WO2015175905A1 - Acoustic standoff and mud velocity using a stepped transmitter - Google Patents

Acoustic standoff and mud velocity using a stepped transmitter Download PDF

Info

Publication number
WO2015175905A1
WO2015175905A1 PCT/US2015/031022 US2015031022W WO2015175905A1 WO 2015175905 A1 WO2015175905 A1 WO 2015175905A1 US 2015031022 W US2015031022 W US 2015031022W WO 2015175905 A1 WO2015175905 A1 WO 2015175905A1
Authority
WO
WIPO (PCT)
Prior art keywords
acoustic
fluid
reflected
signal
wellbore
Prior art date
Application number
PCT/US2015/031022
Other languages
French (fr)
Inventor
Rocco Difoggio
Wei Han
Original Assignee
Baker Hughes Incorporated
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 US14/278,839 external-priority patent/US9366133B2/en
Application filed by Baker Hughes Incorporated filed Critical Baker Hughes Incorporated
Publication of WO2015175905A1 publication Critical patent/WO2015175905A1/en

Links

Classifications

    • EFIXED CONSTRUCTIONS
    • E21EARTH OR ROCK DRILLING; MINING
    • E21BEARTH OR ROCK DRILLING; OBTAINING OIL, GAS, WATER, SOLUBLE OR MELTABLE MATERIALS OR A SLURRY OF MINERALS FROM WELLS
    • E21B47/00Survey of boreholes or wells
    • E21B47/10Locating fluid leaks, intrusions or movements
    • E21B47/107Locating fluid leaks, intrusions or movements using acoustic means

Definitions

  • the present disclosure is related to testing of fluids in a wellbore and, in particular, to methods and apparatus for determining acoustic properties of fluids in the wellbore.
  • Exploration for hydrocarbons commonly includes using a bottomhole assembly including a drill-bit for drilling a borehole in an earth formation.
  • Drilling fluid or "mud” used in the drilling may vary in density or "mud weight” for a number of reasons. Such variations can result from changes in the quantity and density of cuttings (particles of formation); changes in the "mud program" at the surface, changes in temperature, etc.
  • Variations in mud density also occur when gas or liquid enter the borehole from the formation. Such influx of formation fluids may likely be the result of formation overpressures or abnormally high pressures.
  • Pressure detection is useful in drilling operations. Not only does the drilling rate decrease with a high overbalance of mud pressure versus formation pressure, but also lost circulation and differential pressure sticking of the drill pipe can readily occur. More importantly, an underbalance of mud pressure versus formation pressure can cause a pressure "kick.” A well may kick without forewarning. Balanced drilling techniques often require only a fine margin between effective pressure control and a threatened blowout.
  • the present disclosure provides a method of determining an acoustic property of a fluid in a wellbore, the method including: placing a faceplate in the wellbore with a stepped surface of the faceplate in contact with the fluid, wherein the stepped surface includes a non-stepped face and a stepped face; transmitting an acoustic pulse through the faceplate into the fluid, wherein a first portion of the acoustic pulse passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; receiving a first reflected acoustic pulse related to the first portion of the acoustic pulse from a wellbore surface and a second refiected acoustic pulse related to the second portion of the acoustic pulse from the wellbore surface; obtaining a measurement of the first reflected acoustic pulse and a measurement of the second refiected pulse; and determining from
  • the present disclosure provides an apparatus for determining an acoustic property of a fluid in a wellbore, the apparatus including: a faceplate having a stepped surface that includes a non-stepped face and a stepped face, wherein the stepped surface is coupled to the fluid in the wellbore; an acoustic transducer configured to transmit an acoustic signal to pass through the stepped surface of the faceplate into the fluid, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; and a processor configured to: receive measurements of a first reflected pulse related to reflection of the first portion of the transmitted acoustic signal from a wellbore surface a second reflected pulse related to reflection of the second portion of the transmitted acoustic signal from the wellbore surface, and determine the acoustic property of the fluid in the wellbor
  • the present disclosure provides a system for determining an acoustic property of a fluid in a wellbore, the system including: a member disposed in the wellbore; a faceplate disposed on the member, the faceplate having a stepped surface coupled to the fluid in the wellbore, wherein the stepped surface includes a non-stepped face and a stepped face; an acoustic transducer configured to transmit an acoustic signal into the faceplate, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid through the non-stepped face and a second portion of the transmitted acoustic signal passes from the faceplate into the fluid through the stepped face, the acoustic transducer further configured to receive a first reflected acoustic signal related reflection of the first portion of the transmitted acoustic signal from a surface of the wellbore and a second reflected acoustic signal related to reflection of the second portion of the transmitted acou
  • FIG. 1 shows an illustrative wellbore system suitable for determining an acoustic property of fluid in a wellbore in one embodiment of the present disclosure
  • FIG. 2 shows a detailed view of the fluid testing apparatus of FIG. 1 in one embodiment
  • FIG. 3 shows various transmission and/or reflection paths for an acoustic pulse generated by an acoustic transducer of the fluid testing apparatus
  • FIGS. 4A and 4B show schematic waveforms of the pulses received at the acoustic transducer.
