GB2265005A - Liquid level sensor - Google Patents

Liquid level sensor Download PDF

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Publication number
GB2265005A
GB2265005A GB9304579A GB9304579A GB2265005A GB 2265005 A GB2265005 A GB 2265005A GB 9304579 A GB9304579 A GB 9304579A GB 9304579 A GB9304579 A GB 9304579A GB 2265005 A GB2265005 A GB 2265005A
Authority
GB
United Kingdom
Prior art keywords
tube
liquid
sensor according
transducer
ultrasonic
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
GB9304579A
Other versions
GB9304579D0 (en
GB2265005B (en
Inventor
David Sinclair
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.)
Smiths Group PLC
Original Assignee
Smiths Group PLC
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 GB929205148A external-priority patent/GB9205148D0/en
Application filed by Smiths Group PLC filed Critical Smiths Group PLC
Priority to GB9304579A priority Critical patent/GB2265005B/en
Publication of GB9304579D0 publication Critical patent/GB9304579D0/en
Publication of GB2265005A publication Critical patent/GB2265005A/en
Application granted granted Critical
Publication of GB2265005B publication Critical patent/GB2265005B/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F23/00Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
    • G01F23/22Indicating 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
    • G01F23/28Indicating 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
    • G01F23/296Acoustic waves
    • G01F23/2968Transducers specially adapted for acoustic level indicators
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F23/00Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
    • G01F23/22Indicating 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
    • G01F23/28Indicating 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
    • G01F23/296Acoustic waves
    • G01F23/2961Acoustic waves for discrete levels
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F23/00Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
    • G01F23/22Indicating 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
    • G01F23/28Indicating 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
    • G01F23/296Acoustic waves
    • G01F23/2962Measuring transit time of reflected waves

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Electromagnetism (AREA)
  • Thermal Sciences (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)

Abstract

An ultrasonic liquid level sensor has a transducer 68 mounted at the lower end of an aluminium tube 30 that projects upwardly in a liquid tank (4) so that the tube is filled with liquid (6) to the same height as that outside the tube. Internally, the tube has a layer 32 of an acoustically- absorbing plastics to damp the transmission of ultrasonic vibration from the wall of the tube into liquid within the tube. In use, energy is directed up towards the liquid/air interface which reflects the energy back down to the transducer 68. By measuring the time taken between transmission and reception of an energy pulse, it is possible to determine the distance between the transducer 68 and the liquid/air interface, and from this, the depth of the liquid (6). <IMAGE>

