WO1985002016A1 - An apparatus for the measurement of the fraction of gas in a two-component fluid flow comprising a liquid and a gas in mixture - Google Patents

An apparatus for the measurement of the fraction of gas in a two-component fluid flow comprising a liquid and a gas in mixture Download PDF

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Publication number
WO1985002016A1
WO1985002016A1 PCT/NO1984/000046 NO8400046W WO8502016A1 WO 1985002016 A1 WO1985002016 A1 WO 1985002016A1 NO 8400046 W NO8400046 W NO 8400046W WO 8502016 A1 WO8502016 A1 WO 8502016A1
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Prior art keywords
gas
electrodes
mixture
measurement
potential
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Application number
PCT/NO1984/000046
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French (fr)
Inventor
Richard Thorn
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Equinor ASA
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Den Norske Stats Oljeselskap AS
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Priority to DE8484903894T priority Critical patent/DE3476122D1/en
Priority to FI852602A priority patent/FI852602A0/en
Publication of WO1985002016A1 publication Critical patent/WO1985002016A1/en
Priority to DK292085A priority patent/DK153587C/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
    • G01N33/26—Oils; Viscous liquids; Paints; Inks
    • G01N33/28—Oils, i.e. hydrocarbon liquids
    • G01N33/2823—Raw oil, drilling fluid or polyphasic mixtures
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N27/00—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means
    • G01N27/02—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance
    • G01N27/22—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance by investigating capacitance
    • G01N27/221—Investigating or analysing materials by the use of electric, electrochemical, or magnetic means by investigating impedance by investigating capacitance by investigating the dielectric properties

Definitions

  • This invention relates to an apparatus for measuring the
  • the fraction of gas in a two component flow of liquid and gas may be defined as the volume of gas in an arbitrary section of a tube divided by the volume of that section of the tube.
  • the fraction of gas may therefore be expressed as a number
  • the instrument may be constructed in such a way as to give a non-intrusive method of measurement.
  • gas fraction meters based on the capacitance principle are relatively scarce.
  • the object of the present invention is to remove these disadvantages and to provide a gas fraction meter of the above mentioned kind in which a homogeneous electric field is maintained within the sample-volume of the sensor.
  • Fig. 1 shows a gas fraction meter comprising two main components, namely a primary sensor, shown schematically, and a signal processing unit illustrated as a circuit diagram.
  • Fig. 2 illustrates the distribution of the electrical field inside the primary sensor.
  • the primary sensor comprises three elec ⁇ trodes, namely two plate electrodes A and B in parallel together with a third electrode C, which, shaped like a tube, encloses the other two electrodes A, B.
  • the two component flow for example in the form of an oil/gas mixture, which is going to be monitored, passes through between the parallel plate electrodes A, B and thereby causes alterations in the measured capacitance between A and B.
  • This capacitance is measured by means of a sine wave generator and an amplifier A., with capacitance feedback; better known today by the term "charge amplifier”. Because the input of this amplifier is kept clamped on "virtual earth", any alteration in the leakage capacitance to earth will have a very little influence on the result. This makes it possible to employ long screened cables between sensor and amplifier (if this is necessary) , without reducing the accuracy of the measurement in any substantial degree. If the feedback capacitance of the charge amplifier A. is fixed and the amplitude V. of the sinewave generator is kept constant, the amplitude V ⁇ of the output signal from the amplifier will be directly proportional to the alterations in the capacitance of the primary sensor. The output voltage of the charge amplifier is in other words a measure of the fraction of gas in the mixture being monitored.
  • the electrode C In order to maintain a homogeneous electric field within the sample volume of the primary sensor, the electrode C must be kept at potential equivalent to the potential occuring half way between the electrodes A and B. This can be accomplished by using a simple voltage divider and a buffer amplifier A...
  • Fig. 2 illustrated the distribution of the electric field inside the primary sensor, where the electrode A is kept at a potential V. , the electrode B at a potential equal to 0 and the electrode C accordingly at a potential equal to shown by the field curves in Fig. 2, the electrical homogeneous inside the sample region of the primary sensor.