  • FIG. 1 shows an illustrative wellbore system 100 suitable for determining an acoustic property of fluid 108 in a wellbore 104 in one embodiment of the present disclosure.
  • the wellbore system 100 includes a member 102 that extends from a surface location 120 into a borehole or wellbore 104.
  • the wellbore 104 may be an open wellbore or a cased wellbore, in various embodiments.
  • a surface 104a (also referred to herein as a "wellbore wall 104a") of the wellbore 104 may be a surface of a formation or an interior face of a casing (not shown) disposed in the wellbore 104.
  • An annulus 114 is formed between the member 102 and the wellbore wall 104a.
  • the member 102 may be a drillstring that includes a drill bit 106 at a bottom end for drilling the wellbore 104.
  • the member 102 includes a fluid testing apparatus 110 suitable for determining a property of the fluid 108 in the annulus 114 of the wellbore 104.
  • FIG. 2 shows a detailed view of the fluid testing apparatus 110 of FIG. 1 in one embodiment.
  • the fluid testing apparatus 110 includes an acoustic device 200 disposed on the member 102.
  • the acoustic device 200 includes an acoustic transducer 202 and a faceplate 204, which may be a stepped faceplate, as described below.
  • the faceplate 204 includes a first surface 210 and a second surface 212 that is opposite the first surface 210.
  • the second surface 212 is a stepped surface, including a non-stepped face 214 and a stepped face 216. The distance between the non-stepped face 214 and the first surface 210 is less than the distance between the stepped face 216 and the first surface 210. As shown in FIG.
  • a perpendicular distance between the first surface 210 and the non-stepped face 214 is L 0 and a perpendicular distance between the first surface 210 and the stepped face 216 is L 0 +x. Therefore, a perpendicular distance between the stepped face 216 and the non-stepped face 214 is x.
  • the second surface 212 may include more than two faces.
  • the acoustic transducer 202 is coupled to the first face 210 of the faceplate 204 and transmits acoustic signals into the faceplate 204 and receives acoustic signals from the faceplate 204.
  • a seal 206 between the acoustic device 200 and the member 102 prevents ingress of fluids into the member 102.
  • the non-stepped face 214 is at a distance L from the wellbore wall 104a and stepped face 216 is at a distance L-x from the wellbore wall 104a.
  • the fluid testing apparatus 110 further includes a control unit 220 coupled to the acoustic transducer 202.
  • the control unit 220 includes a processor 222 and a memory storage device 224.
  • the memory storage device 224 may be any non-transitory computer- readable storage medium, such as a solid-state memory, ROM, RAM, etc.
  • the memory storage device 224 includes a set of programs 226 stored therein.
  • the programs 226 may include instructions that when read by the processor 222 enable the processor to, among other things, determine an acoustic property of the fluid 108 in the wellbore 104 based on measurements obtained from the acoustic device 200.
  • the control unit 220 may further control an operation of the acoustic device 200 or, specifically, the acoustic transducer 202.
  • the control unit 220 may be disposed downhole with the acoustic device 200 or may be situated at the surface location 120.
  • FIG. 3 shows various transmission and/or reflection paths for an acoustic pulse generated by the acoustic transducer 202 of the exemplary acoustic device 200 of the present disclosure.
  • the acoustic transducer 202 transmits an original acoustic pulse or signal that enters through the faceplate 204 at first surface 210 and travels through the faceplate 204 to the second surface 212.
  • the original acoustic pulse may includes a first portion 302 that intercepts the non-stepped face 214 and a second portion 304 that intercepts the stepped face 216. Reflection and transmission of the incident pulses occurs at each of the non-stepped face 214 and the stepped face 216.
  • an internally reflected signal (A b ) may be reflected back through the faceplate 204 to the acoustic transducer 202.
  • Another part of the first portion 302 is transmitted into the fluid 108 as indicated by signal A bb -
  • Signal A bb propagates through the fluid 108 to the wellbore wall 104a and is reflected from the wellbore wall 104a back through the fluid 108 to the non- stepped face 214.
  • Signal A bb then passes through the non-stepped face 214 and propagates back to the acoustic transducer 202.
  • the path length in the faceplate 204 is distance LQ and the path length in the fluid 108 is distance L.
  • an internally reflected signal A a may be reflected back through the faceplate 204 to the acoustic transducer 202.
  • Another part of the first portion 302 is transmitted into the fluid 108 as indicated by signal A aa .
  • Signal A aa propagates through the fluid 108 to the wellbore wall 104a and is reflected from the wellbore wall 104a back through the fluid 108 to the stepped face 216.
