Method and arrangement for flow rate measurement by means of ultrasonic waves

Claim 2

Method for flow rate measurement by means of ultrasonic waves which are propagated in a medium flowing through a measuring tube (10) between two ultrasonic transducers (12, 14) which are arranged spaced a defined distance apart from each other and of which the one operates as transmitting transducer converting an electrical transmission signal (U S ) to an ultrasonic wave of the same frequency (f M ) whilst the other operates as receiving transducer converting the incoming ultrasonic wave to an electrical reception signal (U E ) of the same frequency, the phase shift between the transmission signal (U S ) and the reception signal (U E ) being measured to determine the flow rate, the method comprising the steps of generating a counting frequency signal (I C ) with a counting frequency (f C ) substantially greater than the measuring frequency (f M ), counting the periods of the counting frequency signal (I C ) in measuring time intervals (T I ) corresponding to the phase shift between the transmission signal (U S ) and the reception signal (U E ), varying a start phase (φ S ) which the counting frequency signal (I C ) has at the beginning of each counting operation with respect to the measuring time interval (T I ) from measuring time interval to measuring time interval in a measuring cycle (T R ) including a plurality of consecutive measuring time intervals (T I ), and evaluating the counts obtained in the course of the measuring cycle (T R ) to form a measured value with increased measurement resolution.

Claim 3

Method according to claim 1, characterized in that the start phase (φ S ) of the counting frequency signal (I C ) is varied in the course of the measuring cycle (T R ) by 2π.

Claim 4

Method according to claim 1 or 2, characterized in that the measuring frequency (f M ) is derived from the counting frequency (f C ) by frequency division and that in each measuring cycle (T r ) a phase shift (φ M ) varying from period to period of the measuring frequency (f M ) is imparted to the measuring frequency (f M ) with respect to the counting frequency (f C ).

Claim 5

Method according to claim 3, characterized in that the phase shift (φ M ) imparted to the measuring frequency (f M ) becomes continuously greater in the course of the measuring cycle (T R ).

Claim 6

Method according to claim 4, characterized in that the phase shift (φ M ) imparted to the measuring frequency (f M ) in each period of the measuring frequency is varied in dependence upon preceding measurement results for the purpose of a successive approximation.

Claim 7

Method according to claim 1 or 2, characterized in that the measuring frequency (f M ) is derived by frequency division from a frequency (f C ) which differs by a predetermined differential frequency (Δf) from the counting frequency (f C ).

Claim 8

Method according to claim 6, characterized in that the differential frequency (Δf) is equal to the measuring frequency (f M ) divided by the number (n) of the measuring time intervals (T I ) per measuring cycle (T R ).

Claim 9

Method according to claim 1, characterized in that a frequency modulation with predetermined frequency swing (f h ) about a middle frequency (f C0 ) is imparted to the counting frequency (f C ).

Claim 10

Method according to claim 8, characterized in that the frequency modulation of the counting frequency (f C ) takes place in accordance with a periodic function which varies symmetrically to the middle frequency (f C0 ) and the period duration of which is equal to the duration of a measuring cycle (T R ).

Claim 11

Method according to claim 9, characterized in that the periodic function is a sinusoidal function.

Claim 12

Method according to claim 9, characterized in that the periodic function is a sawtooth function.

Claim 13

Method according to claim 9, characterized in that the periodic function is a periodic pseudo random function.

Claim 14

Method according to claim 12, characterized in that the periodic pseudo random function is reset to the same initial state prior to the start of each measuring cycle (T R ).

Claim 15

Method according to claim 8, characterized in that the frequency modulation of the counting frequency (f C ) takes place in accordance with a noise function with statistically equal distribution.

Claim 16

Method according to claim 14, characterized in that the frequency spectrum of the noise function is subjected to a bandwidth limitation with an upper and lower limit frequency (f Gmax , f Gmin ).

Claim 17

Method according to claim 15, characterized in that the upper limit frequency (f Gmax ) is small compared with twice the reciprocal (2/T I ) of the duration of a measuring time interval (T I ) and that the lower limit frequency (f Gmin ) is large compared with the reciprocal (1/T R ) of the duration of a measuring cycle (T R ).