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  • Chemical & Material Sciences (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Immunology (AREA)
  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Pathology (AREA)
  • Electrochemistry (AREA)
  • General Chemical & Material Sciences (AREA)
  • Oil, Petroleum & Natural Gas (AREA)
  • Food Science & Technology (AREA)
  • Medicinal Chemistry (AREA)
  • Investigating Or Analyzing Materials By The Use Of Electric Means (AREA)
  • Sampling And Sample Adjustment (AREA)
  • Measuring Volume Flow (AREA)

Abstract

An apparatus for the measurement of the fraction of gas in a two component flow comprising a liquid and a gas in mixture, in particular a flowing oil/gas-mixture. Said apparatus is based on the measurement of alterations of the electric capacitance across two electrodes (A, B) separated in space and working at mutually different potentials, between which the two component mixture is forced to flow, which electrodes (A, B) form an integral part in a primary sensor, where the apparatus moreover includes a signal processing unit, the apparatus being characterized by comprising in addition to the said electrodes (A, B), a third electrode (C), which is designed to enclose the other electrodes (A, B), and which is arranged to be kept at a potential (V/2 x 1), which potential is at least approximately equal to the potential occuring half way between the other two electrodes (A, B), which third electrode (C) by example is fed by a simple voltage divider and a buffer amplifier (A2?), whereby the signal processing unit preferably comprises a sinewave generator and a charge amplifier (amplifier with capacitance feedback) (A?1).

Description

AN APPARATUS FOR THE MEASUREMENT OF THE FRACTION OF GAS IN A TWO-COMPONENT FLUID FLOW COMPRISING A LIQUID AND A GAS IN
10 MIXTURE
TECHNICAL FIELD
This invention relates to an apparatus for measuring the
15 fraction of gas in a two component fluid flow comprising a liquid and a gas in mixture, in particular a flowing oil/gas mixture.
BACKGROUND ART
,20
The fraction of gas in a two component flow of liquid and gas may be defined as the volume of gas in an arbitrary section of a tube divided by the volume of that section of the tube. The fraction of gas may therefore be expressed as a number
25 varying from zero (when the flow is entirely comprised by the liquid) to one (when the flow solely consists of gas) .
While it has been of great importance to know how much of the production from an oil well is comprised by oil and how much
30 of it is gas, measurement of the fraction of gas has always been considered with great interest within the offshore oil business.
Measuring devices whose operating principle is based on the
35 detection of changes in capacitance, have been increasingly employmed for the measurement of the fraction of gas in two component fluid comprising liquid/gas mixtures. The priciple for such a measuring method is well known and amounts essentialy to measuring the electrical capacitance across two electrodes, between which the mixture of the two components is flowing. If the area and the mutual separation of the electrodes are fixed, the measured capacitance will be related to the fraction of gas in the mixture between the electrodes.
By employing such a technique, it is in principle possible to build instruments with rapid dynamic respons. The instrument may be constructed in such a way as to give a non-intrusive method of measurement. In spite of the advantages which is aqhievable in this manner, commercially available gas fraction meters based on the capacitance principle are relatively scarce.
The main disadvantage of known capacitance gas fraction meters is the dependence of the instrument calibration upon the nature of the flow regime being monitored. Thus, by example, the calibration curve required for a bubble flow will deviate from that of an stratified flow.
One of the reasons for this flow regime dependency is the missing homogenity of the electric field through the sample volume. If the electric field varies through the whole sample volume, the measured change in capacity which arises from a change in the gas fraction, will depend upon where the gas is located.
DISCLOSURE OF INVENTION
The object of the present invention is to remove these disadvantages and to provide a gas fraction meter of the above mentioned kind in which a homogeneous electric field is maintained within the sample-volume of the sensor. In addition it is also an object of the present invention to provide a non-intrusive measuring device of sturdy and simple
"BUREA1 construction, by which an output voltage proportional to the fraction of gas is generated by means of a simple signal processing circuit.
These objects are accomplished by designing the apparatus in accordance with the claim. Besides being capable of fulfilling the above mentioned requirements, experiments have shown the gas fraction measuring device not to be as dependant of the flow regime as known gas fraction measuring devices comprising only two electrodes.
BRIEF DESCRIPTION OF DRAWINGS
The measuring device according to the invention will be explained in more detail in the following with reference to the drawing, where:
Fig. 1 shows a gas fraction meter comprising two main components, namely a primary sensor, shown schematically, and a signal processing unit illustrated as a circuit diagram.
Fig. 2 illustrates the distribution of the electrical field inside the primary sensor.
BEST MODE FOR CARRYING OUT THE INVENTION
As shown in Fig. 1, the primary sensor comprises three elec¬ trodes, namely two plate electrodes A and B in parallel together with a third electrode C, which, shaped like a tube, encloses the other two electrodes A, B. The two component flow, for example in the form of an oil/gas mixture, which is going to be monitored, passes through between the parallel plate electrodes A, B and thereby causes alterations in the measured capacitance between A and B.
This capacitance is measured by means of a sine wave generator and an amplifier A., with capacitance feedback; better known today by the term "charge amplifier". Because the input of this amplifier is kept clamped on "virtual earth", any alteration in the leakage capacitance to earth will have a very little influence on the result. This makes it possible to employ long screened cables between sensor and amplifier (if this is necessary) , without reducing the accuracy of the measurement in any substantial degree. If the feedback capacitance of the charge amplifier A. is fixed and the amplitude V. of the sinewave generator is kept constant, the amplitude V^ of the output signal from the amplifier will be directly proportional to the alterations in the capacitance of the primary sensor. The output voltage of the charge amplifier is in other words a measure of the fraction of gas in the mixture being monitored.
In order to maintain a homogeneous electric field within the sample volume of the primary sensor, the electrode C must be kept at potential equivalent to the potential occuring half way between the electrodes A and B. This can be accomplished by using a simple voltage divider and a buffer amplifier A...
Fig. 2 illustrated the distribution of the electric field inside the primary sensor, where the electrode A is kept at a potential V. , the electrode B at a potential equal to 0 and the electrode C accordingly at a potential equal to shown by the field curves in Fig. 2, the electrical
Figure imgf000006_0001
homogeneous inside the sample region of the primary sensor.
"BURE
OMPI

