NO154648B - SENSOR ELEMENT FOR CAPACITY LEVEL MEASUREMENT SYSTEM. - Google Patents
SENSOR ELEMENT FOR CAPACITY LEVEL MEASUREMENT SYSTEM. Download PDFInfo
- Publication number
- NO154648B NO154648B NO840812A NO840812A NO154648B NO 154648 B NO154648 B NO 154648B NO 840812 A NO840812 A NO 840812A NO 840812 A NO840812 A NO 840812A NO 154648 B NO154648 B NO 154648B
- Authority
- NO
- Norway
- Prior art keywords
- sensor element
- self
- capacitor
- heating cable
- metal
- Prior art date
Links
- 238000005259 measurement Methods 0.000 title claims description 13
- 239000003990 capacitor Substances 0.000 claims description 19
- 239000007788 liquid Substances 0.000 claims description 19
- 238000010438 heat treatment Methods 0.000 claims description 13
- 239000002184 metal Substances 0.000 claims description 13
- 229910052751 metal Inorganic materials 0.000 claims description 13
- 239000011248 coating agent Substances 0.000 claims description 9
- 238000000576 coating method Methods 0.000 claims description 9
- 239000000463 material Substances 0.000 claims description 8
- 229920002313 fluoropolymer Polymers 0.000 claims description 7
- 239000004811 fluoropolymer Substances 0.000 claims description 7
- 239000012530 fluid Substances 0.000 claims description 6
- 239000004065 semiconductor Substances 0.000 claims description 5
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims description 5
- 239000004020 conductor Substances 0.000 claims description 4
- 239000000126 substance Substances 0.000 claims description 4
- 239000000523 sample Substances 0.000 description 6
- 238000009413 insulation Methods 0.000 description 4
- 241000549343 Myadestes Species 0.000 description 3
- 230000005684 electric field Effects 0.000 description 2
- 101100279442 Caenorhabditis elegans egg-6 gene Proteins 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 208000012868 Overgrowth Diseases 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 239000002360 explosive Substances 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 239000012466 permeate Substances 0.000 description 1
- 239000004033 plastic Substances 0.000 description 1
- 239000013535 sea water Substances 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
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
- G01F23/26—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 variations of capacity or inductance of capacitors or inductors arising from the presence of liquid or fluent solid material in the electric or electromagnetic fields
- G01F23/263—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 variations of capacity or inductance of capacitors or inductors arising from the presence of liquid or fluent solid material in the electric or electromagnetic fields by measuring variations in capacitance of capacitors
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Electromagnetism (AREA)
- Thermal Sciences (AREA)
- Fluid Mechanics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
- Measurement Of Resistance Or Impedance (AREA)
- Measurement Of Current Or Voltage (AREA)
Description
Oppfinnelsen angår st forbedrer, sansorelemont til bruk i The invention relates to improving, sensor elements for use in
et. kaps.sit.lvt målesystem for nivået av en elektrisk ledende væskes grenseflata mot et ovenforliggende ikke-ledende fludium. 5om eksempel pa ledende væske kan nevnes vann, særlig sjøvann, og ikke-ledende fludium kan eksempelvis vare luft eller olje. a. kaps.sit.lvt measuring system for the level of an electrically conductive liquid's interface with an overlying non-conductive fluid. Examples of conductive fluids include water, especially seawater, and non-conductive fluids can be, for example, air or oil.
Vad de fleste kjente kapasitive nivåmålesystemer benytter man forskjellen i dielektrisitetskonstant mellom væsken og det ovenforliggende medium. Målesondon kan utføres på forskjellige måter. Ln kjent sonde har f.eks. form som to lange, elektrisk ladende rar, anordnet konsentrisk, idet hvert av rørene er en "plate" i en kondensator. In most known capacitive level measurement systems, the difference in dielectric constant between the liquid and the medium above is used. Measuring probes can be carried out in different ways. Ln known probe has e.g. form as two long, electrically charged tubes, arranged concentrically, each of the tubes being a "plate" in a capacitor.
i-.n annen type har form som ligner på. en antennefiatkabe!, i-.n other type has shape similar to. an antenna fiat cable!,
so tverrsnitt vist i fig. 1 . O' et elektriske feltet mellom de to "kondensatorplatene", som her er de to laderne i kabelen, strekker seg ut i det omgivende mediet, og kapasi-tanssn avhenger dermed av mediets dielektrisitetskonstant. so cross section shown in fig. 1. O' an electric field between the two "capacitor plates", which here are the two chargers in the cable, extends into the surrounding medium, and the capacitance thus depends on the dielectric constant of the medium.
