensation time interval, and that the duration of the compensation time interval is equal to one period of the mains frequency or to a multiple thereof. 4 Arrangement in accordance with claim 2 or claim 3, wherein each sample and hold circuit forms the stored sampled value by integration of the output voltage of the masurement amplifier existing during a sampling time interval and that the duration of each sampling time interval is equal to one period of the mains frequency or to a multiple thereof. Apparatus in accordance with any one of claims 2 to 4, wherein the magnetic field generator contains a magnetic field which is connected in a diagonal of a bridge circuit contains a switch in each bridge branch the other bridge diagonal being connected to a constant current source and a control arrangement being arranged alternatelv to close two switches arranged in diametrically opposite bridge branches, and that all the switches are opened in intervening intervals. 6 A method of fluid flow measurement substantially as herein described with reference to the accompanying drawings. 7 Apparatus for fluid flow measurement substantially as herein described with reference to Figures 1 2 and 3 of the accompanying drawings. A.A THORNTON & CO Chartered Patent Agents. Northumberland House. 303/306 High Holborn. London WC 1 V 7 LE. Printed for Her Majesty's Stationery Office, by Croydon Printing Company Limited Croydon Surrey 1981. Published by The Patent Office 25 Southampton Buildings. London WC 2 A l AY, from which copies may be obtained. GB23515/78A 1977-10-05 1978-05-26 Method of and apparatus for the inductive measurment of fluid flow Expired GB1586417A (en) Applications Claiming Priority (1) Application Number Priority Date Filing Date Title DE2744845A DE2744845C3 (en) 1977-10-05 1977-10-05 Process for the compensation of the electrochemical disturbance direct voltage in the magneto-inductive flow measurement with periodically reversed magnetic field Publications (1) Publication Number Publication Date GB1586417A true GB1586417A (en) 1981-03-18 Family ID=6020735 Family Applications (1) Application Number Title Priority Date Filing Date GB23515/78A Expired GB1586417A (en) 1977-10-05 1978-05-26 Method of and apparatus for the inductive measurment of fluid flow Country Status (10) Country Link US (1) US4210022A (en) JP (1) JPS5489658A (en) BE (1) BE870876A (en) CH (1) CH634408A5 (en) DD (1) DD139762A5 (en) DE (1) DE2744845C3 (en) FR (1) FR2405466A1 (en) GB (1) GB1586417A (en) IT (1) IT1099763B (en) NL (1) NL7809681A (en) Cited By (4) * Cited by examiner, † Cited by third party Publication number Priority date Publication date Assignee Title GB2127978A (en) * 1982-09-30 1984-04-18 Tokyo Shibaura Electric Co Electromagnetic flow meter GB2203843A (en) * 1987-03-28 1988-10-26 Diessel Gmbh & Co Means for amplifying timed electrical measuring signals GB2400179A (en) * 2003-04-02 2004-10-06 Abb Ltd Electromagnetic flowmeter US6962087B2 (en) 2003-04-02 2005-11-08 Abb Limited Electromagnetic flow meter Families Citing this family (34) * Cited by examiner, † Cited by third party Publication number Priority date Publication date Assignee Title US4409846A (en) * 1979-02-08 1983-10-18 Aichi Tokei Denki Co., Ltd. Electromagnetic flow meter US4262543A (en) * 1979-10-09 