CA2100807A1 - Method of and device for fluid surface detection using an ultrasonic transducer - Google Patents
Method of and device for fluid surface detection using an ultrasonic transducerInfo
- Publication number
- CA2100807A1 CA2100807A1 CA002100807A CA2100807A CA2100807A1 CA 2100807 A1 CA2100807 A1 CA 2100807A1 CA 002100807 A CA002100807 A CA 002100807A CA 2100807 A CA2100807 A CA 2100807A CA 2100807 A1 CA2100807 A1 CA 2100807A1
- Authority
- CA
- Canada
- Prior art keywords
- voltage
- ultrasonic transducer
- circuit
- generating
- transducer
- Prior art date
- 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.)
- Abandoned
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
- G01F23/296—Acoustic waves
- G01F23/2966—Acoustic waves making use of acoustical resonance or standing waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
- G01F23/296—Acoustic waves
- G01F23/2966—Acoustic waves making use of acoustical resonance or standing waves
- G01F23/2967—Acoustic waves making use of acoustical resonance or standing waves for discrete levels
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2291/00—Indexing codes associated with group G01N29/00
- G01N2291/02—Indexing codes associated with the analysed material
- G01N2291/028—Material parameters
- G01N2291/02836—Flow rate, liquid level
Abstract
METHOD OF AND DEVICE FOR FLUID SURFACE DETECTION
USING AN ULTRASONIC TRANSDUCER
A B S T R A C T
This invention relates to a circuit of an ultrasonic transducer in a surface detecting device, comprising first voltage generating means for generating a first voltage proportional to the resonant frequency of the ultrasonic transducer, means for generating a refe-rence voltage, and comparator means for monitoring the first and reference voltages and generating a surface detect signal when the first voltage drops below the reference voltage as the transducer contacts the fluid surface.
Figure 2.
USING AN ULTRASONIC TRANSDUCER
A B S T R A C T
This invention relates to a circuit of an ultrasonic transducer in a surface detecting device, comprising first voltage generating means for generating a first voltage proportional to the resonant frequency of the ultrasonic transducer, means for generating a refe-rence voltage, and comparator means for monitoring the first and reference voltages and generating a surface detect signal when the first voltage drops below the reference voltage as the transducer contacts the fluid surface.
Figure 2.
Description
2~$~
FIELD OF THE INVENTION
The invention relates to fluid surface detection devices and methods and particularly relates to methods and circuits using ultrasonic transducers for fluid surface detection.
ACKGROUND OF TH~ INV~NTION
Ultrasonic vibratory probes have been used in automated chemical analyzers where a probe is used to automatically withdraw liquid from a vessel containing liguid samples or reagents. Robotic probes of other types have been similarly used in such instruments.
In automated analyzer systems, it is desirable for the probe element to be able to detect the surface of the liquid so the probe's contact with the vessel 18 contents i9 minimized, thus, decreasing the possibility of carry over of liquid on the probe.
Various types of level sensors have been develo-ped to provide such surface or level detection. One typeof level sensor used with robotic probes in chemical analyzers are referred to as capacitive level sensors.
They operate on the principle that every conductor exhi-bits a finite electrical capacitance. When a probe having a capacitive level sensor touches a liquid, the higher dielectric constant and greater surface area of the liquid results in an increased probe capacitance that can be detected.
Among prior art capacitive liquid level sensors is the sensor described in Davis U.S. Patent n 4,977,786.
The sensor disclosed therein is useful in a liquid pipet-ting system that includes an oscillator coupled to a pipette probe for applying a high frequency signal to the probe, the amplitude or phase of the oscillator being affected by the capacitance of the probe and comparator :
21~807 means that generates a level sensor signal according to the amplitude or phase of the oscillator to signal when the probe reaches the liquid surface. The probe also includes means used to vary the frequency of the oscilla-tor in a repetitive manner.
It is desirable in automatic chemical analyzers systems to use an ultrasonically activated pipetting probe that may perform several functions includlng reagent mixing and level sensing. It is therefor desirable for the ultrasonic probe to be also able to detect the fluid surface ln vessels containing reagents and sample.
SUMMARY OF THE INVENTION
The present invention relates to an electrical circuit and method for providing an ultrasonic pipetting probe with surface detect capabilities. This method of the inventlon includes the steps of providing an ultrasonic transducer driver that generates a first voltage propor-tional to the resonant frequency of the ultrasonic trans-ducer, generating a reference voltage, monitoring and '~ 20 comparing the first voltage to the reference voltage, and generating a surface detect signal when the first voltage drops below the reference voltage.
