CN1389743A - Acoustic resonance method of measuring sand flow cavity volume - Google Patents

Acoustic resonance method of measuring sand flow cavity volume Download PDF

Info

Publication number
CN1389743A
CN1389743A CN 02123730 CN02123730A CN1389743A CN 1389743 A CN1389743 A CN 1389743A CN 02123730 CN02123730 CN 02123730 CN 02123730 A CN02123730 A CN 02123730A CN 1389743 A CN1389743 A CN 1389743A
Authority
CN
China
Prior art keywords
hole
source
sound
cavity volume
sound source
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
CN 02123730
Other languages
Chinese (zh)
Other versions
CN1172196C (en
Inventor
乔文孝
李刚
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.)
China National Petroleum Corp
China University of Petroleum East China
Original Assignee
China National Petroleum Corp
China University of Petroleum East China
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
Application filed by China National Petroleum Corp, China University of Petroleum East China filed Critical China National Petroleum Corp
Priority to CNB021237301A priority Critical patent/CN1172196C/en
Publication of CN1389743A publication Critical patent/CN1389743A/en
Application granted granted Critical
Publication of CN1172196C publication Critical patent/CN1172196C/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

A hollow volume formed by sand inflow from oil well and its measurement method features in that the measurement system comprises sound source and sound wave received, transducer to fully use the resonance phenomenon of liquid at the mouth of the hollow between sound source and the received transducer to determine the hollow volume using the extremely small value of the received signal frequency spectrum. Sound source may be a pulse source similar to electric sparks signal source or moving coil, piezoelectric, magnetostriction and mechanical transducer excited by electric signals. The resonance frequency at the hollow mouth is determined by frequency spectrum analysis either with hardware or software.