<:>£t problam med dette måleprinsipp er imidlertid at dielektri-sitetskonstanten i væsken sjelden eller aldri er konstant. Dessuten er kapasitetsforandringen som måles med de kjente sonder av danne type svært liten, og vanskelig å nåle nøy-aktig. F.eks. gir to konsentriske rør en kapasitetsforand-ring av størrelsesorden IDO pF/m. Videre finnes problemer med nullpunktsdrift, p.g.a. at en vesentlig kspssitans også er tilstede når sondefi ikke er omgitt av væske. Sluttelig har det vist seg vanskelig å lage slike sonder som er mekanisk stabile med hensyn på tempsraturutvidelssr. The problem with this measuring principle, however, is that the dielectric constant in the liquid is rarely or never constant. Moreover, the change in capacity measured with the known probes of this type is very small, and difficult to pinpoint precisely. For example gives two concentric tubes a capacity change of the order of magnitude IDO pF/m. Furthermore, there are problems with zero-point operation, due to that a significant pressure is also present when the probe is not surrounded by liquid. Finally, it has proved difficult to make such probes which are mechanically stable with regard to temperature expansion.
Et annet prinsipp er beskrevet i britisk patentskrift 1.31B.512. Dette prinsippet baserer seg på at ett av mediene, primært vasken nederst, er elektrisk ledende og sørger for kontakt fra en utenforliggende metallelektrode inn til et tynt isolasjonsbelegg som er festet på en innenforliggende, langstrakt "kcndensatorplate", som gjerne har sylindrisk form. jermed utgjøres altså den andre "kondensatorplaten" av selva den elektrisk ledende væsken, mens isolasjonsbelegget ar kondensatorens ciislektrikum. dåisd33 or det altså i hovedsak a realet (dvs.longrisn ) av "kondsnsatorpiatena" som sr den variabl» størrelsen. V od Another principle is described in British patent document 1.31B.512. This principle is based on the fact that one of the media, primarily the sink at the bottom, is electrically conductive and ensures contact from an external metal electrode to a thin insulating coating that is attached to an internal, elongated "condenser plate", which is usually cylindrical in shape. thus the second "capacitor plate" is made up of the electrically conductive liquid itself, while the insulating coating is the capacitor's dielectric. dåisd33 it is therefore mainly the real (i.e. longitudinal) of the "condensator piates" which is the variable size. V od
□ rak 11 s k b r u k av denne k j o n t o m å i e s o n d en o p p s t f. r .imi. ei .1 a r ii d problemer med manglende mekanisk stabilitet ved ternpsratur-svingnin<g>ar. Uette gir lav målenøyaktighet. Dessuten finnec et reelt problem med tilgroing av sonden. Bads biologisk tilgroing og uorganiske avleiringer kan forårsake feil-målinger og gi et upålitelig system. □ rak 11 s k b r u k of this k j o n t o m o i e s o n d an o p p s t f. r .imi. ei .1 a r ii d problems with a lack of mechanical stability during temperature fluctuations. Uette gives low measurement accuracy. In addition, there is a real problem with overgrowth of the probe. Bath biofouling and inorganic deposits can cause incorrect measurements and result in an unreliable system.
["led sansorelemsntst ifølge oppfinnelsen, som sr basert på sistnevnte måleprinsipp, oppnås at problemet, med kapasitansmålefeil p.g.a. temperatursvingninger er eliminert, samt. ["led sensor element according to the invention, which is based on the latter measurement principle, it is achieved that the problem with capacitance measurement errors due to temperature fluctuations is eliminated, as well as.
at levetiden for elementet økas vesentlig. Videre hindres i vesentlig grad tilgroing av sensorelemantst. that the lifespan of the element is significantly increased. Furthermore, growth of sensor elements is prevented to a significant extent.
elementet kan dessuten brukes i brann- og eksplosjonsfar]ige miljøer og er ekstremt motstandsdyktig overfor kjemiske på-virkninger. I forhold til de konvensjonelle forannevnte systemer oppnås også en kraftig okning av kapasitanssndring pr. meter væske, typisk over 500 pF'/m. the element can also be used in fire and explosive environments and is extremely resistant to chemical influences. In relation to the conventional systems mentioned above, a sharp increase in capacitance change per meter of liquid, typically over 500 pF'/m.