Description

<Desc/Clms Page number 1>
LIQUID-LEVEL GAUGING This invention relates to liquid-level gauging.
The invention is more particularly concerned with ultrasonic liquid-level gauging sensors.
Ultrasonic liquid-level sensors utilize the fact that ultrasonic vibrations travel freely in a liquid but are rapidly attenuated in air or other gas. If an ultrasonic transducer is mounted on the base of a liquid reservoir so that it directs energy up towards the liquid/air interface, the energy will be reflected back down to the transducer by this interface. By measuring the time taken between transmission and reception of an energy pulse, it is possible to measure the distance between the transducer and the liquid/air interface and, from this, the depth of liquid.
It is common practice for ultrasonic transducers of this kind to be mounted at the lower end of a tube that extends from the bottom to the top of the liquid reservoir. The tube is open at the bottom so that liquid fills the tube to the same depth as in the reservoir outside the tube.
The tube serves several purposes. It helps isolate the transducer from other sensors or sources of interference. It also confines the ultrasonic beam, so that it is directed only at the region of the liquid surface directly above the transducer. Furthermore, the tube produces within it a region of liquid surface that is substantially damped of waves.
Another advantage arising out of the use of the tube is that it is easy to provide a reference height, by mounting some form of reflector at a known height within the tube. In this way, the transducer will receive a reflection from the liquid surface and one from the reference reflector against which the liquid height can be calibrated. This enables the ultrasonic gauging system to compensate for different liquids having different acoustic propagation properties and for temperature variations which can affect ultra-sound propagation. An
<Desc/Clms Page number 2>
example of an ultrasonic probe having a tube of this kind is described in, for example, EP 0106677.
There are various problems with existing ultrasonic liquid gauging sensors. One problem arises from the fact that, in addition to the ultra-sound energy being transmitted through the liquid within the tube, energy is also propagated within the wall of the tube itself.
This can lead to propagation from the wall into the liquid, especially at locations where the tube wall is clamped for support purposes, and hence to false echoes being received by the transducer. Attempts to reduce this problem have included the use of tubes made from plastics materials which are less prone to the generation of stray echoes. This, however, causes another problem in that, because plastics are not as rigid as metals, the wall of the tube has to be relatively thick in order to produce the necessary rigidity with a consequent increase in weight.
In aircraft fuel gauging applications where a dozen or more fuel gauging probes might be used, the weight can be considerable and lead to appreciable increases in operational costs.
A further difficulty with these sensors is caused where ultrasonic energy does not pass axially along the tube since this gives rise to multiple echoes and an increase in path length with a consequent time delay. This is especially a problem where the liquid surface is not at right angles to the tube axis since a majority of the reflected signals will not pass axially along the tube. Although the signals that are reflected axially along the tube can be sufficient to enable the height of liquid to be determined, these signals can be masked by strong signals caused by multiple reflection from the wall of the tube.
It is an object of the present invention to provide an ultrasonic liquid level sensor which can be used to alleviate at least some of these problems.
According to one aspect of the present invention there is provided an ultrasonic liquid level sensor including an ultrasonic transducer mounted towards the lower end of a tube arranged to extend upwardly and to be filled with liquid to the same height as liquid outside the
<Desc/Clms Page number 3>
tube, the tube being made of a first, rigid material and having a surface layer along a major part at least of the length of the tube that is of a second material, different from the first and that is acoustically-absorbing so as to damp the transmission of ultrasonic vibration from the wall of the tube into liquid within the tube.
In this way, it is possible to form a tube which has similar acoustic properties to one which is made entirely of a plastic material; the strength of the first material, however, enables the tube to have a thinner wall and considerably lower weight than an equivalent plastic tube.
Preferably, the first, rigid material is a metal, such as aluminium, although it may be a glass-fibre reinforced plastics. The surface layer is preferably on the inside of the tube and may be of a plastics such as a polysulphide applied as a coating to the tube. The transducer is preferably mounted in an acoustic isolator that substantially reduces the amount of energy transmitted to and from the wall of the tube.
An ultrasonic sensor for an aircraft fuel-gauging system, in accordance with the present invention, will now be described, by way of example, with reference to the accompanying drawings, in which: Figure 1 is a side elevation view of the sensor in an aircraft fuel tank; and Figure 2 is an enlarged sectional side elevation view of the sensor;
<Desc/Clms Page number 4>
With reference to Figure 1, the sensor 2 is mounted vertically in a tank 4 of an aircraft containing liquid fuel 6. The sensor 2 is supported by two clamps 8 and 10 which are secured to the upper and lower end of the sensor respectively and to the wall of the tank 4. The drive signal to the sensor and its electrical output are taken from the lower end of the sensor via a cable 12 to a control unit 13 including a fuel gauging computer which computes the volume of fuel from the height information provided by the sensor and from knowledge of the tank shape.