  • Signal A aa then passes through the stepped face 216 and propagates back to the acoustic transducer 202.
  • the path length in the faceplate 204 is distance Lo+x and the path length in the fluid 108 is distance L-x.
  • Signals propagating through the faceplate 204 travel at an acoustic velocity ex.
  • Signals propagating through the fluid 108 travel at an acoustic velocity ⁇ 3 ⁇ 4 also known as "mud velocity.”
  • the acoustic velocity ⁇ 3 ⁇ 4 may be an unknown value that is determined via the methods disclosed herein.
  • the acoustic velocity cx either may be a known quantity or may be determined using the methods disclosed herein.
  • a sudden drop in the mud velocity can indicate gas influx from the formation into the drilling mud.
  • FIGS. 4A and 4B show measured waveforms (V a , Vb, V aa and Vbb) of the respective pulses A a , A b , A aa and A bb (FIG. 3) received at the acoustic transducer 202.
  • FIG. 3 shows measured waveforms (V a , Vb, V aa and Vbb) of the respective pulses A a , A b , A aa and A bb (FIG. 3) received at the acoustic transducer 202.
  • the travel time for a selected pulse is a difference between a time at which the original acoustic pulse is generated at the acoustic transducer 202 and time at which the reflected pulse corresponding to the selected pulse is detected at the acoustic transducer 202.
  • Pulse A a (traveling entirely within the faceplate 204) has a travel time T a
  • pulse Ab (traveling entirely within the faceplate 204) has a travel time Tb
  • pulse A aa (traveling within both the faceplate 204 and the fluid 108) has a travel time T aa
  • pulse Abb (traveling within both the faceplate 204 and the fluid 108) has a travel time 73 ⁇ 4. Since, pulses A a and Ab are internally reflected, their travel times T a and Tb are earlier that the travel times T aa and 73 ⁇ 4 of pulses A aa and Abb, which travel through the fluid 108 and are reflected from the wellbore wall 104a.
  • FIG. 4B shows the measurements obtained when a velocity of sound in the faceplate 204 ( ⁇ 3 ⁇ 4) is less than a velocity of sound ( ⁇ 3 ⁇ 4) in the fluid 108.
  • the travel times do not change.
  • pulse Abb arrives before pulse
  • the equations for round-trip travel time for a selected reflected pulse may be written in equation form.
  • the round-trip travel time is a function of a length of a path (path length) for the pulse in a particular medium (i.e., the faceplate 204 and/or the fluid 108) as well as the acoustic velocities (i.e., cx and/or c ) of the particular medium.
  • the equation for a round-trip travel time for signal A aa is:
  • T bb 2L 0 /c x + 2L/c L Eq. (2)
  • the speed of sound of the fluid 108 in the wellbore 104 may be determined by solving Eq. (3) to obtain:
  • a standoff L between the faceplate 204 from the wellbore wall 104a (or equivalently, between the member 102 and the wellbore wall 104a) may be determined as
  • the speed of sound (c x ) in the faceplate 204 may be determined from round-trip travel times of the internally reflected acoustic pulses (i.e., signals A a and A b ), as shown in Eqs. (6) - (8).
  • the round-trip travel time for signal A a is:
  • acoustic attenuation coefficients of the faceplate 204 and of the fluid 108 may be determined. Additionally, an acoustic impedance of the fluid 108 may be determined.
  • the amplitudes of the returned pulse waveforms (V a , Vb, V aa , and Vbb) are given by the following equations (9) - (12):
  • V b P 0 e - 2 ⁇ o ££l£ Eq . (9)
  • V a p 0 e -2a x (L 0 +x)£c 3 ⁇ 4 Eq. (10)
  • V bb Poe - 2a * L ° - ⁇ e - 2 ⁇ f Z - Eq. (1 1)
  • V aa P 0 e- 2 ⁇ +X ) ⁇ H ⁇ e -2a f (L- x) ⁇ Eq . ( 1 2 )
  • P 0 is the amplitude of the original acoustic signal generated by the acoustic transducer 202
  • a x and a/ are the sound attenuation coefficient of the material of the face plate and the sound attenuation coefficient of the fluid 108, respectively.
  • Z/, ⁇ and Zc are the acoustic impedances of the fluid, the material of the faceplate 204 and the material of the borehole wall (or of the casing), respectively.
  • the attenuation coefficient of the face plate (a x ) may be determined from Eq. (9) and Eq. (10), to obtain:
  • the attenuation coefficient of the fluid (a j ) may be determined from Eq. (1 1) and Eq. (12) and the determined coefficient a x from Eq. (13) to obtain:
  • the fluid impedance Z may then be solved from Eq. (15).
  • Zc is a known acoustic impedance of the material (e.g., steel casing) of the wellbore wall 104a.
