GB2277992A - A sensor arrangement for ice bank control - Google Patents

A sensor arrangement for ice bank control Download PDF

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Publication number
GB2277992A
GB2277992A GB9324826A GB9324826A GB2277992A GB 2277992 A GB2277992 A GB 2277992A GB 9324826 A GB9324826 A GB 9324826A GB 9324826 A GB9324826 A GB 9324826A GB 2277992 A GB2277992 A GB 2277992A
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GB
United Kingdom
Prior art keywords
ice
probe
tine
sensor arrangement
vibration
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.)
Granted
Application number
GB9324826A
Other versions
GB9324826D0 (en
GB2277992B (en
Inventor
Martin Johnson
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.)
Cornelius Inc
Original Assignee
IMI Cornelius Inc
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.)
Filing date
Publication date
Priority claimed from GB929225838A external-priority patent/GB9225838D0/en
Application filed by IMI Cornelius Inc filed Critical IMI Cornelius Inc
Priority to GB9324826A priority Critical patent/GB2277992B/en
Publication of GB9324826D0 publication Critical patent/GB9324826D0/en
Publication of GB2277992A publication Critical patent/GB2277992A/en
Priority claimed from US08/546,002 external-priority patent/US5627310A/en
Application granted granted Critical
Publication of GB2277992B publication Critical patent/GB2277992B/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/02Analysing fluids
    • G01N29/036Analysing fluids by measuring frequency or resonance of acoustic waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/02Indexing codes associated with the analysed material
    • G01N2291/025Change of phase or condition
    • G01N2291/0251Solidification, icing, curing composites, polymerisation

Abstract

A sensor arrangement principally for ice bank control using a single probe (9) allowed to resonate at its natural resonant frequency. That resonant frequency is different when ice has adhered to the probe and this is detected to indicate ice growth in the ice bank. A resonator/detector (11) oscillates the probe for short periods of time at regular intervals, which allows ice to form about the probe when not in oscillation. <IMAGE>