In another embodiment of the invention a circuit is provided for providing an ultrasonically activated pipetting probe with surface detect capabilities. The circuit includes first voltage generating means for generating a first voltage proportional to the resonant frequency of the oscillations of the ultrasonic transdu-cer, means for generating a reference voltage, comparator means for monitoring the first and reference voltages and generating a surface detect signal when the first voltage drops below the reference voltage and a switch that changes status in response to the surface detect signal.
In a preferred embodiment of the invention, the circuit further includes means for removing substantially ' . '~'' ~ ~' - . ~.
~lQ~D~
all DC Components from the first voltage and amplification means to amplify the voltage to a level that is detectable above the system noise. Differentiation of the first voltage to remove the DC components allows the circuit of the inven'ion to be used in connection with any ultrasonic transducer circuit board without the necessit~ of adjus-ting the circuit to conform to the variations in levels of DC components that occur between different circuit boards.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a block diagram of an ultrasonic transducer circuit board showing a surface detect cir- ' cuit :
, - Figure 2 is a circuit diagram showing a prefer-red embodiment according to the present invention ;
Figure 3 is a graphical representation showing waveforms of voltage from the circuit of Figure 2 ;
Figure 4 is a schematic circuit dlagram of an ultrasonlc probe for use with the invention ;
Figure 5 is a schematic cicuit diagram of a motional bridge for use with the invention ; and Figure 6 is a schematic circuit diagram of a phase locked loop for use with the invention.
DETAIL~D DESC~IPTION OF THE INVENTION
The resonant frequency of an ultrasonic transdu-cer changes under certain loads. In particular, when the tip of the transducer contacts the surface of a fluid, this frequency will change slightly. Reference is now made to the drawings in which Figure 1 illustrates a typical ultrasonic transducer probe 10 driven by a startup circuit 30 11, voltage controlled oscillator 12, driver circuit 13, and motional bridge circuit 14 of conventional design.
Ultrasonic transducers are commonly driven at a resonant frequency at which the electromechanical conver-sion efficiency is the highest. The resonant characteris-tic of an ultrasonic transducer present such a high Q that .
.
-a small shift in the driving frequency from the resonantfrequency causes a significant reduction of the vibration producing efficiency. For this reason, various automatic tracking devices that automatically track the resonant frequency of the transducer to drive the transducer into oscillation, such as a vibration fsedback type oscillator and a phase locked loop type oscillator, have been develo-ped and are commonly used. Such means 15 are illustrated in Figure 1.
A circuit of the invention includes first voltage generating means for yenerating a first voltage proportional to the resonant frequency of the ultrasonic transducer. First voltage generating means useful with this invention may be any means for generating voltage proportional to the resonant frequency such as a voltage controlled oscillator (VC0) that tracks the resonant frequency of the transducer using a circuit such as a motional bridge to provide an electrical fsedback signal representative of the oscillating frequency of the trans-ducer. Motional bridge circuits are well known and can beconfigured in different forms. Motional bridge circuits produce an electrical signal proportional to both the mechanical oscillation frequency and amplitude of an ultrasonic transducer. Various motional bridge circuit designs are described in Neppiras, E.A., "Motional Feed-back Systems For Ultrasonic Transducers" 1971 Ultrasonic Con.PaDsrs. IPC Science ~ Technology Press, pages 56-58 (1971), the disclosure of which is incorporated herein by reference.
A schematic diagram of a transducer used with an ultrasonic probe useful with the invention is shown in Figure 4 where Co is the electrical impedance of the probe and Zm is the electrical equivalent of the mechanical resonance. A motional bridge circuit useful with the invention will substantially nullify the effects of the : .
,: :
-: : ,. :
2~ ~0807 capacitance Co leaving only the signal from Zm. Figure 5 shows a simplified version of a motional bridge useful with the circuit and method of the invention. A capacitor, Cp is included in parallel with the transducer on an ultrasonic driver board to help damp out cable capacitance and to provide a load if the ultrasonic probe is discon-nected while power is on. This capacitor is not a necessa-ry part of the basic motional bridge, and it will not be referred to in the following description.
The transformer 16 is a step-up transformer and r it helps limit the voltage required on the primary. Capa-citor nCo has the same scaling as the feedback tap on the transformer. Since the low side of the probe is grounded, the voltage across nCo is out of phase with the feedback voltage. This cancels the effect of Co and makes the feedback voltage proportional to the mechanical oscilla-tion (Zm). The inductor Lo is included to form a series resonance with Co and nCo to make the load seen by Xo-Yo look resistive.
The motional bridge circuit may be closed with a phase locked loop. The ultrasonic probe typically oscillates at a known frequency under fixed conditions.