Claims

i CLAIM ,5
An apparatus for the measurement of the fraction of gas in a two component fluid flow comprising a liquid and a gas in mixture, in particular a flowing oil/gas -mixture, said apparatus being based on the measurement of alterations of 0 the electric capacitance across two electrodes (A, B) working at mutually different potentials, between which the two component mixture is forced to flow, which electrodes (A, B) form an integral part in a primary sensor, where the apparatus moreover includes a signal processing unit, 5 c h a r a c t e r i z e d b y comprising in addition to the said electrodes (A, B) , a third electrode (C) , which is arranged to be kept at a potential Cg"' ) , which potential is at least approximately equal to the potential occuring half way between the other two electrodes (A, B) , which third 0 electrode (C) by example is fed by a simple voltage divider and a buffer amplifier (A_) , whereby the signal processing unit preferably comprises a sinewave generator and a charge amplifier (amplifier with capacitance feedback) (A..) .
PCT/NO1984/000046 1983-11-02 1984-10-29 An apparatus for the measurement of the fraction of gas in a two-component fluid flow comprising a liquid and a gas in mixture Ceased WO1985002016A1 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
DE8484903894T DE3476122D1 (en) 1983-11-02 1984-10-29 An apparatus for the measurement of the fraction of gas in a two-component fluid flow comprising a liquid and a gas in mixture
FI852602A FI852602A0 (en) 1983-11-02 1984-10-29 ANORDNING FOER MAETNING AV GASFRAKTIONEN I EN TVAOKOMPONENTS FLUIDUMSTROEM OMFATTANDE EN VAETSKA OCH EN GAS I BLANDNING.
DK292085A DK153587C (en) 1983-11-02 1985-06-27 GAS FRACTION MEASUREMENT IN A TWO COMPONENT FLOW AND GAS FLOW

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
NO833983 1983-11-02
NO833983A NO153621C (en) 1983-11-02 1983-11-02 APPLIANCES FOR MEASURING GAS FRACTION IN A TWO COMPONENT CURRENT USING THE MIXTURE OF WATER AND GAS.

Publications (1)

Publication Number Publication Date
WO1985002016A1 true WO1985002016A1 (en) 1985-05-09

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Country Link
US (1) US4713603A (en)
EP (1) EP0160673B1 (en)
JP (1) JPS61500985A (en)
BR (1) BR8405616A (en)
CA (1) CA1236992A (en)
DE (1) DE3476122D1 (en)
DK (1) DK153587C (en)
FI (1) FI852602A0 (en)
IT (1) IT1207489B (en)
NO (1) NO153621C (en)
SU (1) SU1574185A3 (en)
WO (1) WO1985002016A1 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3225554A1 (en) * 1982-07-08 1984-01-12 Robert Bosch Gmbh, 7000 Stuttgart Measuring device for fluid jets
US5017879A (en) * 1987-09-17 1991-05-21 Schlumberger Technology Corporation Capacitive void fraction measurement apparatus
DE4442711A1 (en) * 1994-12-01 1996-06-05 Claas Ohg Capacitive measuring device
SE2250468A1 (en) * 2022-04-19 2023-10-20 Qtf Sweden Ab Device and method for measuring total gas content in a liquid