Description

A Sensor Arrangement The present invention relates to a sensor arrangement and more particularly but not exclusively to a sensor arrangement for an ice bath of a beverage dispense system.
There is a requirement to sense or detect the level of solid or particulate matter such as grain or rice in a holding vessel. With ice banks of a beverage dispense system it is the thickness or weight of ice formed that requires measurement.
Previously, ice in an ice bank has been detected by one of three methods.
A first method is using a temperature operated switch arranged to detect the water temperature in the ice bank which is indicative of the ice formed. This temperature approach suffers from inherent inaccuracy and a wide differential in performance of switches.
Furthermore, location and maintenance of the switch is essential to achieve reasonable results.
A second approach is to employ a mechanical switch which is effectively displaced as the ice grows within the ice bank. Again the problems of inconsistency are present and in addition it is important to ensure the mechanical switch has an actuator that is displaced by the surface of the ice and does not become enveloped within the ice.
A third method involves use of two electrical probes. An electrical current is passed between the probes and the conductance is drastically altered as ice is formed. Obviously, this method has problems of electrolysis of the probes along with disposition of dirt and dissolved salts on the probes. Furthermore, this method is dependent upon water composition as an electrolyte and so each system must be commissioned by experienced personnel.
It is an objective of the present invention to provide a probe arrangement that substantially relieves the above problems.
In accordance with the invention there is provided a sensor arrangement comprising a probe arranged to resonate and detector means arranged to detect changes in the probe resonant frequency, the probe being arranged in a vessel such that alteration in the contents of the vessel will alter the probe resonant frequency or amplitude detected by the detector means.
Preferably, the vessel is an ice bank comprising a vat and refrigeration system arranged to deposit ice from a body of water held in the vat.
The probe may be in a vertical, or in a horizontal or in an inclined attitute.
The sensor arrangement is preferably part of a control system to control level of particulate matter or growth of depositions such as ice in the vessel.
The control system being arranged to control particulate matter vessel entry means or deposition growth means.
An embodiment of the present invention will now be described with reference to an accompanying schematic drawings in which: Figure 1 is a schematic illustration of a ice probe system configuration; Figure 2 is an enlarged schematic illustration of the ice probe in an ice bank vessel.
Figure 3 is a graphical representation of typical ice probe response with various environments.
Figure 4 is a schematic illustration of an ice probe; Figure 5 is a schematic illustration of an input circuitry arrangement for the ice probe; and, Figure 6 is a schematic illustration of an output or pick-up circuitry arrangement for the ice probe.
Referring to Figure 1. An ice bank 1 comprises a vessel or vat 3, water 5, ice 6 and refrigerator evaporator coils 7. The ice 6 is formed about coils 7 as a blanket. A product coil 8 passes though the bank 1 in order to cool a beverage within before dispense through a dispense tap (not shown).
Normally there are several product coils 8 in a bank 1 to accommodate several beverages.
The object of ice 6 is to create an effective cold thermal store during periods of low draw-off through the coils 8 for use during high dispense periods. Thus, it is possible to use a lower rated refrigeration system than would be necessary for peak beverage dispense rates. Evidently, there is an optimum ice thickness as ice is a relatively poor conductor of heat so creation of ice further from coils 7 becomes less efficient. In order to switch the refrigeration system off it is therefore necessary to detect the optimum thickness of ice.
In the present invention, a probe 9 is arranged to extend into the bank 1. The probe 9 is typically 50 to 100 millimetres in length. The probe 9 is water proof and located at a spaced position from the coils 7.
In operation, the probe 9 is oscillated by a resonater/detector 11 at its natural resonant frequency. The resonator 11/probe 9 may be a piezo-electric device. The probe 9 is allowed to oscillate/resonate for short periods at regular intervals so allowing ice to form about the probe 9 when not oscillating. These 'off periods ensure that a water pocket is not created about the probe 9 due to localised mixing and temperature enhancement due to vibration. The time period between oscillation pulses may be up to 5 minutes but is principally determined by the degree of deposition control required of the ice 6.
It is at the core of the present invention, that the resonant frequency of the probe 9 is altered as ice is deposited. Thus, the resonator/detector 11 is arranged to detect this change in resonance between two latched levels. A first latch level equivalent to an ice free condition and a second latch level determined in order to equate to the desired level of ice 6. Once the second latch level is achieved then a controller 15 is arranged to switch off the refrigeration system. The detector 11 latch level is regularly updated at each oscillator pulse period and the refrigeration system switched ON if the ice 6 level has deteriorated.
Although the probe 9 is illustrated in a vertical position it will be appreciated that other orientations including horizontal and an inclined attitute could be used.
The probe 9 could be used to detect the difference between an empty or full grain or rice silo by utilisation of the difference in reasonant frequency between the probe 9 in air and when surrounded by grain/rice.
Figure 2 illustrates an ice probe 21 in greater detail. The probe 21 is made up of an input tine 22 and an output tine 23 separated by an anti-node area 24 of the probe 21. Typically, most of the probe 21 will be submersed in water/ice of a vat 25 which includes evaporator coils 26 of a refrigeration system, a volume of water 27 and product coils 28.
An ice bank 29 is generated about the evaporator coils 26 and grows generally in the direction of arrowhead A. This ice bank 29 as indicated previously acts as a thermal store to accommodate periods of high dispense through the product coils 28. Consequently, the ice bank 29 grows during periods of inactivity or low dispense until it impinges upon the output tine 23 of the probe 21.