Under any kind of a reactive load, however, the resonant frequency of the mechanical tank circuit will change.
Temperature variations and other factors can also affect the resonant frequency. This requires a driver circuit that wlll track the frequency of the probe under any perceived load and environmental condition.
Figure 6 diagrams a circuit useful with the surface detect circuit of the invention.
When the motional bridge is tuned correctly, the correct frequency of oscillation occurs when the phase difference between the drive signal (Xo) and the feedback is approximately zero. The phase locked loop ( PLL ) will adjust the frequency until the rising edges of the phase 210~07 comparator inputs are aligned (no phase error). This should lock the probe at the right frequency, since the MOTIONAL signal is the feedback and Xo is the drive. Once ~he loop is locked, any change in the feedback frequency will cause a corresponding change in the drive frequency.
This allows the system to operate under various loads without losing lock. It is known in the art that an ultrasonic probe will frequently have more than a single resonant frequency and it is important that the phase locked loop focus in on a single resonant frequency rather than switching from one to anot,her during operation.
Methods for initiating an ultrasonic probe and a phase ,; locking loop are known in the art and need not be discus-sed in any detail here.
15Desirably, when the ultrasonic transducer i9 used in an automated chemical analyzer with a probe, a driver circuit will be associated with the VCO and motio-nal bridge for driving the mechanical oscillatlon frequen-cy o the transducer in response to signals from the feed back system. Desirably, a bipolar full bridge driver such as a L298 driver, commercially available from various sources such as SGS-Thomson, France, able to operate with a sùpply voltage as low as 5V will be used. If necessary or desired, the output drive level to the motional bridge can be varied.
In an embodiment of this invention, the frequen-cy change can be measured at the input to the phase locked loop VCO. Figure 2 shows a circuit useful ln making the measurement. As described above, the method of the inven-tion includes the step of generating a first voltage thatis directly proportional to the resonant frequency of the ultrasonic transducer. The measured frequency shift is likely to be very small in the range of about 20 Hz which corresponds to a negative voltage shift of 100 mV.
. ~ '. :-. ':
21~8~7 In a preferred embodiment, the first voltage V1 generated by the transducer is differentiated by capacitor C and resistor Rl as shown in Figure 2 to remove any DC
component of the signal. The capacitor and resistor may be of any common type sufficient to substantially filter the DC component from the slgnal, acting as a high pass filter. Since the break frequency of the signal will vary with the speed of the probe, the capacitor and resistor should be chosen so that low frequency and DC components will be screened out. A capacitor C of 0.47 microfarads and a resistor R of 47 kOhms have been shown to serve this purpose in a circuit of the invention. The resulting AC
voltage is then amplified to a detectable level and an offset is added to provide a known DC level to the signal to generate voltage V2. Adding a gain of about 20 and offsetting the voltage by an amount approximately equal to one-half the supply voltage to the sample and hold ampli-fier (described below) has been used advantageously with a circuit of the invention. Means 17 are used for this purpose.
As described above, the circuit and method of the invention further include means for generating a reference voltage. Desirably, this reference voltage is generated by a sample and hold (S/H) amplifier 18 of a type which is commercially available. Preferably, the S/H
amplifier will include a discrete capacitor capable of holding a substantially constant reference voltage for a period of time longer than that required for the ultra-sonic transducer to detect the fluid surface, e.g. up to a second or more. THe S/H amplifier desirably will provide a substantially constant voltage between about 2 and about 12 volts ; the S/H amplifier of the circuit depicted in Figure 2 is optimally provided with a supply voltage of about 12 volts.
2~008~7 In one preferred embodiment of the invention, depicted in Figure 2, the sample and hold amplifier samples the voltage V2 as the transducer tip approaches the fluid surface. At some time prior to the tip entering the fluid the S/H is put into a hold mode which holds a constant voltage substantially equal to voltage V2 at the tlme the hold cycle of the S/H amplifier is initiated.
Since the voltage output of the S/H amplifier is substan-tially the same as the sampled voltage V2, this voltage is used as the reference voltage to which the scaled voltage of the VCO is compared. When the probe tip contacts the fluid surface, the first voltage (V2) spikes and this spike is what is intended to be detected by the comparator means 19. However, the reference voltage must be at a level which will avoid a false surface detect signal resulting from slight changes in voltage caused by noise in the circuit. In the embodiment of Figure 2, this is accomplished by using resistors R2 and R3 to form a resistor divider and drop the voltage level of the S/H
- 20 output to provide the reference voltage V3 of the inven-tion. It is to be under~tood, though, that any suitable means of providing an offset to the reference voltage can be used.
