Abstrict This invention relates to an ultrasonic flow meter utilizing a
conventional tubular member with an inlet and outlet. An ultrasonic
transducer is located in the member to transmit and receive ultrasonic
energy through liquid flowing through the member. An energizing
means is connected to the transducer so that ultrasonic energy can
be transmitted through the liquid in the member. Reflector means
variably positionable within the member are provided for establishing
a position for the reflector means which is proportional to liquid
flow rate through the member and for reflecting ultrasonic energy
from the transducer back to the transducer. Control means are provided
for producing at least a single pulse of ultrasonic energy from
the transducer to be transmitted through the liquid and for detecting
an echo pulse reflected from the reflector means. Means are provided
for converting the time between transmission of the ultrasonic pulse
and receipt of the echo pulse by the transducer to a signal proportional
to the liquid flow rate through the tubular member.
Claims What I claim is:
1. An ultrasonic flow meter comprising, a vertical tubular member
having an inlet and an outlet in the member with inlet and outlet
being adapted to be connected to a liquid flow system, ultrasonic
transmitting and receiving transducer means positioned in said vertical
tubular member for transmitting and receiving ultrasonic energy
through liquid flowing through the member, energizing means connected
to said transducer means for causing ultrasonic energy to be transmitted
through the liquid in said member, reflector means variably positionable
within said tubular member for providing a position proportional
to liquid flow rate through said member and for reflecting ultrasonic
energy from said transducer means back to said transducer means,
said reflector means being provided by an interface between the
top surface of the liquid and an air-filled space located within
the tubular member above the liquid and defining with the liquid
the top of the column, control means including means for producing
at least a single pulse of ultrasonic energy from said transducer
to be transmitted through the liquid and for detecting an echo pulse
reflected from said reflector means, and means for converting the
time between transmission of said ultrasonic pulse and receipt of
said echo pulse by said transducer means to a signal proportional
to the rate of flow of fluid through said tubular member.
2. The ultrasonic flow meter of claim 1 further including flow
restriction means located in said tubular means for restricting
liquid flow therethrough.
3. The ultrasonic flow meter of claim 2 wherein said flow restriction
means includes a restriction near the outlet.
4. The ultrasonic flow meter of claim 1 in which the ultrasonic
transmitting and receiving means is a single transducer.
5. The ultrasonic flow meter of claim 1 in which the energizing
means connected to the transducer means includes an astable multivibrator
controlling a monostable multivibrator to provide the pulsed output
having a spacing greater than the time required for receipt of an
echo pulse by said transducer means in said tubular member.
6. The ultrasonic flow meter of claim 1 in which the transducer
means is a Barium titanite crystal mounted in the tubular member
between the inlet and outlet.
Description FIELD AND BACKGROUND OF THE INVENTION
This invention relates to ultrasonic flow meters and more particularly
to an improved ultrasonic flow meter using a single transducer which
is sensitive, accurate and simple in design.
Acoustic or ultrasonic flow meters are known and in use. These
prior designs, however, are all exceedingly complex in both the
design of the flow chamber and transducers and in the circuitry
associated with the same. The patent to Pederson et al U.S. Pat.
No. 4011755 dated Mar. 15 1977 and entitled ACOUSTIC FLOW METER
is one of such type. It utilizes a pair of transducers at opposite
points in the flow meter between which gated bursts of relatively
high frequency of acoustic energy is transmitted. The transmission
is alternately in an upstream and downstream direction. By measuring
the relative phase shifts of the upstream and downstream transmissions,
a measurement proportional to a flow rate is obtained. The patent
to E. Hausler U.S. Pat. No. 4011753 dated Mar. 15 1977 and entitled
METHOD AND DEVICE FOR MEASURING THE FLOW VELOCITY OF MEDIA BY MEANS
OF ELECTROSOUND discloses an arrangement in which ultrasonic transducers
are located at the opposite ends of a measuring section with the
transducers having concave surfaces which face each other and which
are located in mutual co-focal relationship. The ultrasonic transducers
operate alternately as emitters or receivers or two transducers
may be used at each end of the measuring section, one being an emitter
and one being the receiver. By measuring transit time of the ultrasonic
energy in the flow direction and in the opposite direction, a time
differential proportional to flow rate is obtained.