Description

A kind of method of measuring sand flow cavity volume with acoustic resonance
The present invention relates to a kind ofly measure the method for sand flow cavity volume with acoustic resonance, it is the method that belong to applied geophysics, petroleum engineering field a kind of measures the empty volume that sand production causes.It mainly is the method that adopted sound wave measuring system to combine with specific hole mathematical model determine the to shake out volume in hole.
At present, in oil formation testing and petroleum production engineering, because aspects such as geologic condition and exploitation construction sand production can occur and form the stratum cavitation.Shake out and may stop up on the one hand oil pipe and also may destroy geologic structure on the other hand and cause the oil well underproduction even stopping production.So the sand control construction is a crucial job.Owing to the volume that does not also have means to the hole that shakes out now both at home and abroad carries out quantitative measurment.Therefore, make the sand control construction have certain blindness, success ratio to have a greatly reduced quality.The object of the present invention is to provide a kind of method of the empty volume that can cause at the measurement sand production of down-hole use, it is to have adopted in pit shaft to be measured sound wave measuring system is set, and the hole that will shake out is specific for certain mathematical model, utilizes the minimal value of received signal frequency spectrum to determine the volume in cavity then.Thereby can improve measuring accuracy widely and improve the efficient of sand control construction.This method mainly is to have adopted the method that combines of sound wave measuring system and specific hole mathematical model, its major technology characteristics are that the measuring system that is adopted is to be made of sound source and sound wave receiving transducer, and be arranged among the pit shaft to be measured, the cavity that shakes out in the pit shaft to be measured is set at specific hole mathematical model, by the resonance effect of mouthful place's liquid of existing cavity between measurement sound source and the receiver, and utilize the minimal value of received signal frequency spectrum to determine empty volume; The mathematical modulo in its hole that shakes out is a heimholtz resonator, and the resonance frequency of its hole mouth is: f r = c 2 π S Vl , In the formula, S is the sectional area at hole, and l is the length at hole, and V is a cavity volume, and c is the velocity of sound of empty inner fluid; Employed sound source can be an impulse source that is similar to the spark signal source, also can be the signal source that can send the frequency sweep sound wave continuously.
Below in conjunction with embodiment in detail technical characterstic of the present invention is described in detail.
In actual design and construction, the deviser is the method for the present invention that realizes like this: measuring system is made of a sound source and an acoustic receiver and corresponding measurement mechanism, and is shown in the pit shaft by accompanying drawing 1 and is provided with.During measurement, measuring system is carried on transferring to the bottom of measuring well section, and measures last carrying in the process.Sound source is propagated to receiving transducer one side in in-hole fluid after sending acoustic signals.If a perf (borehole) is arranged send out receiving between the probe, and the sleeve pipe external cause shakes out and has a cavity of a certain volume, and the fluid of then should cavity mouth (borehole) locating will vibrate.When the resonance frequency of the frequency of sound wave and hole fluid was identical, resonance took place and the strong absorption acoustic wave energy in the fluid at mouthful place, cavity, and then the signal of this frequency content that receives of receiving transducer is a minimal value for other frequency content signal.The acoustic model of the fluid oscillation at place, cavity is set at heimholtz resonator as shown in Figure 2.This model is an open containers of being made up of cavity and short tube, and hypothesis satisfies: the dimension of (1) cavity (hole) volume V is much smaller than wave length of sound.(2) volume of short tube is much smaller than the hole volume.(3) medium compression and when expanding in the hole, the hole wall can not be out of shape.So the fluid in the short tube at hole mouth place is done body vibration just as one " piston ", its resonance frequency is f r = c 2 π S Vl In the formula, S is the sectional area of short tube (borehole), and l is the length (can be taken as the thickness of sleeve pipe) of short tube, and V is a cavity volume, and c is the velocity of sound of empty inner fluid.As seen, as long as accurately measure the minimal value of the frequency spectrum of received signal, just can determine the resonant frequency of the fluid oscillation at mouthful place, cavity, and then can calculate the cavity volume that shakes out according to formula (1).If the thickness of getting sleeve pipe is the diameter of 10mm, borehole is that the velocity of sound of liquid in 10mm, the cavity is 1550m/s, when the variation range of empty volume is 0.01m 3~5m 3The time, the scope that requires frequency of sound wave is 10Hz~300Hz.
Measuring system is carried on the bottom of well section to be measured begins, and measures in last each depth point of carrying in the process, and this method has two kinds of metering systems.(1) frequency sweep working method
Press measuring principle shown in the accompanying drawing 1, repeatedly encourage sonic probe to make it to launch the frequency sweep acoustic signals with the frequency sweep electric signal, the scope of frequency of sound wave is 10Hz~300Hz, and the frequency spectrum of the signal that receiving transducer is received is analyzed, minimal value by the received signal frequency spectrum is determined resonance frequency, again by f r = c 2 π S Vl The calculating cavity volume that shakes out.This moment, sound source was moving-coil type or piezoelectric type or a magnetostriction type or a mechanical type transducer that is encouraged by electric signal.(2) pulsed mode
By measuring principle shown in Figure 1, employing is similar to the broadband laser pulse focus of sparker source as sound source, and the pulsed sound that it produces is propagated in well, and the time-domain signal that receiving transducer is received carries out spectrum analysis, minimal value by the received signal frequency spectrum is determined resonance frequency, again by f r = c 2 π S Vl The calculating cavity volume that shakes out.
The acoustic measurement method of the measurement sand flow cavity volume that the present invention proposes, the shape in measurement result and hole is irrelevant.Therefore, do not require the systematicness of void shape.Its measuring method reliability height, be easy to realize, cost is low, has great promotion and application prospect.

Claims (3)

1. method of measuring sand flow cavity volume with acoustic resonance, it mainly is the method that combines that has adopted sound wave measuring system and specific hole mathematical model, it is characterized in that the measuring system that is adopted is to be made of sound source and sound wave receiving transducer, and be arranged among the pit shaft to be measured, the cavity that shakes out in the pit shaft to be measured is set at specific hole mathematical model, by the resonance effect of mouthful place's liquid of existing cavity between measurement sound source and the receiver, and utilize the minimal value of received signal frequency spectrum to determine empty volume.
2. a kind of method according to claim 1 with acoustic resonance measurement sand flow cavity volume, the mathematical modulo that it is characterized in that the described hole that shakes out is a heimholtz resonator, the resonance frequency of its hole mouth is: f r = c 2 π S Vl Wherein, S is the sectional area at hole, and l is the length at hole, and V is a cavity volume, and c is the velocity of sound of empty inner fluid.
3. a kind of method of measuring sand flow cavity volume with acoustic resonance according to claim 1, it is characterized in that described sound source can be an impulse source that is similar to the spark signal source, also can be the signal source that can send the frequency sweep sound wave continuously.
CNB021237301A 2002-06-21 2002-06-21 Acoustic resonance method of measuring sand flow cavity volume Expired - Fee Related CN1172196C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB021237301A CN1172196C (en) 2002-06-21 2002-06-21 Acoustic resonance method of measuring sand flow cavity volume

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB021237301A CN1172196C (en) 2002-06-21 2002-06-21 Acoustic resonance method of measuring sand flow cavity volume