Comparator means of the invention monitors the first and reference voltages and when the first voltage drops below the reference voltage, the comparator means produces a surface detect signal. Voltage comparators are well known in the art ; voltage comparator means useful in the invention can be selected from a range of commercially available voltage comparators.
In one useful embodiment, the circuit of the invention further includes a switch that changes status in response to the surface detect signal. The switch can be any known type of switch, but a "flip flop" 20 has been found to serve particularly well. Flip flop switches are , `:
'':
2~0~ 7 'commercially available. The flip flop used in the inven-tion should obviously be chosen such that it is appro-priate for the power supply being used ; a 4013 flip flop has been found to serve its intended function.
The comparator means monitors and compares the reference voltage to the first voltage (or, as shown in Figure 2, a voltage V2 which is proportional to the first voltage V1). When the ultrasonic transducer contacts the surface of the fluid the first voltage will be a voltage spike as shown as V2 in figure 3. When the voltage spike occurs, the tip has entered the fluid and the voltage V2 drops below the voltage V3 as shown in Figure 3. The comparator's output then goes to a logic high state and triggers the flip flop switch to signal a "surface de-tect". ~he surface detect signal will remain in a trigge-red state until the S/H is put in to the sample mode. This resets the flip flop to do another surface detect.
Another posslble method of detecting a fluld surface using an ultrasonic transducer would measure the power delivered to the transducer by sampling the ultraso-nic transducer current. This method uses the principle that the impedance of the ultrasonic transducer changes when it contacts a load, such as fluid. This impedance change causes a change in the ultrasonic transducer current when the drive voltage is constant. I found this method to present several problems in attempting to adapt it for use with an ultrasonic transducer used in connec-tion with a pipetting probe. One difficulty was the fact that the total current change can be very small (almost unmeasurable) depending on the configuration of the transducer and the size of the load. Also the current waveform is an AC waveform so it would have to be peak detected or rectified to sample the change, which would require a more complex circuit to be used. Another problem with this method is that sampling current usually requires .
;.: ~ . , : , '. .
.; ., , . . .
~' ~
some type of sample resistor to be used which increases the power drive required.
While a preferred embodiment of the present invention has been described, it should be understood that various changes, adaptations and modifications may be made ,~ therein without departing frcm the spirit of the invention and the scope of the appended claims.
'' ~ ' , ~ - , .. :,. . .
FIELD OF THE INVENTION
The invention relates to fluid surface detection devices and methods and particularly relates to methods and circuits using ultrasonic transducers for fluid surface detection.
ACKGROUND OF TH~ INV~NTION
Ultrasonic vibratory probes have been used in automated chemical analyzers where a probe is used to automatically withdraw liquid from a vessel containing liguid samples or reagents. Robotic probes of other types have been similarly used in such instruments.
In automated analyzer systems, it is desirable for the probe element to be able to detect the surface of the liquid so the probe's contact with the vessel 18 contents i9 minimized, thus, decreasing the possibility of carry over of liquid on the probe.
Various types of level sensors have been develo-ped to provide such surface or level detection. One typeof level sensor used with robotic probes in chemical analyzers are referred to as capacitive level sensors.
They operate on the principle that every conductor exhi-bits a finite electrical capacitance. When a probe having a capacitive level sensor touches a liquid, the higher dielectric constant and greater surface area of the liquid results in an increased probe capacitance that can be detected.
Among prior art capacitive liquid level sensors is the sensor described in Davis U.S. Patent n 4,977,786.
The sensor disclosed therein is useful in a liquid pipet-ting system that includes an oscillator coupled to a pipette probe for applying a high frequency signal to the probe, the amplitude or phase of the oscillator being affected by the capacitance of the probe and comparator :
21~807 means that generates a level sensor signal according to the amplitude or phase of the oscillator to signal when the probe reaches the liquid surface. The probe also includes means used to vary the frequency of the oscilla-tor in a repetitive manner.
It is desirable in automatic chemical analyzers systems to use an ultrasonically activated pipetting probe that may perform several functions includlng reagent mixing and level sensing. It is therefor desirable for the ultrasonic probe to be also able to detect the fluid surface ln vessels containing reagents and sample.
SUMMARY OF THE INVENTION
The present invention relates to an electrical circuit and method for providing an ultrasonic pipetting probe with surface detect capabilities. This method of the inventlon includes the steps of providing an ultrasonic transducer driver that generates a first voltage propor-tional to the resonant frequency of the ultrasonic trans-ducer, generating a reference voltage, monitoring and '~ 20 comparing the first voltage to the reference voltage, and generating a surface detect signal when the first voltage drops below the reference voltage.