Still other known flow meters have utilized the transducer arrangement
of two emitter receiver units transmitting in both directions with
a resolution of the frequency difference in the transmissions to
determine time of transmission and hence, rate of flow of the medium.
A further known ultrasonic flow meter is based on the Doppler-frequency
shift of a movable reflector or reflector material. The reflected
sound waves are picked up by a receiver and the determined Doppler
shift is used for determining the velocity of flow of the fluid.
The disadvantage of this measuring method is in the extensive equipment
for beaming the sound waves as well as for the elimination of temperature
influence and presence of particles in the fluid necessary for the
reflection of sound waves.
Another known ultrasonic device for acoustic flow measurements
in fluids uses special modulation means for measuring the transit
time for the sound waves along at least one path extending through
the fluid. The signal generator emits an oscillation which is frequency-modulated
in accord with an exacting predetermined principal and has a constant
duration. The difference in transit times of the sound waves in
the media is measured and the output signal representing this difference
is measured by means of a timing frequency which is corrected as
a function of the sound velocity of the fluid. The main drawback
of this measuring device is the great band width of the acoustic
electric transducer necessary for accomplishing the method.
SUMMARY OF INVENTION
The present invention in its preferred embodiment is directed to
an ultrasonic flow meter which utilizes a conventional flow meter
tube having a level indicating float therein or Rotameter with an
ultrasonic transducer to electrically provide an indication of flow
through the flow meter. The flow meter tube is a generally tapered
vertical tube member having input and output connections at the
ends of the same which are adapted to be connected into the flow
stream. Suitable restrictions or orifices may be included at either
or both the inlet and outlet. The float seeks a height or level
within the tube determined by the float characteristics and the
flow of liquid around the same within the tube member. As an alternate
embodiment, the flow meter may employ a tube with restriction in
the outlet positioned in the wall of the tube in which liquid will
seek a height within the tube equal to flowrate therethrough. The
signal ultrasonic transducer within the tube member performs a transmitting
and receiving function and is preferrably positioned at or near
the inlet of the tubular member. An energizing means connected to
the transducer provides for pulsed ultrasonic energy to be transmitted
through liquid in the member and to be reflected off the float in
the one embodiment or the surface of the liquid within the tubular
member in the alternate embodiment. The spacing of the pulsed energization
of the transducer is of such duration as to permit an echo to be
received by the transducer before it is reenergized. Suitable control
means gates the response from the transducer in a receiver mode
of operation to a detecting and comparing network which operates
through a flip-flop to determine a pulse width which is proportional
to the flowrate of fluid through the meter. This pulse width is
converted into flow indication at a meter.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic view of the flow tube portion of the ball
flow meter with transducer for the improved ultrasonic flow meter;
FIG. 2 is a schematic block diagram of the electrical circuit portion
of the same;
FIG. 3 is a timing diagram of the outputs of various components
of the measuring circuit;
FIG. 4 is a schematic electrical diagram of the circuit of FIG.
2;
FIG. 5 is a block diagram of one embodiment of the measuring and
indicating portion of the control circuit;
FIG. 6 is a block diagram of an alternate embodiment of the measuring
and indicating portion of the control circuit, and,
FIG. 7 is a schematic view of another form of the flow meter with
an ultrasonic transducer.
DESCRIPTION OF THE INVENTION
FIG. 1 shows the sensing portion of the flow meter schematically
at 10. It includes a generally tubular member 12 with restrictions
14 and 15 normally at the ends of the member and with a float member
20 positioned within the tubular member and adapted to ride on the
fluid built up therein. It should be understood that in some applications
either one or both of restrictions 14 and 15 may be unnecessary.