Claim 18

Method according to claim 1, characterized in that the counting frequency signal (I C ) is generated in each case only in the duration of the measuring time interval (T I ), that the phase position of the counting frequency signal (I C ) is stored at the end of each measuring time interval and that the generation of the counting frequency signal (I C ) at the start of each following measuring time interval is continued with the stored phase position.

Claim 19

Method according to claim 17, characterized in that the counting frequency signal (I C ) is derived from a delta voltage (U D ) generated in each case only in the duration of each measuring time interval (T I ) and at the beginning of each measuring time interval continued from the signal level reached at the end of the preceding measuring time interval.

Claim 20

Method according to claim 1, characterized in that on detection of a duration of the measuring time intervals (T I ) too small for correct measurement of the phase shift an additional phase shift through 180° is imparted to one of the two signals (U S , U E ) having a relative phase shift.

Claim 21

Method according to claim 19, characterized in that the phase shift between two square-wave signals (Q S , Q E ) derived from the transmission signal (U S ) and the reception signal (U E ) is measured and that to obtain the additional phase shift through 180° one of the two square-wave signals (Q S , Q E ) is inverted.

Claim 22

Method according to claim 1, characterized in that to determine whole wavelengths of the ultrasonic waves in the medium flowing through the measuring tube (10) between the two ultrasonic transducers (12, 14) the transmitting transducer is stimulated by a short pulse (I D ) to transmit a wave train and the periods of a signal (S R ) with the measuring frequency (f M ) or an integer multiple (2·f M ) of the measuring frequency are counted during the travel time (T L ) of the wave train from the transmitting transducer to the receiving transducer.

Claim 23

Method according to claim 1, characterized in that the amplitude of the reception signal (U E ) is monitored and on detection of an amplitude insufficient for proper evaluation a signal is sent to an evaluating circuit (32).

Claim 24

Arrangement for flow rate measurement by means of ultrasonic waves comprising a measuring tube (10) traversed by a medium, two ultrasonic transducers (12, 14) arranged on the measuring tube (10) at a definite distance (L M ) from each other, means for applying an electrical transmission signal (U S ) with a measuring frequency (f M ) to one of the two ultrasonic transducers which operates as transmitting transducer converting said electrical transmission signal (U S ) to an ultrasonic wave of the measuring frequency which is propagated in said medium while the other ultrasonic transducer operates as receiving transducer converting the ultrasonic wave to an electrical reception signal (U E ) of the measuring frequency, means for receiving the electrical reception signal (U E ) with the measuring frequency emitted by the other ultrasonic transducer, a counting frequency generator generating a counting frequency signal (I C ) with a counting frequency (f C ) substantially greater than the measuring frequency (f M ), a counter (30) counting the periods of the counting frequency signal (I C ) in measuring time intervals (T I ) which correspond to the phase shift between the transmission signal (U S ) and the reception signal (U E ), and an evaluating circuit (32) to which the count reached in each measuring time interval (T I ) is transferred, characterized by means which vary the start phase (φ S ) which the counting frequency signal (I C ) has at the beginning of each counting operation with respect to the measuring time interval (T I ) from measuring time interval to measuring time interval in a measuring cycle (T R ) including a plurality of consecutive measuring time intervals (T I ).

Claim 25

Arrangement for flow rate measurement by means of ultrasonic waves comprising a measuring tube (10) traversed by a medium, two ultrasonic transducers (12, 14) arranged on the measuring tube (10) at a definite distance (L M ) from each other, means for applying an electrical transmission signal (U S ) with a measuring frequency (f M ) to one of the two ultrasonic transducers which operates as transmitting transducer converting said electrical transmission signal (U S ) to an ultrasonic wave of the measuring frequency which is propagated in said medium while the other ultrasonic transducer operates as receiving transducer converting the ultrasonic wave to an electrical reception signal (U E ) of the measuring frequency, means for receiving the electrical reception signal (U E ) with the measuring frequency emitted by the other ultrasonic transducer, a counting frequency generator generating a counting frequency signal (I C ) with a counting frequency (f C ) substantially greater than the measuring frequency (f M ), a counter (30) counting the periods of the counting frequency signal (I C ) in measuring time intervals (T I ) which correspond to the phase shift between the transmission signal (U S ) and the reception signal (U E ), and an evaluating circuit (32) to which the count reached in each measuring time interval (T I ) is transferred, characterized by means which vary the start phase (φ S ) which the counting frequency signal (I C ) has at the beginning of each counting operation with respect to the measuring time interval (T I ) from measuring time interval to measuring time interval in a measuring cycle (T R ) including a plurality of consecutive measuring time intervals (T I ).