In another embodiment of the invention a circuit is provided for providing an ultrasonically activated pipetting probe with surface detect capabilities. The circuit includes first voltage generating means for generating a first voltage proportional to the resonant frequency of the oscillations of the ultrasonic transdu-cer, means for generating a reference voltage, comparator means for monitoring the first and reference voltages and generating a surface detect signal when the first voltage drops below the reference voltage and a switch that changes status in response to the surface detect signal.
In a preferred embodiment of the invention, the circuit further includes means for removing substantially ' . '~'' ~ ~' - . ~.
~lQ~D~
all DC Components from the first voltage and amplification means to amplify the voltage to a level that is detectable above the system noise. Differentiation of the first voltage to remove the DC components allows the circuit of the inven'ion to be used in connection with any ultrasonic transducer circuit board without the necessit~ of adjus-ting the circuit to conform to the variations in levels of DC components that occur between different circuit boards.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a block diagram of an ultrasonic transducer circuit board showing a surface detect cir- ' cuit :
, - Figure 2 is a circuit diagram showing a prefer-red embodiment according to the present invention ;
Figure 3 is a graphical representation showing waveforms of voltage from the circuit of Figure 2 ;
Figure 4 is a schematic circuit dlagram of an ultrasonlc probe for use with the invention ;
Figure 5 is a schematic cicuit diagram of a motional bridge for use with the invention ; and Figure 6 is a schematic circuit diagram of a phase locked loop for use with the invention.
DETAIL~D DESC~IPTION OF THE INVENTION
The resonant frequency of an ultrasonic transdu-cer changes under certain loads. In particular, when the tip of the transducer contacts the surface of a fluid, this frequency will change slightly. Reference is now made to the drawings in which Figure 1 illustrates a typical ultrasonic transducer probe 10 driven by a startup circuit 30 11, voltage controlled oscillator 12, driver circuit 13, and motional bridge circuit 14 of conventional design.
Ultrasonic transducers are commonly driven at a resonant frequency at which the electromechanical conver-sion efficiency is the highest. The resonant characteris-tic of an ultrasonic transducer present such a high Q that .
.
-a small shift in the driving frequency from the resonantfrequency causes a significant reduction of the vibration producing efficiency. For this reason, various automatic tracking devices that automatically track the resonant frequency of the transducer to drive the transducer into oscillation, such as a vibration fsedback type oscillator and a phase locked loop type oscillator, have been develo-ped and are commonly used. Such means 15 are illustrated in Figure 1.
A circuit of the invention includes first voltage generating means for yenerating a first voltage proportional to the resonant frequency of the ultrasonic transducer. First voltage generating means useful with this invention may be any means for generating voltage proportional to the resonant frequency such as a voltage controlled oscillator (VC0) that tracks the resonant frequency of the transducer using a circuit such as a motional bridge to provide an electrical fsedback signal representative of the oscillating frequency of the trans-ducer. Motional bridge circuits are well known and can beconfigured in different forms. Motional bridge circuits produce an electrical signal proportional to both the mechanical oscillation frequency and amplitude of an ultrasonic transducer. Various motional bridge circuit designs are described in Neppiras, E.A., "Motional Feed-back Systems For Ultrasonic Transducers" 1971 Ultrasonic Con.PaDsrs. IPC Science ~ Technology Press, pages 56-58 (1971), the disclosure of which is incorporated herein by reference.
A schematic diagram of a transducer used with an ultrasonic probe useful with the invention is shown in Figure 4 where Co is the electrical impedance of the probe and Zm is the electrical equivalent of the mechanical resonance. A motional bridge circuit useful with the invention will substantially nullify the effects of the : .
,: :
-: : ,. :
2~ ~0807 capacitance Co leaving only the signal from Zm. Figure 5 shows a simplified version of a motional bridge useful with the circuit and method of the invention. A capacitor, Cp is included in parallel with the transducer on an ultrasonic driver board to help damp out cable capacitance and to provide a load if the ultrasonic probe is discon-nected while power is on. This capacitor is not a necessa-ry part of the basic motional bridge, and it will not be referred to in the following description.
The transformer 16 is a step-up transformer and r it helps limit the voltage required on the primary. Capa-citor nCo has the same scaling as the feedback tap on the transformer. Since the low side of the probe is grounded, the voltage across nCo is out of phase with the feedback voltage. This cancels the effect of Co and makes the feedback voltage proportional to the mechanical oscilla-tion (Zm). The inductor Lo is included to form a series resonance with Co and nCo to make the load seen by Xo-Yo look resistive.