  • Zy is an acoustic impedance of the material of the faceplate 204, which is either known or may be determined from Eq. (13), L is the standoff distance (determined in Eq. (5)) and a/ is the fluid attenuation coefficient, determined in Eq. (14).
  • Zy is an acoustic impedance of the material of the faceplate 204, which is either known or may be determined from Eq. (13)
  • L is the standoff distance (determined in Eq. (5))
  • a/ is the fluid attenuation coefficient, determined in
  • the present disclosure provides a method of determining an acoustic property of a fluid in a wellbore, the method including: placing a faceplate in the wellbore with a stepped surface of the faceplate in contact with the fluid, wherein the stepped surface includes a non-stepped face and a stepped face; transmitting an acoustic pulse through the faceplate into the fluid, wherein a first portion of the acoustic pulse passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; receiving a first reflected acoustic pulse related to the first portion of the acoustic pulse from a wellbore surface and a second reflected acoustic pulse related to the second portion of the acoustic pulse from the wellbore surface; obtaining a measurement of the first reflected acoustic pulse and a measurement of the second reflected pulse; and determining from
  • a path of the first reflected acoustic pulse intersects the non-stepped face of the faceplate and a path of the second reflected acoustic pulse intersects the stepped face of the faceplate.
  • the method determines the acoustic velocity of the fluid using a difference between a travel time of the first reflected signal and a travel time of the second reflected signal. The difference between the travel time of the first reflected signal and the travel time of the second reflected signal is related to a difference between a path length through the fluid of the first reflected signal and a path length through the fluid of the second reflected signal.
  • a standoff distance between the faceplate and the wellbore surface may be determined using the determined acoustic velocity of the fluid.
  • the acoustic property of the fluid is an acoustic attenuation of the fluid
  • the acoustic attenuation of the fluid may be determined from an amplitude of the first reflected signal an amplitude of the second reflected signal.
  • the method may further include determining an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
  • the present disclosure provides an apparatus for determining an acoustic property of a fluid in a wellbore, the apparatus including: a faceplate having a stepped surface that includes a non-stepped face and a stepped face, wherein the stepped surface is coupled to the fluid in the wellbore; an acoustic transducer configured to transmit an acoustic signal to pass through the stepped surface of the faceplate into the fluid, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; and a processor configured to: receive measurements of a first reflected pulse related to reflection of the first portion of the transmitted acoustic signal from a wellbore surface a second reflected pulse related to reflection of the second portion of the transmitted acoustic signal from the wellbore surface, and determine the acoustic property of the fluid in the wellbor
  • a path of the first reflected signal intersects the non-stepped face a path of the second reflected acoustic pulse intersects the stepped face.
  • the processor may determine the acoustic velocity of the fluid from a difference between a travel time of the first reflected signal and a travel time of the second reflected signal.
  • the processor may further determine a standoff distance between a member and the wellbore surface using the determined acoustic velocity for the faceplate disposed on the member.
  • a difference between the travel time of the first reflected signal and the travel time of the second reflected signal is related to a difference in a path length of the first reflected signal through the fluid and a path length of the second reflected signal through the fluid.
  • the processor may determine the attenuation of the acoustic signal in the fluid using an amplitude of the first signal and an amplitude of the second signal.
  • the processor may further determine an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
  • the present disclosure provides a system for determining an acoustic property of a fluid in a wellbore, the system including: a member disposed in the wellbore; a faceplate disposed on the member, the faceplate having a stepped surface coupled to the fluid in the wellbore, wherein the stepped surface includes a non-stepped face and a stepped face; an acoustic transducer configured to transmit an acoustic signal into the faceplate, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid through the non-stepped face and a second portion of the transmitted acoustic signal passes from the faceplate into the fluid through the stepped face, the acoustic transducer further configured to receive a first reflected acoustic signal related reflection of the first portion of the transmitted acoustic signal from a surface of the wellbore and a second reflected acoustic signal related to reflection of the second portion of the transmitted acou
  • a path of the first reflected acoustic pulse intersects the non-stepped face and a path of the second reflected acoustic pulse intersects the stepped face.
  • the processor may determine the acoustic velocity of the fluid from a difference between measured travel times of the first reflected signal and the second reflected signal.
  • the processor may further determine a standoff distance between the member and the wellbore surface.
  • the processor may determine the attenuation of the acoustic signal in the fluid using an amplitude of the first signal and an amplitude of the second signal.
  • the processor may further determine an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.