The effect of this ice contact is to alter the pick-up frequency of the output tine 23 received from the input tine 22. This alteration in pick-up frequency or amplitude in the output tine 23 is conveniently detected using a piezo-electric crystal 29. Such crystals 29 provide an eledtrical signal when stressed by deformation. Thus, these electrical signals can be sent to electronic process elements to determine changes in environmental conditions about the tine 23 and so control operation of the ice bank refrigeration system.
It will be understood that the input tine 22 induces oscillation in the pick-up or output tine 23.
Conveniently, the input tine 22 is forced to oscillate by a driving piezo-electric crystal 30. Oscillation is achieved by applying an electrical potential across the crystal 30. As an alternative, and in suitable circumstance, it may be possible to use the natural vibration effects in the vat 25 from the refrigeration system compressor and other environmental vibration sources such as agitator elements. Furthermore, independent dedicated vibration sources could be used including bubble generators etc.
It will be understood the major advantage of using a piezo-electric crystal or dedicated vibration generator is that environmental noise can be more easily eliminated and so the prospect of spurious results reduced. Furthermore, frequencies such as those used in electrical mains (50 HZ) and their multiples should be avoided for similar reasons.
In the present invention it is intended to use pulses of vibration at intervals of about 30 seconds.
The frequency of the vibrations may be 120 HZ or several KHZ in order to avoid environmental noise impinging upon the system. Obviously, the actual vibration frequency and pulse interval is tailored to individual requirements.
Figure 3 illustrates a typical output response from tine 23 in comparison with environmental conditions. It will be seen the response is substantially linear. Furthermore, the tine 23 will vibrate in air with a distinct output compared with water. Thus, the probe 21 can be used as a vat 25 out of water detector as well as an ice bank level detector or as a water level control. As the water 27 is chilled and the ice bank 29 develops until it impinges upon the probe 21 the degree of induced vibration in the output tine 23 diminishes.
Obvidusly, when the tine 23 is embedded in ice the degree of vibration and thus electrical output is minimal. Normally, the electrical output of a piezo-electric crystal 29 is in the range of mV and a typical output from induced vibration would be 10 mV.
Figure 4 illustrates in greater detail the ice probe 21 with input tine 22 and output tine 23.
Each tine 22, 23 has a piezo-electric crystal 29, 30 such as PbZnTiO3 attached at it base near the anti-node 24 between the tines 22, 23. Typically, the probe 21 is made of polyacrylate, titanium, invar, aluminium or glass.
The resonant frequency (n) of the ice probe 21 illustrated in Figure 4 is given by the formula.
where k = constant = 1.1937 t = tine thickness 1 = tine length e = Youngs Modulus p = density Thus, if the ice probe 21 is formed from invar 10 with a Youngs Modulus of 21 x 10, a density of 8800 3 Kg M, t = lmm and 1 = 50 mm then the resonant frequency n = 75 HZ. However, this frequency will alter as ice is deposited about the tines 22, 23.
Furthermore, input piezo-electric crystal 30 may induce different frequencies in the ice probe. In order to locate the ice probe 21 in the vat 25 a stem 32 is provided such that the orientation and depth of the probe 21 may be adjusted. To enable such adjustment the stem typically has a screw thread.
The ice probe or sensor 21 may be moulded from plastics material such as polyacrylate for ease of fabrication and to reduce costs.
The drive circuitry for input piezo-electric crystal 30 is shown in schematic form in Figure 5.
The crystal 30 is adhered to the wall of tine 22 in some acoustically suitable fashion. A signal generator 33 is arranged to provide pulses or bursts of vibration frequency. Typically, these bursts may be 30 seconds apart and the osciliation or vibration frequency may be 400HZ. The generator 33 may include two 555 microprocessors suitably coupled to provide the vibration pulses. However, there are a wide range of signal generator systems that could be used.
The vibration pulses are passed to a driving circuit 34. This circuit 34 provides the electrical stimulus for the crystal 30. A convenient driving circuit includes a transformer in which the vibration pulse drives one side and the crystal 30 is coupled to the otherside. However, the piezo-electric crystal could be powered in variety of ways.
The vibration pulses are typically spaced by 30 seconds or so to enable ice to develop about the tines 22, 23.
Figure 6 schematically illustrates the pick-up circuitry coupled to the output or pick-up piezo-electric crystal 29 coupled to tine 23. The electrical signals produced by the crystal 29 are typically in the order of mV. Thus, signals from the crystal 29 are amplified by a factor of 100 or 1000 by an amplifier 35. The signals from the amplifier 35 are electrically filtered in order to remove spurious signals and possibly limit the signals passed to a comparison circuit 36. Thus, the filter 37 may be of the band type or high pass type or low pass type dependent upon requirements.
The comparison circuit may be a simple comparator in which signals are compared with stored values for air, water and ice and dependent upon the results a controller 37 is stimulated.
The controller 37 may simply switch the refrigeration system of the ice bank apparatus on or off in response to ice probe 21 signals. However, the controller may also give a visual indication of ice probe status ie in ice or water. Furthermore, it is advantageous that the controller 37 ensures that several successive ice probe signals are received before determining ice bank status.
It will be understood that several ice probes could be placed at different locations in the vat 25 in order to move accurately determine ice bank growth.
The driving circuitry and pick-up circuitry is conveniently time synchronised so that the pick-up circuitry is only operational when the driving circuitry is causing the input tine 22 to vibrate.
It will be understood by a person skilled in the art that vibration amplitude could be detected rather than frequency.