The motional bridge circuit may be closed with a phase locked loop. The ultrasonic probe typically oscillates at a known frequency under fixed conditions.
Under any kind of a reactive load, however, the resonant frequency of the mechanical tank circuit will change.
Temperature variations and other factors can also affect the resonant frequency. This requires a driver circuit that wlll track the frequency of the probe under any perceived load and environmental condition.
Figure 6 diagrams a circuit useful with the surface detect circuit of the invention.
When the motional bridge is tuned correctly, the correct frequency of oscillation occurs when the phase difference between the drive signal (Xo) and the feedback is approximately zero. The phase locked loop ( PLL ) will adjust the frequency until the rising edges of the phase 210~07 comparator inputs are aligned (no phase error). This should lock the probe at the right frequency, since the MOTIONAL signal is the feedback and Xo is the drive. Once ~he loop is locked, any change in the feedback frequency will cause a corresponding change in the drive frequency.
This allows the system to operate under various loads without losing lock. It is known in the art that an ultrasonic probe will frequently have more than a single resonant frequency and it is important that the phase locked loop focus in on a single resonant frequency rather than switching from one to anot,her during operation.
Methods for initiating an ultrasonic probe and a phase ,; locking loop are known in the art and need not be discus-sed in any detail here.
15Desirably, when the ultrasonic transducer i9 used in an automated chemical analyzer with a probe, a driver circuit will be associated with the VCO and motio-nal bridge for driving the mechanical oscillatlon frequen-cy o the transducer in response to signals from the feed back system. Desirably, a bipolar full bridge driver such as a L298 driver, commercially available from various sources such as SGS-Thomson, France, able to operate with a sùpply voltage as low as 5V will be used. If necessary or desired, the output drive level to the motional bridge can be varied.
In an embodiment of this invention, the frequen-cy change can be measured at the input to the phase locked loop VCO. Figure 2 shows a circuit useful ln making the measurement. As described above, the method of the inven-tion includes the step of generating a first voltage thatis directly proportional to the resonant frequency of the ultrasonic transducer. The measured frequency shift is likely to be very small in the range of about 20 Hz which corresponds to a negative voltage shift of 100 mV.
. ~ '. :-. ':
21~8~7 In a preferred embodiment, the first voltage V1 generated by the transducer is differentiated by capacitor C and resistor Rl as shown in Figure 2 to remove any DC
component of the signal. The capacitor and resistor may be of any common type sufficient to substantially filter the DC component from the slgnal, acting as a high pass filter. Since the break frequency of the signal will vary with the speed of the probe, the capacitor and resistor should be chosen so that low frequency and DC components will be screened out. A capacitor C of 0.47 microfarads and a resistor R of 47 kOhms have been shown to serve this purpose in a circuit of the invention. The resulting AC
voltage is then amplified to a detectable level and an offset is added to provide a known DC level to the signal to generate voltage V2. Adding a gain of about 20 and offsetting the voltage by an amount approximately equal to one-half the supply voltage to the sample and hold ampli-fier (described below) has been used advantageously with a circuit of the invention. Means 17 are used for this purpose.
As described above, the circuit and method of the invention further include means for generating a reference voltage. Desirably, this reference voltage is generated by a sample and hold (S/H) amplifier 18 of a type which is commercially available. Preferably, the S/H
amplifier will include a discrete capacitor capable of holding a substantially constant reference voltage for a period of time longer than that required for the ultra-sonic transducer to detect the fluid surface, e.g. up to a second or more. THe S/H amplifier desirably will provide a substantially constant voltage between about 2 and about 12 volts ; the S/H amplifier of the circuit depicted in Figure 2 is optimally provided with a supply voltage of about 12 volts.
2~008~7 In one preferred embodiment of the invention, depicted in Figure 2, the sample and hold amplifier samples the voltage V2 as the transducer tip approaches the fluid surface. At some time prior to the tip entering the fluid the S/H is put into a hold mode which holds a constant voltage substantially equal to voltage V2 at the tlme the hold cycle of the S/H amplifier is initiated.
Since the voltage output of the S/H amplifier is substan-tially the same as the sampled voltage V2, this voltage is used as the reference voltage to which the scaled voltage of the VCO is compared. When the probe tip contacts the fluid surface, the first voltage (V2) spikes and this spike is what is intended to be detected by the comparator means 19. However, the reference voltage must be at a level which will avoid a false surface detect signal resulting from slight changes in voltage caused by noise in the circuit. In the embodiment of Figure 2, this is accomplished by using resistors R2 and R3 to form a resistor divider and drop the voltage level of the S/H
- 20 output to provide the reference voltage V3 of the inven-tion. It is to be under~tood, though, that any suitable means of providing an offset to the reference voltage can be used.