Claim 26

Arrangement according to claim 23, characterized in that to the output of the counting frequency generator (28) a frequency divider (34) is connected of which the division factor (N) corresponds to the ratio between the counting frequency (f C ) and the measuring frequency (f M ), that the frequency divider (34) is followed by a controllable phase shifter (36) which imparts a phase shift defined by a phase control signal (U R ) to the output signal of the frequency divider (34), and that the output signal of the controllable phase shifter (36) is employed for the electrical transmission signal (U S ).

Claim 27

Arrangement according to claim 24, characterized in that the phase control signal (U R ) is a ramp signal varying linearly in the course of each measuring cycle.

Claim 28

Arrangement according to claim 24, characterized by a digital-analog converter (70) which converts digital code groups to the phase control signal (U R ).

Claim 29

Arrangement according to any one of claims 24 to 26, characterized in that the controllable phase shifter (36) is formed by a PLL circuit.

Claim 30

Arrangement according to claim 23, characterized in that the counting frequency generator furnishes at a first output (80a) the counting frequency signal (I C ) and at a second output a signal having a frequency (f C ') which differs from the counting frequency (f C ) by a predetermined differential frequency (Δ f ) and that to the second output (80b) of the counting frequency generator (80) a frequency divider (34) is connected and the output signal (R S ) thereof is used to generate the electrical transmission signal (U S ).

Claim 31

Arrangement according to claim 23, characterized in that the counting frequency generator includes a frequency modulator (100) and a modulation signal generator (112) and that the counting frequency signal (I C ) is formed from the output signal of the frequency modulator (100) frequency-modulated by the modulation signal.

Claim 32

Arrangement according to claim 29, characterized in that the frequency modulator (100) is formed by a PLL circuit which includes a voltage-controlled oscillator (116) on the control signal of which the modulation signal furnished by the modulation signal generator (112) is superimposed and which at the output furnishes a signal with the frequency-modulated counting frequency (f C ).

Claim 33

Arrangement according to claim 29 or 30, characterized in that the modulation signal generator (112) is a noise generator.

Claim 34

Arrangement according to claim 29 or 30, characterized in that modulation signal generator (112) is a pseudo random generator.

Claim 35

Arrangement according to claim 29 or 30, characterized in that the modulation signal generator (112) is followed by a bandpass (114).

Claim 36

Arrangement according to claim 23, characterized in that the counting frequency generator is stopped at the end of each measuring time interval (T I ) and restarted again at the beginning of the respective following measuring time interval (T I ) with the phase position of the counting frequency reached on the stopping.

Claim 37

Arrangement according to claim 34, characterized in that the counting frequency generator includes a delta generator (124) which in the duration of the measuring time interval (T I ) generates a delta voltage (U D ) with the counting frequency (f C ) and at the start of each measuring time interval continues the generation of the delta voltage (U D ) with the signal level reached at the end of the preceding measuring time interval.

Claim 38

Arrangement according to claim 35, characterized in that the delta generator (124) is followed by a pulse shaper (126) which transforms the output voltage (U D ) of the delta generator (124) to counting pulses (I C ) in phase therewith.

Claim 39

Arrangement according to 23, characterized by a pulse generator (202) which for the determination of the number (m) of whole wavelengths of the ultrasonic wave in the measuring tube (10) applies a short single pulse (I D ) to one of the two ultrasonic transducers (12, 14) so that the latter is stimulated to transmit a short wave train, a counter (222) which is set in operation on application of the single pulse (I D ) for counting a counting signal (S R ) with the transmission frequency (f M ) or an integer multiple (2·f M ) of the transmission frequency, and by a pulse-receiving circuit (210) which is connected to the other ultrasonic transducer and stops the counter (222) on arrival of the short wave train at the other ultrasonic transducer.