Dette oppnås ifølge oppfinnelsen ved at metall-elektroden This is achieved according to the invention by the metal electrode
i kondensatoren utgjøres av skjerman på en selvregulerando varmekabel. in the condenser is made up of the screen on a self-regulating heating cable.
rin nærmere beskrivelse av oppfinnelsen føTger, med henvis-ning til figurene, hvor fig. 1 viser en tidligere kjent kapasitiv,:isensorkabal i tverrsnitt, fig. 2 viser en sensorkabel ifølga oppfinnelsen, også i tverrsnitt, mens fig. 5 viser et enkelt elektrisk ekvivalentskjerna fer kabelen og væsken. A more detailed description of the invention follows, with reference to the figures, where fig. 1 shows a previously known capacitive sensor cable in cross-section, fig. 2 shows a sensor cable according to the invention, also in cross section, while fig. 5 shows a simple electrical equivalent core fer the cable and the liquid.
En typisk, vanlig brukt sensorkabel for kapasitiv nivå-måling i væsken, basert på prinsippet om forskjellige di-elektrisitetskonstanter, er vist i tverrsnitt på fig. i. Kapasitcnsen måles mellom de to kooperlederne 1 som ar omsluttet i hele sin lengde av en plastisolasjon 2, og avhenger av det omgivende mediets 3 dielektrisitetskonstant, 'la dat elektriske feltet son antydet figuren også. gjennomtrenger mediet j>. I praksis, med kabalen strukket ned i et reservoar el].er en tank, vil nivået for overgangen mellom do to aktuelle mediene 1, f.eks. vann og luft, bestemme den totals kapasitansen for kabelen. A typical, commonly used sensor cable for capacitive level measurement in the liquid, based on the principle of different dielectric constants, is shown in cross-section in fig. i. The capacitance is measured between the two copper conductors 1, which are enclosed along their entire length by a plastic insulation 2, and depends on the dielectric constant of the surrounding medium 3, 'let the electric field as the figure also indicated. permeates the medium j>. In practice, with the solitaire stretched down into a reservoir or a tank, the level for the transition between the two relevant media 1, e.g. water and air, determine the total capacitance of the cable.
I fig. 2 vises et tverrsnitt av et sensorelement ifnlgo oppfinnelsen, som også i hovedsak er en kabal som strokkes ned i et reservoar eller en tank....'at nngivande medium <'■ In fig. 2 shows a cross-section of a sensor element according to the invention, which is also essentially a solitaire that is lowered into a reservoir or a tank...
sr en elektrisk ledende vaske, eksempelvis vann, evaniuoit st ikke-ledende fluidum, eksempelvis olje, avhengig av i hvilken høyde snittet ar lagt. in jord ingsoi ektrode r av bart metall er ført ned sammen mad kabelen, og er i eksempelet på fig. 2 vist med sylindrisk form. Formen ar dog ikke avgjørande, da elektrodene 5 hensikt bara er å gi alsktrisk kontakt til den ladende væsken. Den affektive kondensator dannes der den ledende væsken finnes, med selve denne væsken som "kondensatorplate" inntil et dielektrikum som utgjøres av en varmekabels ytra isolas jonsbel.egg 6. sr an electrically conductive wash, for example water, evaniuoit st non-conductive fluid, for example oil, depending on the height at which the cut is placed. in earth ingsoi ektrode r of bare metal is brought down together with the cable, and is in the example in fig. 2 shown with cylindrical shape. However, the shape is not decisive, as the purpose of the electrodes 5 is only to provide electrical contact to the charging liquid. The affective capacitor is formed where the conductive liquid is found, with this liquid itself as the "capacitor plate" next to a dielectric which is made up of a heating cable's outer insulation. Egg 6.
På innsiden av dielektrikumet 6 er kondensatorens andre "plate", nemlig varmekabelens metallskjerm 7. Kondensatorens kapasitans måles altså mellom varmekabelens skjerm 7 og den ledende væsken, som en får elektrisk kontakt med via jordingselektroden 5. On the inside of the dielectric 6 is the capacitor's second "plate", namely the heating cable's metal shield 7. The capacitor's capacitance is thus measured between the heating cable's shield 7 and the conductive liquid, with which one makes electrical contact via the grounding electrode 5.