Comparator means of the invention monitors the first and reference voltages and when the first voltage drops below the reference voltage, the comparator means produces a surface detect signal. Voltage comparators are well known in the art ; voltage comparator means useful in the invention can be selected from a range of commercially available voltage comparators.
In one useful embodiment, the circuit of the invention further includes a switch that changes status in response to the surface detect signal. The switch can be any known type of switch, but a "flip flop" 20 has been found to serve particularly well. Flip flop switches are , `:
'':
2~0~ 7 'commercially available. The flip flop used in the inven-tion should obviously be chosen such that it is appro-priate for the power supply being used ; a 4013 flip flop has been found to serve its intended function.
The comparator means monitors and compares the reference voltage to the first voltage (or, as shown in Figure 2, a voltage V2 which is proportional to the first voltage V1). When the ultrasonic transducer contacts the surface of the fluid the first voltage will be a voltage spike as shown as V2 in figure 3. When the voltage spike occurs, the tip has entered the fluid and the voltage V2 drops below the voltage V3 as shown in Figure 3. The comparator's output then goes to a logic high state and triggers the flip flop switch to signal a "surface de-tect". ~he surface detect signal will remain in a trigge-red state until the S/H is put in to the sample mode. This resets the flip flop to do another surface detect.
Another posslble method of detecting a fluld surface using an ultrasonic transducer would measure the power delivered to the transducer by sampling the ultraso-nic transducer current. This method uses the principle that the impedance of the ultrasonic transducer changes when it contacts a load, such as fluid. This impedance change causes a change in the ultrasonic transducer current when the drive voltage is constant. I found this method to present several problems in attempting to adapt it for use with an ultrasonic transducer used in connec-tion with a pipetting probe. One difficulty was the fact that the total current change can be very small (almost unmeasurable) depending on the configuration of the transducer and the size of the load. Also the current waveform is an AC waveform so it would have to be peak detected or rectified to sample the change, which would require a more complex circuit to be used. Another problem with this method is that sampling current usually requires .
;.: ~ . , : , '. .
.; ., , . . .
~' ~
some type of sample resistor to be used which increases the power drive required.
While a preferred embodiment of the present invention has been described, it should be understood that various changes, adaptations and modifications may be made ,~ therein without departing frcm the spirit of the invention and the scope of the appended claims.
'' ~ ' , ~ - , .. :,. . .
Claims (2)
1.- A method of detecting a fluid surface with an ultrasonic transducer comprising the steps of providing an ultrasonic transducer driver that generates a first voltage proportional to the resonant frequency of the ultrasonic transducer, generating a reference voltage, monitoring and comparing the first voltage to the refe-rence voltage, and generating a surface detect signal when the first voltage drops below the reference voltage as the transducer contacts the fluid surface.
2.- A circuit of an ultrasonic transducer in a surface detecting device, comprising first voltage genera-ting means for generating a first voltage proportional to the resonant frequency of the ultrasonic transducer, means for generating a reference voltage, and comparator means for monitoring the first and reference voltages and gene-rating a surface detect signal when the first voltage drops below the reference voltage as the transducer contacts the fluid surface.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US07/917,205 US5428997A (en) | 1992-07-20 | 1992-07-20 | Method of and device for fluid surface detection using an ultrasonic transducer |
| US917205 | 1992-07-20 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2100807A1 true CA2100807A1 (en) | 1994-01-21 |
Family
ID=25438487
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002100807A Abandoned CA2100807A1 (en) | 1992-07-20 | 1993-07-19 | Method of and device for fluid surface detection using an ultrasonic transducer |
Country Status (6)