Landscapes

  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Geology (AREA)
  • Mining & Mineral Resources (AREA)
  • Acoustics & Sound (AREA)
  • Geophysics (AREA)
  • Environmental & Geological Engineering (AREA)
  • Fluid Mechanics (AREA)
  • General Life Sciences & Earth Sciences (AREA)
  • Geochemistry & Mineralogy (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Abstract

A system, apparatus and method for determining an acoustic property of a fluid in a wellbore is disclosed. A faceplate is placed in the wellbore with a stepped surface of the faceplate in contact with the fluid. The stepped surface includes a non-stepped face and a stepped face. A first portion of an acoustic pulse passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face. A first reflected acoustic pulse related to the first portion of the acoustic pulse is received. A second reflected acoustic pulse related to the second portion of the acoustic pulse is received. A measurement of the first reflected acoustic pulse and a measurement of the second reflected pulse are used to determine the acoustic property of the fluid in the wellbore.

Description

ACOUSTIC STANDOFF AND MUD VELOCITY USING A STEPPED
TRANSMITTER
CROSS-REFERENCE TO RELATED APPLICATIONS
[0001] This application claims the benefit of U.S. Application No. 14/278839, filed on May 15, 2014, which is incorporated herein by reference in its entirety.
BACKGROUND OF THE DISCLOSURE
1. Field of the Disclosure
[0002] The present disclosure is related to testing of fluids in a wellbore and, in particular, to methods and apparatus for determining acoustic properties of fluids in the wellbore.
2. Description of the Related Art
[0003] Exploration for hydrocarbons commonly includes using a bottomhole assembly including a drill-bit for drilling a borehole in an earth formation. Drilling fluid or "mud" used in the drilling may vary in density or "mud weight" for a number of reasons. Such variations can result from changes in the quantity and density of cuttings (particles of formation); changes in the "mud program" at the surface, changes in temperature, etc.
Variations in mud density also occur when gas or liquid enter the borehole from the formation. Such influx of formation fluids may likely be the result of formation overpressures or abnormally high pressures.
[0004] Pressure detection is useful in drilling operations. Not only does the drilling rate decrease with a high overbalance of mud pressure versus formation pressure, but also lost circulation and differential pressure sticking of the drill pipe can readily occur. More importantly, an underbalance of mud pressure versus formation pressure can cause a pressure "kick." A well may kick without forewarning. Balanced drilling techniques often require only a fine margin between effective pressure control and a threatened blowout.
Additionally, there are situations where it is desired to maintain underbalance to avoid formation damage. Thus, there is a need to measure the properties of the borehole fluid downhole in order to detect, among other things, kicks and inflow of formation liquids.
SUMMARY OF THE DISCLOSURE
[0005] In one aspect, the present disclosure provides a method of determining an acoustic property of a fluid in a wellbore, the method including: placing a faceplate in the wellbore with a stepped surface of the faceplate in contact with the fluid, wherein the stepped surface includes a non-stepped face and a stepped face; transmitting an acoustic pulse through the faceplate into the fluid, wherein a first portion of the acoustic pulse passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; receiving a first reflected acoustic pulse related to the first portion of the acoustic pulse from a wellbore surface and a second refiected acoustic pulse related to the second portion of the acoustic pulse from the wellbore surface; obtaining a measurement of the first reflected acoustic pulse and a measurement of the second refiected pulse; and determining from the obtained measurements the acoustic property of the fluid in the wellbore.
[0006] In another aspect, the present disclosure provides an apparatus for determining an acoustic property of a fluid in a wellbore, the apparatus including: a faceplate having a stepped surface that includes a non-stepped face and a stepped face, wherein the stepped surface is coupled to the fluid in the wellbore; an acoustic transducer configured to transmit an acoustic signal to pass through the stepped surface of the faceplate into the fluid, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; and a processor configured to: receive measurements of a first reflected pulse related to reflection of the first portion of the transmitted acoustic signal from a wellbore surface a second reflected pulse related to reflection of the second portion of the transmitted acoustic signal from the wellbore surface, and determine the acoustic property of the fluid in the wellbore from the received measurements of the first reflected acoustic pulse and the second refiected acoustic pulse.
[0007] In yet another aspect, the present disclosure provides a system for determining an acoustic property of a fluid in a wellbore, the system including: a member disposed in the wellbore; a faceplate disposed on the member, the faceplate having a stepped surface coupled to the fluid in the wellbore, wherein the stepped surface includes a non-stepped face and a stepped face; an acoustic transducer configured to transmit an acoustic signal into the faceplate, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid through the non-stepped face and a second portion of the transmitted acoustic signal passes from the faceplate into the fluid through the stepped face, the acoustic transducer further configured to receive a first reflected acoustic signal related reflection of the first portion of the transmitted acoustic signal from a surface of the wellbore and a second reflected acoustic signal related to reflection of the second portion of the transmitted acoustic signal from the surface of the wellbore; and a processor configured to: receive measurements of the first reflected pulse and the second reflected pulse from the acoustic transducer, and determine the acoustic property of the fluid in the wellbore from the received measurements of the first reflected acoustic pulse and the second reflected acoustic pulse.