The output from the control unit 13 is supplied to a display 14, or other utilization means, which may be in terms of either volume or mass if a density input is provided.
With reference now also to Figure 2, the sensor 2 comprises a tubular assembly 15 and a base assembly 16 mounted at the lower end of the tubular assembly.
The tubular assembly 15 is about 530mm long and has an external diameter of about 25mm. The assembly is made up from a cylindrical tube 30 of metal, such as aluminium, which has a wall thickness of about 0. 5mm and a coated layer 32 on its inside of an acousticallyabsorbing plastics material such as a two-part polysulphide or similar plastics material. The thickness of the layer 32 is not critical and is typically about equal to the wall thickness of the tube 30, being between about 0.4 to 0.5mm. The layer of acoustically-absorbing material could instead be applied to the outside of the tube although the improvement this produces is not as great as for an internal layer. The coating can be carried out by any conventional technique such as by pouring the coating material in a liquid form though the tube. At its upper end, the assembly 15 is closed by a metal cap 33 soldered to the tube 30. At its lower end, the assembly is open to fuel within the tank 4 through four equally-spaced slots 34 around the lower end of the tube 30. One or more reference reflectors 35 extend through the wall of the tubular assembly 15 at points along its length.
<Desc/Clms Page number 5>
The base assembly 16 includes an inner support structure 60 with a tubular sleeve 61 that embraces the lower end of the tube 30, the sleeve having slots 62 that align with the slots 34 in the tube. At its upper end, the support structure 60 has a radially-extending flange 63.
On one side, this is secured with the tube 30 by means of a metal strap 64 which is brazed to the outside of the tube at one end and is bolted to the flange 63 at its other end. A mounting bracket 65 projects vertically from the flange 63, this being attached to the clamp 10 at the lower end of the sensor. At the lower end of the base assembly 16 there is a transducer assembly 66 which comprises a mounting plate 67 and an ultrasonic transducer 68 potted onto the underside of the plate with an acoustically-absorbing plastics 69 such as polysulphide. The transducer 68 is positioned on the axis of the tube 30 and its wires 70 extend into a terminal block 71, the hollow space around the wires being potted with a plastics material that is slightly conductive electrically, such as a polysulphide with a dispersed conductive powder. This provides a safety leakage path with a resistance of the order of several thousand ohms to prevent charge built-up in the event of damage to the sensor 2. The mounting plate 67 is of a plastics material such as polyphenylene sulphide and its thickness is such that it enables the axial beam of energy from and to the transducer to pass through the plate without substantial attenuation. The plastics material of the plate 67, however, with the potting material 69, acts as an acoustic isolator, isolating the transducer from the tubular assembly 15.
The base assembly 16 is completed by a cylindrical outer cover 72 which encloses the structure 60 and the transducer assembly 66. Apertures 73 towards the lower end of the cover 72 allow fuel to flow into and out of the base assembly 16, and hence, into and out of the tubular assembly 15.
In use, the control unit 13 energizes the transducer 68 with electrical pulses that cause the transducer to emit ultrasonic energy pulses with a frequency of about 111Hz and a pulse repetition frequency of about 1 second. The ultrasonic energy is directed vertically upwards, along the axis of the tubular assembly 15.
<Desc/Clms Page number 6>
Each pulse of ultrasonic energy travels axially up the assembly 15 within the fuel 6 until it meets the interface with the air or gas in the tank 4 above the fuel. At this point the energy pulse is reflected downwardly back to the transducer 68. The transducer 68 will also receive an echo pulse arising from reflection from the reflectors 35. These echo pulses provide calibration pulses against which the echo from the liquid surface can be calibrated. The coating 32 on the inside of the assembly 15 reduces considerably both the amount of energy transferred to the tube 30 from the fuel within the tube and the amount of energy transferred from the tube to the fuel. This leads to a considerably cleaner output signal, that is, one with far less spurious noise than would be produced by a metal tubular assembly that did not have a similar coating. It has not been possible previously to use metal tubes because of the high noise levels. The performance of tubes made from other rigid materials such as a rigid glass-fibre reinforced plastic can also be improved by coating with a different, acoustically-absorbing material. More
particularly, a tubular assembly may be made of a resin-impregnated glass-fibre strip, such as . (P, (r) Fiberite/from ICI Fiberite in California, USA, wound onto a polybutadiene tube, such as Buna 1 2 CB made by Bayer AG of Leverkusen, Germany. After curing, the glass-fibre provides a rigid outer structure with the polybutadiene tube providing an elastic, acoustically-absorbing inner layer.
Because the plastics material surrounding the transducer 68 is of an acoustically- absorbing material, it acts to isolate the transducer from the tubular assembly 15. This reduces further the amount of energy propagated from the transducer 68 into the tube wall and hence reduces both the external interference caused by the sensor to other sensors and the amount of energy propagated into the fuel within the sensor from the wall.
[Y : \PATENTS\SPEC\92\UFGP. DOC] 04/03/93