Publications (2)

Publication Number Publication Date
CN1389743A true CN1389743A (en) 2003-01-08
CN1172196C CN1172196C (en) 2004-10-20

Family

ID=4745197

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB021237301A Expired - Fee Related CN1172196C (en) 2002-06-21 2002-06-21 Acoustic resonance method of measuring sand flow cavity volume

Country Status (1)

Country Link
CN (1) CN1172196C (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106054240A (en) * 2016-06-12 2016-10-26 刘照朗 Novel high-level earthquake monitoring and prediction method
CN107859515A (en) * 2017-09-13 2018-03-30 杭州瑞利声电技术公司 A kind of acoustic logging transmitter unit
RU2669268C1 (en) * 2018-02-09 2018-10-09 Анна Борисовна Шмелева Method of seismic signal filtration in seismic liquid measuring system
CN108806197A (en) * 2018-06-28 2018-11-13 广东安元矿业勘察设计有限公司 A kind of new method of big rank earthquake monitoring and forecasting
TWI683104B (en) * 2018-12-28 2020-01-21 財團法人工業技術研究院 Detecting system and detection method
US11525811B2 (en) 2018-12-28 2022-12-13 Industrial Technology Research Institute Detection system and detection method

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106054240A (en) * 2016-06-12 2016-10-26 刘照朗 Novel high-level earthquake monitoring and prediction method
CN107859515A (en) * 2017-09-13 2018-03-30 杭州瑞利声电技术公司 A kind of acoustic logging transmitter unit
RU2669268C1 (en) * 2018-02-09 2018-10-09 Анна Борисовна Шмелева Method of seismic signal filtration in seismic liquid measuring system
CN108806197A (en) * 2018-06-28 2018-11-13 广东安元矿业勘察设计有限公司 A kind of new method of big rank earthquake monitoring and forecasting
TWI683104B (en) * 2018-12-28 2020-01-21 財團法人工業技術研究院 Detecting system and detection method
US11525811B2 (en) 2018-12-28 2022-12-13 Industrial Technology Research Institute Detection system and detection method

Also Published As

Publication number Publication date
CN1172196C (en) 2004-10-20

Similar Documents

Publication Publication Date Title
US4628725A (en) Apparatus and method for analyzing a fluid that includes a liquid phase, contained in a tubular conduit
CN107849916B (en) Method and apparatus for measuring fluid properties using an electromechanical resonator
US4571693A (en) Acoustic device for measuring fluid properties
US8576660B2 (en) Ultrasonic imaging in wells or tubulars
CN103323195B (en) A kind of whirling vibration excitation and dynamic measurement device
CN102146791A (en) Method and device for measuring working fluid level of oil well
US11067711B2 (en) Time-reversed nonlinear acoustic downhole pore pressure measurements
JP5096571B2 (en) Measurement of sound velocity of downhole fluid using tube wave
AU2012216617B2 (en) Apparatus and method for measuring the acoustic impedance of wellbore fluids
CN101050702B (en) Measuring device and method for overcurrent type resonant sound spectrum multiple phase flow state test
RU2006143592A (en) Cementometry based on radially bending modes of resonant casing oscillations
GB2585499A (en) Downhole fluid density and viscosity sensor based on ultrasonic plate waves
JP2010531429A (en) Measurement of sound velocity of downhole fluid with Helmholtz resonator
CN101393172A (en) Non-damage detection for cracks in solid by non-linear resonating sound spectrum method
US6941819B1 (en) Apparatus and method for determining the dynamic mechanical properties of a cement sample
CN1172196C (en) Acoustic resonance method of measuring sand flow cavity volume
CN100380101C (en) Doppler type ultrasonic flowmeter
US10677757B2 (en) Method for acoustically determining properties of a medium, and device for acoustically determining properties of a medium, comprising a reflective element
CN112593926A (en) Method and system for measuring cementing quality of cased well by using SH wave
CN202108505U (en) Acoustic velocity measurement device of drilling mud
RU2661455C1 (en) Method for determining the viscoelastic properties of liquid and solid media and the device for its implementation
CN113982562A (en) Well cementation quality evaluation method based on array acoustic logging
JPS63247608A (en) Method for measuring thickness and internal cracking position of concrete
CN206114597U (en) A giant magnetostrictive adherence transmission oscillator that is used for two receipts of PS well logging to pop one's head in
RU2115892C1 (en) Method determining level of fluid in well and gear for its implementation

Legal Events

Date Code Title Description
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20041020

Termination date: 20210621