1981-04-21 Emerson Electric Co. Magnetic flowmeter having multiple stage amplifier with automatic zeroing DE3029791C3 (en) * 1980-08-06 1994-08-04 Aichi Tokei Denki Kk Electromagnetic flow meter US4382387A (en) * 1980-10-02 1983-05-10 Flowtec Ag Method of compensating the interference DC voltages in the electrode circuit in magnetic-conductive flow measurement DE3037305C2 (en) * 1980-10-02 1986-04-03 Flowtec AG, Reinach, Basel Arrangement for generating constant magnetic fields of alternating polarity for magnetic-inductive flow measurement DE3132471C2 (en) * 1980-10-02 1984-11-29 Flowtec AG, Reinach, Basel Method and arrangement for the compensation of the interference DC voltages in the electrode circuit in the magnetic-inductive flow measurement JPH039090Y2 (en) * 1981-04-07 1991-03-07 JPS57166514A (en) * 1981-04-08 1982-10-14 Yokogawa Hokushin Electric Corp Electromagnetic flowmeter DE3133330C2 (en) * 1981-08-22 1983-11-24 Eckardt Ag, 7000 Stuttgart Magnetic-inductive flow meter US4468971A (en) * 1982-07-16 1984-09-04 Fischer And Porter Company Ultrasonic flowmeter for clean and dirty fluids JPS5983016A (en) * 1982-11-04 1984-05-14 Fuji Electric Co Ltd Converter for low frequency exciting type electromagnetic flowmeter DE3314954A1 (en) * 1983-04-25 1984-10-25 Fischer & Porter GmbH, 3400 Göttingen CIRCUIT ARRANGEMENT FOR THE SUPPRESSION OF COMMUNICATION VOLTAGES AND ELECTRODE INTERFERENCE DC VOLTAGES IN THE EVALUATION OF MEASURED VALUE VOLTAGES THAT ARE OUTPUT BY MEASURING ELECTRODES OF AN INDUCTIVE FLOW MEASURING DEVICE DE3340330A1 (en) * 1983-11-08 1985-05-15 Flowtec AG, Reinach, Basel METHOD AND ARRANGEMENT FOR COMPENSATING AN ELECTRICAL SIGNAL THAT CHANGES NON-LINEAR JPS60242318A (en) * 1984-05-16 1985-12-02 Aichi Tokei Denki Co Ltd Remanent magnetism type electromagnetic flow meter DE3423076A1 (en) * 1984-06-22 1986-01-02 Bopp & Reuther Gmbh, 6800 Mannheim MAGNETIC-INDUCTIVE FLOW MEASUREMENT METHOD JPS6166123A (en) * 1984-09-07 1986-04-04 Toshiba Corp Converter of electromagnetic flowmeter CH668124A5 (en) * 1985-04-03 1988-11-30 Gas & Wassermesserfab Ag METHOD FOR INTERMITTENTLY MEASURING THE FLOW RATE OF A LIQUID BY MEANS OF AN INDUCTIVE FLOW CONVERTER AND DEVICE FOR CARRYING OUT THIS METHOD. DE3537752A1 (en) * 1985-10-23 1987-04-23 Flowtec Ag METHOD FOR COMPENSATING INTERFERENCE VOLTAGES IN THE ELECTRODE CIRCUIT IN MAGNETIC-INDUCTIVE FLOW MEASUREMENT FR2589571B1 (en) * 1985-10-31 1990-02-09 Sereg Soc ELECTROMAGNETIC FLOW METER WITH PULSE MAGNETIC FIELD GB2183343B (en) * 1985-11-25 1989-11-01 Danfoss As Electromagnetic flowmeters JP2514960B2 (en) * 1987-04-13 1996-07-10 愛知時計電機株式会社 Electromagnetic flow meter DE3728342A1 (en) * 1987-08-25 1989-03-09 Fischer & Porter Gmbh METHOD FOR GENERATING A SIGNAL THAT MEANS THE CURRENT STRENGTH OF A FLOWING, ELECTRICALLY CONDUCTIVE MEDIUM, AND CIRCUIT ARRANGEMENTS FOR IMPLEMENTING THE METHOD DE3815190A1 (en) * 1988-05-04 1989-11-16 Fischer & Porter Gmbh METHOD FOR COMPENSATING THE ELECTRIC VOLTAGE SENSING IN THE ELECTRODE CIRCUIT OF A MAGNETIC-INDUCTIVE FLOWMETER ARRANGEMENT, AND OFFSET VOLTAGE REPLACED BY THE ELECTRICITY CIRCUIT DE59106867D1 (en) * 1991-06-08 1995-12-14 Flowtec Ag Magnetic-inductive flow meter. LT3483B (en) 1993-05-21 1995-11-27 Juozapas Arvydas Virbalis Electromagnetic device