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US4774680B1 (en) * 1986-09-19 1993-10-12 Agar Corporation Ltd. Method and apparatus for net oil measurement
US4899101A (en) * 1988-01-21 1990-02-06 The United States Of America As Represented By The United States Department Of Energy Online capacitive densitometer
GB8820687D0 (en) * 1988-09-01 1988-10-05 Chr Michelsen Inst Three component ratio measuring instrument
GB2227841B (en) * 1988-12-03 1993-05-12 Schlumberger Ltd Impedance cross correlation logging tool
GB2267571B (en) * 1992-05-27 1995-09-06 Univ Southampton Gas detector
US5631568A (en) * 1995-08-31 1997-05-20 Caterpillar Inc. Capacitive oil life sensor
US5670721A (en) * 1995-08-31 1997-09-23 Caterpillar Inc. Capacitive pressure sensor with heated electrodes
US5672831A (en) * 1995-08-31 1997-09-30 Caterpillar Inc. Capacitive flow sensor
US5646539A (en) * 1995-08-31 1997-07-08 Caterpillar Inc. Multi-purpose capacitive sensor
US5668309A (en) * 1995-08-31 1997-09-16 Caterpillar Inc. Capacitive particle sensor
US5861755A (en) * 1995-11-06 1999-01-19 The United States Of America As Represented By The Adminstrator Of National Aeronautics And Space Administration Two-phase quality/flow meter
DE19632529A1 (en) * 1996-08-13 1998-02-19 Peter Dipl Ing Tillack Measurement of gas component in multi-phase fluid
JP3767075B2 (en) * 1997-03-24 2006-04-19 ソニー株式会社 Film position detection apparatus, film position detection method, and video film projection apparatus
DE19806477C1 (en) * 1998-02-17 1999-08-26 Deutsch Zentr Luft & Raumfahrt Method and measuring device for determining the volumetric gas content
DE19956958A1 (en) * 1999-11-16 2001-06-13 Vogel Willi Ag Method and device for monitoring the oil flow of a device for oil + air lubrication of components
ITMI20071019A1 (en) 2007-05-21 2008-11-22 Siviero Enrico METHOD AND EQUIPMENT FOR THE MEASUREMENT AND CONTROL OF THE QUANTITY OF NUCLEATION GAS EXPOSED IN A MULTIFASE FLUID
CN101413911B (en) * 2008-11-27 2012-05-09 上海交通大学 Method and device for measuring two-phase flow parameters based on double-head capacitance probe
CN106247917B (en) * 2016-07-12 2018-10-02 清华大学 Horizontal flow pattern of gas-liquid two-phase flow quantitatively judges method and device
US10697846B2 (en) * 2018-05-04 2020-06-30 Ademco Inc. Capacitive leak and flammable vapor detection system

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SE411593B (en) * 1973-07-09 1980-01-14 Akad Gorniczo Hutnicza ELECTRICAL SYSTEM FOR SEATING THE CONTENT OF A MIXTURE TRANSPORTED IN A PIPELINE
DE3227631A1 (en) * 1981-07-27 1983-02-17 Hitachi, Ltd., Tokyo METHOD AND DEVICE FOR MEASURING GAS COMPONENTS IN OIL IN A DEVICE FILLED WITH OIL

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DE2160526A1 (en) * 1971-01-28 1972-08-17 Usines Balteau Sa Device for measuring the gas content of oil
SE411593B (en) * 1973-07-09 1980-01-14 Akad Gorniczo Hutnicza ELECTRICAL SYSTEM FOR SEATING THE CONTENT OF A MIXTURE TRANSPORTED IN A PIPELINE
DE3227631A1 (en) * 1981-07-27 1983-02-17 Hitachi, Ltd., Tokyo METHOD AND DEVICE FOR MEASURING GAS COMPONENTS IN OIL IN A DEVICE FILLED WITH OIL

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Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3225554A1 (en) * 1982-07-08 1984-01-12 Robert Bosch Gmbh, 7000 Stuttgart Measuring device for fluid jets
US5017879A (en) * 1987-09-17 1991-05-21 Schlumberger Technology Corporation Capacitive void fraction measurement apparatus
DE4442711A1 (en) * 1994-12-01 1996-06-05 Claas Ohg Capacitive measuring device
US5708369A (en) * 1994-12-01 1998-01-13 Claas Kommanditgesellschaft Auf Aktien Capacitive measuring device
SE2250468A1 (en) * 2022-04-19 2023-10-20 Qtf Sweden Ab Device and method for measuring total gas content in a liquid
SE545735C2 (en) * 2022-04-19 2023-12-27 Qtf Sweden Ab Device and method for measuring total gas content in a liquid

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BR8405616A (en) 1985-09-10
FI852602L (en) 1985-07-01
EP0160673A1 (en) 1985-11-13
DK153587B (en) 1988-07-25
DK153587C (en) 1988-12-19
NO833983L (en) 1985-05-03
DE3476122D1 (en) 1989-02-16
SU1574185A3 (en) 1990-06-23
DK292085A (en) 1985-06-27
IT1207489B (en) 1989-05-25
IT8423442A0 (en) 1984-11-02
EP0160673B1 (en) 1989-01-11
US4713603A (en) 1987-12-15
JPS61500985A (en) 1986-05-15
DK292085D0 (en) 1985-06-27
CA1236992A (en) 1988-05-24
NO153621B (en) 1986-01-13
NO153621C (en) 1986-04-23
FI852602A7 (en) 1985-07-01
FI852602A0 (en) 1985-07-01

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