Claims (15)

CLAIMS:
1. A sensor arrangement comprising a probe arranged to resonate and detector means arranged to detect changes in the probe resonant frequency, the probe being arranged in a vessel such that alteration in the contents of the vessel will alter the probe resonant frequency or amplitude detected by the detector means.
2. A sensor arrangement as claimed in claim 1 wherein the probe includes an input tine and an output or pick-up tine arranged such that vibrations of the input tine are picked-up by the output tine such that differences in said vibration frequency or amplitude can be determined by the detection means.
3. A sensor arrangement as claimed in claim 2 wherein the vibration of the input tine is provided by a driving piezo-electric device and/or picked-up vibration by the output tine is detected by a piezo-electric device.
4. A sensor arrangement as claimed in claim 3 wherein the driving piezo-electric device provides pulses of vibration of a specified frequency at set time intervals.
5. A sensor arrangement as claimed in any preceding claim wherein the probe is made of a plastics material such as polyacyrlate or aluminium or invar or any other suitable material.
6. A sensor arrangement as claimed in any preceding claim wherein the vessel is an ice bank comprising a vat and refrigeration system arranged to deposit ice from a body of water held in the vat in response to signals received from the sensor arrangement.
7. A sensor arrangement as claimed in any preceding claim wherein the probe is vertical or horizontal or in an inclined attitude within the vessel.
8. A sensor arrangement as claimed in any preceding claim included as part of a control system to control particulate matter or ice growth in the vessel by adjusting vessel entry means or deposition growth means.
9. An ice bank control system for an ice bath including an ice probe having an input tine and an output tine, the output tine being arranged to resonate in response to vibration induced by the input tine and being positioned so that ice growth impinges upon the output tine and so alter its resonant frequency or amplitude, said alteration being determined by a detector piezo-electric device fixed to the output tine arranged to provide electrical signals indicative of frequency or amplitude, these electrical signals being supplied to a controller which is arranged to control ice bank growth in response to these electrical signals.
10. An ice bank control as claimed in claim 9 wherein the input tine includes a source piezo-electric device arranged to vibrate the input tine and so stimulate vibration in the output tine.
11. An ice bank control as claimed in claim 10 wherein the source piezo-electrical device is arranged to provide pulses of vibration at specified time intervals.
12. An ice bank control as claimed in claim 11 wherein the controller is arranged to be operational in synchronisation with the pulses of vibration and so allow ice to develop about the probe.
13. An ice bank control as claimed in any of claims 9 to 12 in which the controller indicates water level in the ice bath or that water is present in the ice bath or the environmental status of the probe in response to electrical signals from the probe.
14. A sensor arrangement substantially is herein before described with reference to the accompanying drawings.
15. An ice bank control substantially as hereinbefore described with reference to the accompanying drawings.
GB9324826A 1992-12-10 1993-12-03 A sensor arrangement Expired - Fee Related GB2277992B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
GB9324826A GB2277992B (en) 1992-12-10 1993-12-03 A sensor arrangement

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
GB929225838A GB9225838D0 (en) 1992-12-10 1992-12-10 Ice probe
GB9324826A GB2277992B (en) 1992-12-10 1993-12-03 A sensor arrangement
US08/546,002 US5627310A (en) 1992-12-10 1995-10-20 Sensor arrangement for ice bank control

Publications (3)

Publication Number Publication Date
GB9324826D0 GB9324826D0 (en) 1994-01-19
GB2277992A true GB2277992A (en) 1994-11-16
GB2277992B GB2277992B (en) 1996-09-18

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Family Applications (1)

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GB9324826A Expired - Fee Related GB2277992B (en) 1992-12-10 1993-12-03 A sensor arrangement

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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1197565A (en) * 1966-09-08 1970-07-08 Joshua Creer Quayle A Continuous Flow Cryometer
GB2078955A (en) * 1980-06-26 1982-01-13 Atomic Energy Authority Uk Improvements in detecting an interface between two media
GB2202944A (en) * 1987-03-11 1988-10-05 Schlumberger Electronics Vibrating element fluid transducer

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1197565A (en) * 1966-09-08 1970-07-08 Joshua Creer Quayle A Continuous Flow Cryometer
GB2078955A (en) * 1980-06-26 1982-01-13 Atomic Energy Authority Uk Improvements in detecting an interface between two media
GB2202944A (en) * 1987-03-11 1988-10-05 Schlumberger Electronics Vibrating element fluid transducer

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Publication number Publication date
GB9324826D0 (en) 1994-01-19
GB2277992B (en) 1996-09-18

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Legal Events

Date Code Title Description
911A Proceeding under rule 110(4) of the patent rules 1990
732E Amendments to the register in respect of changes of name or changes affecting rights (sect. 32/1977)
PCNP Patent ceased through non-payment of renewal fee

Effective date: 20051203