| Country | Link |
|---|---|
| US (1) | US5428997A (en) |
| EP (1) | EP0580483B1 (en) |
| JP (1) | JPH06167375A (en) |
| AU (1) | AU669175B2 (en) |
| CA (1) | CA2100807A1 (en) |
| DE (1) | DE69300128T2 (en) |
Families Citing this family (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB9408176D0 (en) * | 1994-04-25 | 1994-06-15 | Interface Devices Distribution | Fluid level detectors |
| US5705750A (en) * | 1995-03-15 | 1998-01-06 | Sanyo Electric Co., Ltd. | Ultrasonic sensor and pipetting apparatus using same |
| DE19720519C2 (en) * | 1997-05-16 | 2000-03-30 | Pepperl & Fuchs | Device for determining and / or monitoring a fill level of a medium in a container |
| EP1261876B1 (en) * | 2000-02-29 | 2015-09-09 | Gen-Probe Incorporated | Fluid dispense and liquid surface verification system |
| DE10132530A1 (en) | 2001-07-09 | 2003-01-30 | Evotec Ag | Method for monitoring the functionality of a liquid delivery device and liquid delivery device |
| DE10242970A1 (en) * | 2002-09-17 | 2004-04-01 | Vega Grieshaber Kg | Vibration level sensor compares mechanical oscillator amplitude and/or frequency with value and detects fault in mechanical oscillator if amplitude and/or frequency of value differs in defined manner |
| DE10360526A1 (en) | 2003-12-22 | 2005-07-14 | Roche Diagnostics Gmbh | Reagent cassette with reagent container for particle-containing reagent for its noninvasive homogenization |
| DE102008009626A1 (en) * | 2008-02-18 | 2009-08-27 | Advalytix Ag | Method for checking the state of a pipette, pipetting method, pipetting device and suction tube for a pipetting device |
| US7804599B2 (en) * | 2008-07-24 | 2010-09-28 | MGM Instruments, Inc. | Fluid volume verification system |
| US10072927B2 (en) | 2016-01-07 | 2018-09-11 | Rarecyte, Inc. | Detecting a substrate |
Family Cites Families (14)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5610792A (en) * | 1979-07-06 | 1981-02-03 | Taga Denki Kk | Method and circuit for driving ultrasonic-wave converter |
| GB2084322B (en) * | 1980-09-18 | 1984-08-30 | Avery Hardoll Ltd | Fluid measuring system |
| US4540981A (en) * | 1981-10-29 | 1985-09-10 | Edo Western Corporation | Method and apparatus for detecting the presence of liquid |
| JPS5916572A (en) * | 1982-07-21 | 1984-01-27 | 多賀電気株式会社 | Method of controlling drive frequency of ultrasonic converter drive |
| US4587958A (en) * | 1983-04-04 | 1986-05-13 | Sumitomo Bakelite Company Limited | Ultrasonic surgical device |
| US4445064A (en) * | 1983-04-25 | 1984-04-24 | E. I. Du Pont De Nemours And Company | Self resonant power supply for electro-acoustical transducer |
| US4578650A (en) * | 1983-06-15 | 1986-03-25 | Watson Industries, Inc. | Resonance drive oscillator circuit |
| US4641053A (en) * | 1984-08-14 | 1987-02-03 | Matsushita Seiko Co., Ltd. | Ultrasonic liquid atomizer with an improved soft start circuit |
| EP0209872A3 (en) * | 1985-07-22 | 1988-07-27 | E.I. Du Pont De Nemours And Company | Method and apparatus for ultrasonic interface detection |
| JPS62294915A (en) * | 1986-06-13 | 1987-12-22 | Matsushita Electric Ind Co Ltd | Water level detector |
| US4754186A (en) * | 1986-12-23 | 1988-06-28 | E. I. Du Pont De Nemours And Company | Drive network for an ultrasonic probe |
| NL8801836A (en) * | 1988-07-20 | 1990-02-16 | Enraf Nonius Delft | DEVICE FOR DETERMINING THE LEVEL OF THE BOUNDARY AREA BETWEEN A FIRST AND A SECOND MEDIUM IN A RESERVOIR. |
| US4937466A (en) * | 1988-09-29 | 1990-06-26 | Ball Corporation | Remote as signal attenuator |
| US4977786A (en) * | 1990-01-18 | 1990-12-18 | E. I. Du Pont De Nemours And Company | Capacitive liquid level sensor |
-
1992
- 1992-07-20 US US07/917,205 patent/US5428997A/en not_active Expired - Lifetime
-
1993
- 1993-07-14 AU AU41924/93A patent/AU669175B2/en not_active Ceased
- 1993-07-16 DE DE69300128T patent/DE69300128T2/en not_active Expired - Fee Related
- 1993-07-16 EP EP93401845A patent/EP0580483B1/en not_active Expired - Lifetime
- 1993-07-19 CA CA002100807A patent/CA2100807A1/en not_active Abandoned
- 1993-07-19 JP JP5177902A patent/JPH06167375A/en active Pending
Also Published As
| Publication number | Publication date |
|---|---|
| DE69300128D1 (en) | 1995-06-01 |
| JPH06167375A (en) | 1994-06-14 |
| DE69300128T2 (en) | 1995-09-28 |
| US5428997A (en) | 1995-07-04 |
| AU4192493A (en) | 1994-01-27 |
| AU669175B2 (en) | 1996-05-30 |
| EP0580483A1 (en) | 1994-01-26 |
| EP0580483B1 (en) | 1995-04-26 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| FZDE | Discontinued |