Det ytre isolasjonsbelsgget 6 på varmekabelen er laget The outer insulation seal 6 on the heating cable is made
av en spesiell fluorpolymer med svært glatt overflate, hvilket motvirker tilgroing av både kjemisk og biologisk type. Det foretrukne materiale er en modifisert fluorpolymer med varemerket "Tefzei", som fremstilles av Du Pont de Nemours & Co., USmI Materialet er også særdeles motstandsdyktig overfor kjemisk angrep. of a special fluoropolymer with a very smooth surface, which counteracts fouling of both chemical and biological types. The preferred material is a modified fluoropolymer under the trademark "Tefzei" manufactured by Du Pont de Nemours & Co., USmI The material is also highly resistant to chemical attack.
Varmekabelen er innenfor skjermen 7 forsynt med et isola-sjonslag 8, fortrinsvis av fluorpolymermaterials. The heating cable is provided within the screen 7 with an insulation layer 8, preferably of fluoropolymer material.
Innenfor laget 3 befinner selve varmeelemantet seg, som er et halvledermateriale 9, som fyller opp kjernen i kabelen. To metall-ladere 10 ar innleiret i kjernen. I bruk er de to metall-lsderne 10 tilkoplet en spenningskilde, f.eks. 220 voltvskseispenning. Within layer 3 is the heating element itself, which is a semiconductor material 9, which fills up the core of the cable. Two metal chargers 10 ar embedded in the core. In use, the two metal sensors 10 are connected to a voltage source, e.g. 220 volts.
Halvledermaterialets 9 egenskaper (dv/s . temperaturavhengig resistivitet) medfører at en viss temperatur holdes konstant langs hele kabelens lengde. For det første fjernes dermed problemet med kapasitansmålefeil tilknyttet temperaturvariasjoner, og for det andre medfører an konstant kabeitemperatur på f.eks. 80 gr.Celcius at biologisk tilgroing reduseres. Dette vil også hindre tilising og even-tuelle olje/voksbelegg på kabelen. The semiconductor material's 9 properties (dv/s . temperature-dependent resistivity) mean that a certain temperature is kept constant along the entire length of the cable. Firstly, the problem of capacitance measurement errors associated with temperature variations is thereby removed, and secondly, a constant cable temperature of e.g. 80 degrees Celsius that biological growth is reduced. This will also prevent icing and any oil/wax coating on the cable.
Formen og de relative dimensjoner i fig. 2 er tilfeldige. Kabelen har ikke nødvendigvis sirkulærsylindrisk form, The shape and relative dimensions in fig. 2 are random. The cable does not necessarily have a circular cylindrical shape,
men kan f.eks. likne på en flatkabal. but can e.g. similar to a flat solitaire.
En standard selvregulerende varmekabel som ved forsøk har vist seg å fungere utmerket som sentralelement i kondsn-satoranordningen ifølge oppfinnelsen, produseres av Raychem Corporation, USA under betegnelsen "Chemelex Auto-Trace QTV2-CT". Kabelen viser seg å være svært stabil A standard self-regulating heating cable which has been shown to function excellently as a central element in the condenser device according to the invention is manufactured by Raychem Corporation, USA under the designation "Chemelex Auto-Trace QTV2-CT". The cable proves to be very stable
både mekanisk, kjemisk og med hensyn til temperatur. both mechanically, chemically and with regard to temperature.
I fig. 3 er vist en elektrisk ekvivalentkrets til ytter-ligere belysning av sensorelementets virkemåte. Punktet 14 representerer jordingselektroden 5 i fig. 2. I realiteten må en regne med at den elektrisk ledende væsken har en viss resistans Rv. Heri inkluderes også en kontaktmotstand i grenseflaten mellom jordingselektroden og væsken. In fig. 3 shows an electrical equivalent circuit for further illumination of the sensor element's operation. The point 14 represents the grounding electrode 5 in fig. 2. In reality, one must assume that the electrically conductive liquid has a certain resistance Rv. This also includes a contact resistance in the interface between the grounding electrode and the liquid.