for measuring of yield JP3602636B2 (en) * 1996-02-26 2004-12-15 愛知時計電機株式会社 Electromagnetic flow meter EP0814324B1 (en) * 1996-06-20 1999-08-18 Endress + Hauser Flowtec AG Instrumentation amplifier arrangements of electromagnetic flowmeters US5907103A (en) * 1996-06-20 1999-05-25 Endress + Hauser Flowtec Ag Instrumentation amplifier arrangements of electromagnetic flowmeters DE19938160C2 (en) * 1999-08-16 2003-11-20 Krohne Messtechnik Kg Magnetic-inductive flow measuring method and flow meter US6708569B2 (en) * 2001-07-06 2004-03-23 Endress + Hauser Flowtec Ag Method of operating an electromagnetic flowmeter DE10346409A1 (en) * 2003-10-07 2005-05-25 Abb Patent Gmbh Magnetic inductive fluid flow sensor uses operational amplifier impedance transformer DC output voltage to derive medium level and conductivity in measurement tube JP5163852B2 (en) * 2007-03-13 2013-03-13 横河電機株式会社 Electromagnetic flowmeter and its zero point measuring method JP5224886B2 (en) * 2008-04-14 2013-07-03 株式会社東芝 Electromagnetic flow meter US8434371B2 (en) 2010-10-14 2013-05-07 Brickhouse Innovations, Llc Electromagnetic fluid velocity sensor with adjustable electrodes Family Cites Families (8) * Cited by examiner, † Cited by third party Publication number Priority date Publication date Assignee Title US3316762A (en) * 1963-08-28 1967-05-02 Statham Instrument Inc Apparatus and process for measuring fluid flow US3550446A (en) * 1969-02-28 1970-12-29 Nat Res Dev Electromagnetic flowmeters DE2052175C3 (en) * 1970-10-23 1978-12-21 Karl Walter Prof. Dr.- Ing. 5910 Kreuztal Bonfig Process for the compensation of the electrochemical disturbance direct voltage in the inductive flow measurement with direct field or switched direct field US3783687A (en) * 1972-05-26 1974-01-08 Fischer & Porter Co Electromagnetic flowmeter with square-wave excitation JPS5439750B2 (en) 1973-03-05 1979-11-29 DE2410407C3 (en) * 1974-03-05 1981-05-21 Fa. Ludwig Krohne, 4100 Duisburg Method for the compensation of the electrochemical disturbance DC voltage in the inductive flow measurement with a DC field periodically switched back and forth between two induction values JPS5375966A (en) * 1976-12-15 1978-07-05 Hokushin Electric Works Electromagnetic flow meter US4144751A (en) * 1977-09-06 1979-03-20 Honeywell Inc. Square wave signal generator 1977 1977-10-05 DE DE2744845A patent/DE2744845C3/en not_active Expired 1978 1978-05-26 GB GB23515/78A patent/GB1586417A/en not_active Expired 1978-09-20 US US05/944,030 patent/US4210022A/en not_active Expired - Lifetime 1978-09-21 FR FR7827083A patent/FR2405466A1/en active Granted 1978-09-25 NL NL7809681A patent/NL7809681A/en not_active Application Discontinuation 1978-09-29 BE BE2057321A patent/BE870876A/en not_active IP Right Cessation 1978-09-29 DD DD78208203A patent/DD139762A5/en unknown 1978-10-04 CH CH1028978A patent/CH634408A5/en not_active IP Right Cessation 1978-10-05 JP JP12309878A patent/JPS5489658A/en active Granted 1978-10-05 IT IT7828477A patent/IT1099763B/en active Cited By (8) * Cited by examiner, † Cited by third party Publication number Priority date Publication date Assignee Title GB2127978A (en) * 1982-09-30 1984-04-18 Tokyo Shibaura Electric Co Electromagnetic flow meter US4545257A (en) * 1982-09-30 1985-10-08 Tokyo Shibaura Denki Kabushiki