Such a flow meter is conventional and will normally take a flow
therethrough as indicated by the arrow 25. The rate of flow of the
fluid through the tubular member and the type of fluid flowing through
the tube will cause the float 20 to rise in the tube to a height
proportional to the rate of flow of the fluid. The height of the
float within the tubular member as determined by graduations on
the member can then be related to rate of flow through the use of
corresponding charts. Such a flow meter is particularly adapted
for use in the measurement of relatively low flow rates and with
various types of fluids.
In the present invention, this type of flow meter is modified to
include the positioning of an ultrasonic transducer 30 in the base
of the tubular member adjacent the inlet port and restriction thereto.
The height of the float within the tubular member can then be determined
ultrasonically with a simplified circuit to be hereinafter defined.
In this arrangement of parts, the transducer operates as a transmitter
and receiver with periodic pulses gated therefrom. The transducer,
which employs a Barium titanate crystal, is readily positioned within
the flow meter body or tubular member through the use of the removable
end caps which include the restrictions and pipe connections thereto.
Suitable insulated electrical wiring connects the transducer in
a circuit, with the wiring being brought out through the wall of
the fittings. The transducer is preferably located at the inlet
end of the transducer, although it will be recognized that in measuring
the position of the float within the tubular member, that it may
be placed at the outlet end if desired. The present invention is
particularly adapted for use in the medical field because the system
is non-invasive and the system may be built with materials which
are inert and non-reactive to the body.
FIG. 2 shows a block diagram of the electrical circuit of the improved
ultrasonic flow meter. The ultrasonic transducer 30 is energized
from an astable multivibrator 40 which in turn is connected to and
controls the operation of a monostable multivibrator 45. The peaked
output of the monostable multivibrator is directed through an amplifier
50 to the transducer 30 to direct the ultrasonic pulse through the
liquid in the flow meter body. The return or echo pulse received
by the transducer is coupled through a filter 60 and gated amplifier
70 to a comparator 75. The output of the comparator controls an
input of the flip-flop 80 marked CLEAR. The output of the astable
multivibrator 40 is also coupled to the flip-flop 80 and the 70
gated amplifier as indicated by the connections 82 and 83 respectively,
with the connection 82 providing an input to the input marked SET
of the flip-flop 80. The flip-flop in turn controls the width of
a pulse which is connected by a pulse-width-to-analog-amplitude
converter 85. Converter 85 provides an analog amplitude output proportional
to the rate of flow through the flow meter, as indicated by the
conductor 90. Although not shown, it will be understood that this
output will be connected to and control the operation of an indicating
meter.
A timing diagram of FIG. 3 for the flow meter shows at 3 (a) that
the pulsed output from the astable multivibrator 40 has a pulse
spacing or frequency which is adjusted to be greater than the time
it takes for a pulse of ultrasonic energy to be transmitted through
the liquid medium and the echo to be returned to the receiver. Diagram
3 (b) shows that the monostable multivibrator 45 as controlled by
the astable multivibrator 40 provides a peaked output pulse or spiked
pulse which is provided simultaneously with the initiation of the
pulse from astable multivibrator 40 and which after being amplified
by amplifier 50 is fed to the transducer 30. Diagram 3 (c) shows
the signal at the transducer in which the basic spiked output pulse
is transmitted by the transducer and then an echo signal, as indicated
by the blip at 91 is received by the transducer sometime prior
to the next transmitted pulse from the transducer. Diagram 3 (d)
shows the output of the comparator 75. Although gated by the pulse
signal from the multivibrator 40 the gating amplifier 70 does not
prevent all of the transmitted signal from reaching the comparator
and consequently, the comparator will normally show a slight response
at the start of the transmission of the pulse. The echo pulse similarly
appears between the transmission pulses. Diagram 3 (e) shows the
output of the flip-flop control circuit which provides a positive
going pulse at the start of the transmission which continues and
is shut off at the time of the receipt of the echo pulse. The width
of this pulse is the time of transmission and receipt of the ultrasonic
signal by the transducer and is proportional to the height of the
column of liquid in the flow meter and hence, the rate of flow therethrough.