Forøvrig representeres den ledende væsken rfærmest kabelen som en kondensatorplate 15. Dielektrikumet 16 i kondensatoren tilsvarer isolasjonsbelegget 6, og kondensatorsiden 17 representerer metallskjermen 7. Det fremgår således at resistansen Ru, som må foruentes å være uariabel med niuået som måles og også over tid, vil influere på målingene. Den målebroen som konstrueres til kapasitans-målingen, kan imidlertid innrettes slik at variasjoner i Ru betyr lite for måleresultatet. Incidentally, the conducting liquid nearer the cable is represented as a capacitor plate 15. The dielectric 16 in the capacitor corresponds to the insulating coating 6, and the capacitor side 17 represents the metal screen 7. It thus appears that the resistance Ru, which must be assumed to be invariable with the current being measured and also over time, will influence the measurements. The measuring bridge that is constructed for the capacitance measurement can, however, be arranged so that variations in Ru mean little for the measurement result.
Claims (5)
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NO840812A NO154648C (en) | 1984-03-05 | 1984-03-05 | SENSOR ELEMENT FOR CAPACITY LEVEL MEASUREMENT SYSTEM. |
PCT/NO1985/000012 WO1985004008A1 (en) | 1984-03-05 | 1985-03-04 | Sensing element for a capacitive level measuring system |
EP19850901099 EP0174333A1 (en) | 1984-03-05 | 1985-03-04 | Sensing element for a capacitive level measuring system |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NO840812A NO154648C (en) | 1984-03-05 | 1984-03-05 | SENSOR ELEMENT FOR CAPACITY LEVEL MEASUREMENT SYSTEM. |
Publications (3)
Publication Number | Publication Date |
---|---|
NO840812L NO840812L (en) | 1985-09-06 |
NO154648B true NO154648B (en) | 1986-08-11 |
NO154648C NO154648C (en) | 1986-11-19 |
Family
ID=19887518
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
NO840812A NO154648C (en) | 1984-03-05 | 1984-03-05 | SENSOR ELEMENT FOR CAPACITY LEVEL MEASUREMENT SYSTEM. |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP0174333A1 (en) |
NO (1) | NO154648C (en) |
WO (1) | WO1985004008A1 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE4131582A1 (en) * | 1991-09-23 | 1993-03-25 | Elektro Merseburg Gmbh I G | Capacitive level measurement device for liquids or bulk material - uses measurement-, screening- and base-electrodes with intermediate insulation, and operates as capacitive potential divider |
EP1677085A3 (en) * | 2004-12-31 | 2007-08-01 | Moonhaven LLC | Capacitive level sensor |
Family Cites Families (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB1318512A (en) * | 1969-03-12 | 1973-05-31 | Greater London Council | Apparatus for detecting changes in the level of a pourable material |
US3706980A (en) * | 1970-04-27 | 1972-12-19 | Drexelbrook Controls | Rf system for measuring the level of materials |
FR2129245A5 (en) * | 1971-03-19 | 1972-10-27 | Pennaneach Marcelle | |
US4064753A (en) * | 1974-12-12 | 1977-12-27 | Drexelbrook Controls, Inc. | RF admittance measuring method and apparatus for determining the level of a conductive liquid |
US4122718A (en) * | 1975-07-16 | 1978-10-31 | Gustafson Reuben V | Liquid level sensor |
US4242573A (en) * | 1979-01-24 | 1980-12-30 | Raychem Corporation | Water immersible heater |
US4301681A (en) * | 1979-09-06 | 1981-11-24 | Drexelbrook Controls, Inc. | Method of using capacitor probe with a semiconductive electrode |
US4412270A (en) * | 1981-06-25 | 1983-10-25 | Simmonds Precision Products, Inc. | Electrode assembly for a capacitance type probe |
-
1984
- 1984-03-05 NO NO840812A patent/NO154648C/en unknown
-
1985
- 1985-03-04 WO PCT/NO1985/000012 patent/WO1985004008A1/en unknown
- 1985-03-04 EP EP19850901099 patent/EP0174333A1/en not_active Withdrawn
Also Published As
Publication number | Publication date |
---|---|
NO154648C (en) | 1986-11-19 |
EP0174333A1 (en) | 1986-03-19 |
NO840812L (en) | 1985-09-06 |
WO1985004008A1 (en) | 1985-09-12 |
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