Claims (11)

1. An ultrasonic liquid level sensor including an ultrasonic transducer mounted towards the lower end of a tube arranged to extend upwardly and to be filled with liquid to the same height as liquid outside the tube, wherein the tube is made of a first, rigid material and has a surface layer along a major part at least of the length of the tube that is of a second material, different from the first and that is acoustically-absorbing so as to damp the transmission of ultrasonic vibration from the wall of the tube into liquid within the tube.
2. A sensor according to Claim 1, wherein the first, rigid material is a metal.
3. A sensor according to Claim 2, wherein the metal is aluminium.
4. A sensor according to Claim 1, wherein the first material is of glass-fibre reinforced plastics.
5. A sensor according to any one of the preceding claims, wherein the surface layer is on the inside of the tube.
6. A sensor according to any one of the preceding claims, wherein the second material is a plastics material.
7. A sensor according to Claim 6, wherein the plastics material is a polysulphide.
<Desc/Clms Page number 8>
8. A sensor according to any one of the preceding claims, wherein the second material is applied as a coating.
9. A sensor according to any one of the preceding claims, wherein the transducer is mounted in an acoustic isolator that substantially reduces the amount of energy transmitted to and from the wall of the tube.
10. A sensor substantially as hereinbefore described with reference to the accompanying drawings.
11. Any novel feature or combination of features as hereinbefore described.
GB9304579A 1992-03-10 1993-03-05 Liquid-level gauging Expired - Lifetime GB2265005B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
GB9304579A GB2265005B (en) 1992-03-10 1993-03-05 Liquid-level gauging

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
GB929205148A GB9205148D0 (en) 1992-03-10 1992-03-10 Liquid level gauging
GB9304579A GB2265005B (en) 1992-03-10 1993-03-05 Liquid-level gauging

Publications (3)

Publication Number Publication Date
GB9304579D0 GB9304579D0 (en) 1993-04-21
GB2265005A true GB2265005A (en) 1993-09-15
GB2265005B GB2265005B (en) 1995-06-21

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GB9304579A Expired - Lifetime GB2265005B (en) 1992-03-10 1993-03-05 Liquid-level gauging

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2333156A (en) * 1998-01-13 1999-07-14 Whitlenge Drink Equipment Ltd Method and apparatus for detecting an interface
EP1069411A1 (en) * 1999-07-10 2001-01-17 SONOTEC Dr. zur Horst-Meyer und Münch OHG Device for measuring continuously the level in fuel tanks
DE19934876B4 (en) * 1998-08-12 2009-11-12 Ge Aviation Uk Füllstandsmeßsystem
DE19637978B4 (en) * 1995-10-04 2012-04-05 Ontic Engineering & Manufacturing Uk Ltd. Fluidmengenmeßsystem

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102012212210A1 (en) * 2012-07-12 2014-01-16 Continental Automotive Gmbh Method and apparatus for determining a height of a fluid level in a fluid container

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19637978B4 (en) * 1995-10-04 2012-04-05 Ontic Engineering & Manufacturing Uk Ltd. Fluidmengenmeßsystem
GB2333156A (en) * 1998-01-13 1999-07-14 Whitlenge Drink Equipment Ltd Method and apparatus for detecting an interface
GB2333156B (en) * 1998-01-13 2002-03-20 Whitlenge Drink Equipment Ltd Apparatus and method for detecting an interface
DE19934876B4 (en) * 1998-08-12 2009-11-12 Ge Aviation Uk Füllstandsmeßsystem
EP1069411A1 (en) * 1999-07-10 2001-01-17 SONOTEC Dr. zur Horst-Meyer und Münch OHG Device for measuring continuously the level in fuel tanks

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Publication number Publication date
GB9304579D0 (en) 1993-04-21
GB2265005B (en) 1995-06-21

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732E Amendments to the register in respect of changes of name or changes affecting rights (sect. 32/1977)
732E Amendments to the register in respect of changes of name or changes affecting rights (sect. 32/1977)

Free format text: REGISTERED BETWEEN 20111222 AND 20111223

PE20 Patent expired after termination of 20 years

Expiry date: 20130304