In the circuit diagram of FIG. 4 the astable multivibrator 40
is shown as an LM555 timer connected for astable operation. The
input and control terminals are connected to a 5 volt DC source
95 with the source being connected through a filter capacitor 96
to ground 101 and common to the control terminal. The 5 volt source
95 is also connected through resistors 98 99 and capacitor 100
to ground 101 with a discharge terminal being connected between
the resistors 98 and 99 and the threshold and trigger terminals
being connected between the resistor 99 and capacitor 100. The operation
of the timer is astable operation provides an output as shown in
timing diagram 3 (a). The external capacitor 100 charges through
resistors 98 and 99 and discharges through resistor 99. The duty
cycle can be precisely set by the ratio of these two resistors.
The charge and discharge times of the capacitor and hence, its output
cycle are independent of supply voltage. The output terminal is
connected to conductor 102 leading to the monostable multivibrator
45. This is a conventional monostable multivibrator having the type
number N74121. Its input terminals are connected to the conductor
102. A 5 volt supply 95 is connected to the input energization terminals,
one of the control terminals 14 and through a resistor 104 and
capacitor 105 to two of the control terminals or timing pins 11
and 10 respectively. The vibrator is grounded through terminal 7
as at 101 and the output is taken on conductor 106. The input on
the control terminals 3 and 4 from conductor 102 are negative-edge
triggered logic input which will trigger a one shot output with
a positive signal on the input terminal 5. Thus the peaked output
as seen in timing diagram 3 (b) is obtained. The pulsed output is
fed through the power amplifier, indicated generally at 50 and
including transistors 110 and 115 respectively. The conductor 106
is connected through a bias resistor 111 to the base of transistor
110 with the base of the transistor being grounded through resistor
112. Its emitter is also grounded. The collector 114 is connected
through a resistor 116 to the base of transistor 115 which receives
a plus supply from a 24 volt source 120 through a resistor 121.
The emitter of transistor 115 is also connected directly to the
24 volt source 120 with the collector being connected to the transducer
30 which is grounded as at 101. The output from the transducer is
connected through a resistor 122 to a pair of clamping diodes 125
which have the type number IN4448 the diodes being grounded as
at 101. The signal is coupled through a capacitor 126 to a resistor
127 and capacitor 128 connected in parallel, which are grounded
at 101 and form the filter portion 60 of the circuit. The signal
from the filter is coupled to the input terminal 5 of the gated
amplifier 70 which takes the type number MC1445. Amplifier 70 has
a terminal 9 connected to the 5 volt source 95 with the source being
connected through a capacitor 130 to ground at 101. A gate control
input for this gated amplifier is obtained from the conductor 102
at terminal 2 having the output of the astable multivibrator thereon.
A minus 5 volt input supply 51 is connected by line 135 to another
terminal with the supply being connected to a capacitor 136 and
ground at 101. The output of the gated amplifier 70 on terminal
1 is taken through the capacitor 140 to a negative input terminal
142 of the comparator amplifier 75. This input terminal is also
connected through a resistor 143 to ground. The reference signal
terminal 144 is connected to a 5 volt DC supply 95 through voltage
divider resistors 146 and 147. The latter are grounded and the mid-point
of the resistors 146 and 147 is connected through a resistor 148
and the plus input terminal 144. The output of the comparator, as
indicated by the terminal or conductor 150 is connected to the
5 volt supply 95 through a resistor 151 to provide a voltage output
on conductor 160 leading to one input of a pair of nand gates connected
in a flip-flop circuit 80. The flip-flop circuit 80 is comprised
of nand gates 165 and 170 each taking the type number N7400 which
are dual input positive nand gates. One input of gate 165 is connected
to the conductor 102 receiving the output of astable multivibrator
40. The control input of the nand gate 170 is connected to the conductor
160 to receive the control input from the comparator 75. The respective
outputs of the nand gates are interconnected by conductors 172 and
173 to the opposite input terminals of the opposite nand gate. The
output terminal 172 of gate 165 is also connected to a convertor
through a conductor 180 which senses the width of the pulse shown
at timing diagram 3 (e). This pulse width is proportional to the
height of the float in the flow meter or the time it takes for a
pulse leaving the transducer 30 to be received as an echo from the
float. The pulse width is therefore proportional to the rate of
flow of the fluid through the flow meter.