[0008] Examples of certain features of the apparatus and method disclosed herein are summarized rather broadly in order that the detailed description thereof that follows may be better understood. There are, of course, additional features of the apparatus and method disclosed hereinafter that will form the subject of the claims.
BRIEF DESCRIPTION OF THE DRAWINGS
[0009] For detailed understanding of the present disclosure, references should be made to the following detailed description, taken in conjunction with the accompanying drawings, in which like elements have been given like numerals and wherein:
FIG. 1 shows an illustrative wellbore system suitable for determining an acoustic property of fluid in a wellbore in one embodiment of the present disclosure;
FIG. 2 shows a detailed view of the fluid testing apparatus of FIG. 1 in one embodiment;
FIG. 3 shows various transmission and/or reflection paths for an acoustic pulse generated by an acoustic transducer of the fluid testing apparatus; and
FIGS. 4A and 4B show schematic waveforms of the pulses received at the acoustic transducer.
DETAILED DESCRIPTION OF THE DISCLOSURE
[0010] FIG. 1 shows an illustrative wellbore system 100 suitable for determining an acoustic property of fluid 108 in a wellbore 104 in one embodiment of the present disclosure.
The wellbore system 100 includes a member 102 that extends from a surface location 120 into a borehole or wellbore 104. The wellbore 104 may be an open wellbore or a cased wellbore, in various embodiments. A surface 104a (also referred to herein as a "wellbore wall 104a") of the wellbore 104 may be a surface of a formation or an interior face of a casing (not shown) disposed in the wellbore 104. An annulus 114 is formed between the member 102 and the wellbore wall 104a. In one embodiment, the member 102 may be a drillstring that includes a drill bit 106 at a bottom end for drilling the wellbore 104. A fluid
108 such as a drilling mud may be pumped into the wellbore 104 through a bore 112 in the member 102 to exit the member 102 at the drill bit 106. The fluid 108 then travels back to the surface location 120 via the annulus 114. In the annulus 114, the fluid 108 may include drilling mud as well as formation fluids and/or formation gases. Determining properties of the fluid in the annulus 114 is useful in drilling operations. The member 102 includes a fluid testing apparatus 110 suitable for determining a property of the fluid 108 in the annulus 114 of the wellbore 104.
[0011] FIG. 2 shows a detailed view of the fluid testing apparatus 110 of FIG. 1 in one embodiment. The fluid testing apparatus 110 includes an acoustic device 200 disposed on the member 102. The acoustic device 200 includes an acoustic transducer 202 and a faceplate 204, which may be a stepped faceplate, as described below. The faceplate 204 includes a first surface 210 and a second surface 212 that is opposite the first surface 210. The second surface 212 is a stepped surface, including a non-stepped face 214 and a stepped face 216. The distance between the non-stepped face 214 and the first surface 210 is less than the distance between the stepped face 216 and the first surface 210. As shown in FIG. 2, a perpendicular distance between the first surface 210 and the non-stepped face 214 is L0 and a perpendicular distance between the first surface 210 and the stepped face 216 is L0+x. Therefore, a perpendicular distance between the stepped face 216 and the non-stepped face 214 is x. In alternate embodiments, the second surface 212 may include more than two faces. The acoustic transducer 202 is coupled to the first face 210 of the faceplate 204 and transmits acoustic signals into the faceplate 204 and receives acoustic signals from the faceplate 204. A seal 206 between the acoustic device 200 and the member 102 prevents ingress of fluids into the member 102. As disposed on the member 102, the non-stepped face 214 is at a distance L from the wellbore wall 104a and stepped face 216 is at a distance L-x from the wellbore wall 104a.
[0012] The fluid testing apparatus 110 further includes a control unit 220 coupled to the acoustic transducer 202. The control unit 220 includes a processor 222 and a memory storage device 224. The memory storage device 224 may be any non-transitory computer- readable storage medium, such as a solid-state memory, ROM, RAM, etc. The memory storage device 224 includes a set of programs 226 stored therein. The programs 226 may include instructions that when read by the processor 222 enable the processor to, among other things, determine an acoustic property of the fluid 108 in the wellbore 104 based on measurements obtained from the acoustic device 200. The control unit 220 may further control an operation of the acoustic device 200 or, specifically, the acoustic transducer 202. The control unit 220 may be disposed downhole with the acoustic device 200 or may be situated at the surface location 120. [0013] FIG. 3 shows various transmission and/or reflection paths for an acoustic pulse generated by the acoustic transducer 202 of the exemplary acoustic device 200 of the present disclosure. The acoustic transducer 202 transmits an original acoustic pulse or signal that enters through the faceplate 204 at first surface 210 and travels through the faceplate 204 to the second surface 212. The original acoustic pulse may includes a first portion 302 that intercepts the non-stepped face 214 and a second portion 304 that intercepts the stepped face 216. Reflection and transmission of the incident pulses occurs at each of the non-stepped face 214 and the stepped face 216.