Kaisha Electromagnetic flow meter GB2203843A (en) * 1987-03-28 1988-10-26 Diessel Gmbh & Co Means for amplifying timed electrical measuring signals GB2203843B (en) * 1987-03-28 1991-09-18 Diessel Gmbh & Co An amplifier of consecutive alternate polarity electrical measuring signals GB2400179A (en) * 2003-04-02 2004-10-06 Abb Ltd Electromagnetic flowmeter US6962087B2 (en) 2003-04-02 2005-11-08 Abb Limited Electromagnetic flow meter US6973839B2 (en) 2003-04-02 2005-12-13 Abb Limited Electromagnetic flow meter having processing means resolving output data into a non-flow waveform component GB2400179B (en) * 2003-04-02 2006-08-09 Abb Ltd Electromagnetic flow meter Also Published As Publication number Publication date NL7809681A (en) 1979-04-09 JPS6250764B2 (en) 1987-10-27 DE2744845C3 (en) 1985-08-08 FR2405466A1 (en) 1979-05-04 BE870876A (en) 1979-01-15 DD139762A5 (en) 1980-01-16 IT7828477D0 (en) 1978-10-05 FR2405466B1 (en) 1984-10-19 CH634408A5 (en) 1983-01-31 US4210022A (en) 1980-07-01 DE2744845B2 (en) 1980-04-03 DE2744845A1 (en) 1979-04-19 JPS5489658A (en) 1979-07-16 IT1099763B (en) 1985-09-28 Similar Documents Publication Publication Date Title GB1586417A (en) 1981-03-18 Method of and apparatus for the inductive measurment of fluid flow US4408497A (en) 1983-10-11 Electromagnetic flowmeter for measuring ferromagnetic slurries CA1049148A (en) 1979-02-20 Analog-to-digital conversion apparatus US4672331A (en) 1987-06-09 Signal conditioner for electromagnetic flowmeter US4112428A (en) 1978-09-05 Clocked precision integrating analog to digital converter system US4157035A (en) 1979-06-05 Inductive flow meter JP3142994B2 (en) 2001-03-07 Power calculation device US4417479A (en) 1983-11-29 Electromagnetic flowmeter system having a feedback loop EP0228809B1 (en) 1991-06-05 Electromagnetic flowmeters US3776024A (en) 1973-12-04 Densitometer components SU721783A1 (en) 1980-03-15 Digital ferroprobe magnetometer SU972222A1 (en) 1982-11-07 Electromagnetic flowmeter with frequency output SU437990A1 (en) 1974-07-30 Device for determining a dynamic loop of magnetization reversal of ferromagnetic materials SU432419A1 (en) 1974-06-15 DIGITAL LOW-FREQUENCY PHASOMETER SU1132240A1 (en) 1984-12-30 Pulse voltmeter SU660002A1 (en) 1979-04-30 Arrangement for measuring maximum specific magnetic power RU2017161C1 (en) 1994-07-30 Capacitance measurement device SU828097A1 (en) 1981-05-07 Integrating converter of strain gauge bridge un balance to pulse repeitition frequency SU1610278A1 (en) 1990-11-30 Apparatus for adjusting semi-circular deviation SU1023264A1 (en) 1983-06-15 Ferromagnetic material static magnetic characteristic determination device SU1089395A1 (en) 1984-04-30 Measuring converter of displacement RU2020579C1 (en) 1994-09-30 Device for measuring relations of amplitudes of quasisinusoidal signals RU1774296C (en) 1992-11-07 Magnetic field metering device SU796764A1 (en) 1981-01-15 Device for discriminating variable and constant components of electric signal McCullough 1966 A new and unique analog-to-digital conversion technique Legal Events Date Code Title Description 1981-06-03 PS Patent sealed [section 19, patents act 1949] 1994-01-26 PCNP Patent ceased through non-payment of renewal fee Effective date: 19930526
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