It will be noted in the circuit that the astable multivibrator
40 controls the gated amplifier 70 but that the peaked output from
the monostable multivibrator 45 to the transducer 30 will be detected
therethrough and provide an output pulse from the comparator 75.
However, the pulses are of a short duration and do not alter the
condition of the flip-flop circuit 80 which is set by the output
of the astable multivibrator 40 or the signal impressed on conductor
102 as shown in timing diagram 3 (a). The flip-flop circuit will
provide a positive going pulse, the duration of which will continue
until the comparator senses the echo pulse and provides a input
signal on the nand gate 170 causing the flip-flop circuit to change
the output of the nand gate 165 and terminating the output from
the flip-flop circuit.
In FIG. 5 as shown in block diagram, an intergrator 185 connected
to the output of the flip-flop circuit 80 through the conductor
180 which integrator is connected to an indicating meter indicated
generally at 190. The width of the output pulse controls the operation
of the integrator to provide an analog output signal in proportion
to the magnitude of the pulse width which is coupled to the meter
190 to provide an indication of flow.
In FIG. 6 the output of the flip-flop circuit 180 energizes a
controller 192 which controls a free running clock 195. The clock
will provide a series of pulses to a counter 196 in accord with
the pulse width from the flip-flop connect. The counter output provides
visual indication in analog or digital form on a meter or indicator
200. In each instance, the frequency of pulses from the astable
multivibrator will be such that the integrator or the control of
the clock will be shut off with the receipt of the echo pulse. The
timing of the pulses will be such that the indicating meter or indicator
will have sufficient built-in delay to indicate the converted signal
or rate of fluid-flow, as determined by the width of the signal
on the flip-flop output.
FIG. 7 shows an alternate embodiment of a flow meter 210 which
employs the generally vertical tubular member 212 without the float
member. A restriction 218 is positioned in the outlet 219 of the
tubular member 212 which is located in the wall of the same. In
some applications it may not be necessary to have restriction 218.
The inlet 220 is unrestricted and the top of the tubular member
212 may be vented to atmosphere, as at 221. Flow of liquid into
the tubular member will establish a height or column of liquid in
the tubular member which will be determined by the pressure of the
liquid flowing into inlet 220 inlet pressure and the flow rate of
the liquid through the tubular member. The height of the column
will be proportional (not linearly) to velocity of flow out of the
tubular member. A transducer crystal 230 is mounted in the base
or bottom of the tubular member 212 and the ultrasonic energy transmitted
by transducer 230 will be reflected off of the interface between
the top surface of the column of liquid and the air-filled space
above the liquid shown at 232.
The operation of this version of the flow meter is the same as
the preferred embodiment in which the pulsed ultrasonic energy is
transmitted through the column of liquid within the tubular member
and reflected back to the transducer as an echo pulse. The time
elapse between transmission and echo is proportional to the height
of the liquid column and hence proportional to flow through the
meter. The same circuit embodiments shown in FIGS. 2-4 are used
in the measurement of elapsed time and flow rate. In using flow
meter 210 of FIG. 7 FIG. 5 or FIG. 6 must be modified to include
a non-linear convertor to convert fluid height, h, to flow rate
Q by Q = K.sqroot.h where K is a constant.
In considering this invention, it should be remembered that the
present disclosure is illustrative only and the scope of the invention
should be determined by the appended claims. |