[0014] For the first portion 302 impinging on non-stepped face 214, an internally reflected signal (Ab) may be reflected back through the faceplate 204 to the acoustic transducer 202. Another part of the first portion 302 is transmitted into the fluid 108 as indicated by signal Abb- Signal Abb propagates through the fluid 108 to the wellbore wall 104a and is reflected from the wellbore wall 104a back through the fluid 108 to the non- stepped face 214. Signal Abb then passes through the non-stepped face 214 and propagates back to the acoustic transducer 202. For signals resulting from the first portion 302, the path length in the faceplate 204 is distance LQ and the path length in the fluid 108 is distance L.
[0015] Similarly, for the second portion 304 impinging on the stepped face 216, an internally reflected signal Aa may be reflected back through the faceplate 204 to the acoustic transducer 202. Another part of the first portion 302 is transmitted into the fluid 108 as indicated by signal Aaa. Signal Aaa propagates through the fluid 108 to the wellbore wall 104a and is reflected from the wellbore wall 104a back through the fluid 108 to the stepped face 216. Signal Aaa then passes through the stepped face 216 and propagates back to the acoustic transducer 202. For signals resulting from the second portion 304, the path length in the faceplate 204 is distance Lo+x and the path length in the fluid 108 is distance L-x.
[0016] Signals propagating through the faceplate 204 travel at an acoustic velocity ex. Signals propagating through the fluid 108 travel at an acoustic velocity <¾ also known as "mud velocity." The acoustic velocity <¾ may be an unknown value that is determined via the methods disclosed herein. The acoustic velocity cx either may be a known quantity or may be determined using the methods disclosed herein. A sudden drop in the mud velocity can indicate gas influx from the formation into the drilling mud.
[0017] FIGS. 4A and 4B show measured waveforms (Va, Vb, Vaa and Vbb) of the respective pulses Aa, Ab, Aaa and Abb (FIG. 3) received at the acoustic transducer 202. FIG.
4 A shows the waveform measurements obtained when a velocity of sound (<¾) in the faceplate 204 is greater than a velocity of sound (<¾) in the fluid 108. The travel time for a selected pulse is a difference between a time at which the original acoustic pulse is generated at the acoustic transducer 202 and time at which the reflected pulse corresponding to the selected pulse is detected at the acoustic transducer 202. Pulse Aa (traveling entirely within the faceplate 204) has a travel time Ta, pulse Ab (traveling entirely within the faceplate 204) has a travel time Tb, pulse Aaa (traveling within both the faceplate 204 and the fluid 108) has a travel time Taa and pulse Abb (traveling within both the faceplate 204 and the fluid 108) has a travel time 7¾. Since, pulses Aa and Ab are internally reflected, their travel times Ta and Tb are earlier that the travel times Taa and 7¾ of pulses Aaa and Abb, which travel through the fluid 108 and are reflected from the wellbore wall 104a. Since the pulse Aaa spends more time in the faceplate 204 than pulse Abb and since CX>CL, pulse Aaa arrives before pulse Abb- [0018] FIG. 4B shows the measurements obtained when a velocity of sound in the faceplate 204 (<¾) is less than a velocity of sound (<¾) in the fluid 108. For the internally reflected pulses Aa and Ab, the travel times do not change. However, since pulse Aaa spends more time in the faceplate 204 than pulse Abb and since CX<CL, pulse Abb arrives before pulse
[0019] The equations for round-trip travel time for a selected reflected pulse may be written in equation form. The round-trip travel time is a function of a length of a path (path length) for the pulse in a particular medium (i.e., the faceplate 204 and/or the fluid 108) as well as the acoustic velocities (i.e., cx and/or c ) of the particular medium. The equation for a round-trip travel time for signal Aaa is:
Taa = 2{L0 + x)/cx + 2{L - x)/cL Eq. (1)
The equation for a round-trip travel time for signal Abb is:
Tbb = 2L0/cx + 2L/cL Eq. (2)
From Eqs. (1) and (2), the difference between travel times for signal Aaa and signal Abb is Taa - Tbb = 2x(l/cx - l/cL) Eq. (3)
Since Taa, bb are measured quantities and x and cx are known quantities, the speed of sound of the fluid 108 in the wellbore 104 may be determined by solving Eq. (3) to obtain:
cL = l/[l/cx - {Taa - Tbb)/2x] Eq. (4)
Once the speed of sound in the fluid 108 in the wellbore 104 is known, a standoff L between the faceplate 204 from the wellbore wall 104a (or equivalently, between the member 102 and the wellbore wall 104a) may be determined as
= cLTbb/2 - LQ/cx Eq. (5) [0020] In addition, the speed of sound (cx) in the faceplate 204 may be determined from round-trip travel times of the internally reflected acoustic pulses (i.e., signals Aa and Ab), as shown in Eqs. (6) - (8). The round-trip travel time for signal Aa is:
Ta = 2 (L0 + x)/cx Eq. (6) and the round-trip travel time for signal Ab is
Tb = 2L0/cx Eq. (7)