Claim 40

Arrangement according to 23, characterized by a pulse generator (202) which for the determination of the number (m) of whole wavelengths of the ultrasonic wave in the measuring tube (10) applies a short single pulse (I D ) to one of the two ultrasonic transducers (12, 14) so that the latter is stimulated to transmit a short wave train, a counter (222) which is set in operation on application of the single pulse (I D ) for counting a counting signal (S R ) with the transmission frequency (f M ) or an integer multiple (2·f M ) of the transmission frequency, and by a pulse-receiving circuit (210) which is connected to the other ultrasonic transducer and stops the counter (222) on arrival of the short wave train at the other ultrasonic transducer.

Claim 41

Arrangement according to claim 37, characterized in that the pulse-receiving circuit (210) includes in succession an input amplifier (212), a rectifier circuit (214) and a threshold value switch (216).

Claim 42

Arrangement according to claim 37 or 38, characterized in that the counting signal (S R ) is supplied to the counter (222) via a start-stop logic (218) which is opened by a start signal (I S ) initiating the generation of the short single pulse (I D ) and is blocked by a stop signal (S S ) emitted by the output of the pulse-receiving circuit (210).

Claim 43

Arrangement according to claim 37 or 38, characterized by a frequency doubler (220) which receives a square-wave signal (R S ) with the transmission frequency (f M ) and emits the counting signal (S R ) with twice the frequency (2·f M ).

Claim 44

Arrangement according to claim 23, characterized by signal processing circuits (20, 22) which convert the reception signal (U E ) and the transmission signal (U S ) to square-wave voltages (Q E , Q S ) in phase therewith and by a phase detector (24) which receives the square-wave voltages (Q E , Q S ) and furnishes measuring pulses (I M ) having a duration which corresponds to the phase shift between its input signals and governs the duration of the measuring time intervals (T I ).

Claim 45

Arrangement according to claim 41, characterized in that between the output of one of the two signal processing circuits (20, 22) and the associated input of the phase detector (24) an inverting circuit (226) is inserted which is actuated by a control signal furnished by the evaluating circuit (32) for inversion of the square-wave voltage (Q S or Q E ) supplied thereto when the evaluating circuit (32) detects that the duration (T I ) of the measuring pulses (I M ) furnished by the phase detector (24) lies beneath a predetermined value.

Claim 46

Arrangement according to claim 23, characterized by an amplitude monitoring circuit (224) which receives the reception AC voltage and supplies a signal to the evaluating circuit (32) when the amplitude of the reception AC voltage lies beneath a predetermined value.

Claim 47

Arrangement according to claim 43, characterized in that each ultrasonic transducer (12, 14) is formed by an annular piezoelectric transducer (130) which is installed coaxially to the measuring tube (10) and which for measuring the phase shift is stimulated by a measuring frequency (f M ) equal to its radial resonant frequency.

Claim 48

Arrangement according to claim 44, characterized in that the radial resonant frequency of the annular piezoelectric transducer (130) is so chosen that the wavelength of the ultrasonic wave propagated in the medium is greater than 1.6 times the internal diameter of the measuring tube (10).

Claim 49

Arrangement according to claim 44 or 45, characterized in that the acoustic characteristic impedance of the measuring tube (10) is substantially greater than the acoustic characteristic impedance of the medium flowing therein.

Claim 50

Arrangement according to claim 44, characterized in that the annular piezoelectric transducer (130) for determining the number of whole wavelengths in the measuring tube (10) is stimulated by a short single pulse (I D ) to oscillations at its longitudinal resonant frequency.

Claim 51

Arrangement according to claim 44, characterized in that the inner surface of the annular piezoelectric transducer (130) is covered with a protective layer (138) resistant to aggressive media.

Claim 52

Arrangement according to claim 48, characterized in that between the annular piezoelectric transducer (130) and the adjacent tube sections seals (150, 152) are inserted having an acoustic characteristic impedance which is substantially smaller than the acoustic characteristic impedance of the tube sections.

Claim 53

Arrangement according to claim 44, characterized in that on both sides of the measuring tube (10) attenuation tubes (160) are arranged of which the inner side is lined with a nonporous damping material (164).