From Eqs. (6) and (7), the speed of sound <¾ is determined as
cx = 2x/{Ta - Tb) Eq. (8)
[0021] In another aspect of the present disclosure, acoustic attenuation coefficients of the faceplate 204 and of the fluid 108 may be determined. Additionally, an acoustic impedance of the fluid 108 may be determined. The amplitudes of the returned pulse waveforms (Va, Vb, Vaa, and Vbb) are given by the following equations (9) - (12):
Vb = P0e -2^o ££l£ Eq. (9)
Zf+Ζχ
Va = p0e -2ax(L0 +x)£c¾ Eq. (10)
Zf+Ζχ
Vbb = Poe -2a*L° -^ e -2^ fZ - Eq. (1 1)
(Zf+Zx) Zc+Zf
Vaa = P0e-2^+X ) ^H^ e -2af(L-x) ^ Eq. ( 1 2)
(Zf+Zx) zc+zf
In Eqs. (9) - (12), P0 is the amplitude of the original acoustic signal generated by the acoustic transducer 202, and ax and a/ are the sound attenuation coefficient of the material of the face plate and the sound attenuation coefficient of the fluid 108, respectively. Z/, Ζχ and Zc are the acoustic impedances of the fluid, the material of the faceplate 204 and the material of the borehole wall (or of the casing), respectively.
[0022] The attenuation coefficient of the face plate (ax) may be determined from Eq. (9) and Eq. (10), to obtain:
«* = -stei- <13>
The attenuation coefficient of the fluid (aj) may be determined from Eq. (1 1) and Eq. (12) and the determined coefficient ax from Eq. (13) to obtain:
Figure imgf000008_0001
By taking the ratio of Vbb (Eq. (1 1)) and Vb (Eq. (9)), the following Eq. (15) is obtained: Vbb _ 4ZfzX c -2afL Zc~zf
Eq. (15) Vb zj~zx Zc+Zf
The fluid impedance Z may then be solved from Eq. (15). Zc is a known acoustic impedance of the material (e.g., steel casing) of the wellbore wall 104a. Zy is an acoustic impedance of the material of the faceplate 204, which is either known or may be determined from Eq. (13), L is the standoff distance (determined in Eq. (5)) and a/ is the fluid attenuation coefficient, determined in Eq. (14). Moreover, the density of the fluid may be then estimated by pf =
[0023] Therefore, in one aspect, the present disclosure provides a method of determining an acoustic property of a fluid in a wellbore, the method including: placing a faceplate in the wellbore with a stepped surface of the faceplate in contact with the fluid, wherein the stepped surface includes a non-stepped face and a stepped face; transmitting an acoustic pulse through the faceplate into the fluid, wherein a first portion of the acoustic pulse passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; receiving a first reflected acoustic pulse related to the first portion of the acoustic pulse from a wellbore surface and a second reflected acoustic pulse related to the second portion of the acoustic pulse from the wellbore surface; obtaining a measurement of the first reflected acoustic pulse and a measurement of the second reflected pulse; and determining from the obtained measurements the acoustic property of the fluid in the wellbore. In one embodiment, a path of the first reflected acoustic pulse intersects the non-stepped face of the faceplate and a path of the second reflected acoustic pulse intersects the stepped face of the faceplate. When the acoustic property of the fluid is an acoustic velocity of the fluid, the method determines the acoustic velocity of the fluid using a difference between a travel time of the first reflected signal and a travel time of the second reflected signal. The difference between the travel time of the first reflected signal and the travel time of the second reflected signal is related to a difference between a path length through the fluid of the first reflected signal and a path length through the fluid of the second reflected signal. Additionally, a standoff distance between the faceplate and the wellbore surface may be determined using the determined acoustic velocity of the fluid. When the acoustic property of the fluid is an acoustic attenuation of the fluid, the acoustic attenuation of the fluid may be determined from an amplitude of the first reflected signal an amplitude of the second reflected signal. The method may further include determining an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid. [0024] In another aspect, the present disclosure provides an apparatus for determining an acoustic property of a fluid in a wellbore, the apparatus including: a faceplate having a stepped surface that includes a non-stepped face and a stepped face, wherein the stepped surface is coupled to the fluid in the wellbore; an acoustic transducer configured to transmit an acoustic signal to pass through the stepped surface of the faceplate into the fluid, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; and a processor configured to: receive measurements of a first reflected pulse related to reflection of the first portion of the transmitted acoustic signal from a wellbore surface a second reflected pulse related to reflection of the second portion of the transmitted acoustic signal from the wellbore surface, and determine the acoustic property of the fluid in the wellbore from the received measurements of the first reflected acoustic pulse and the second reflected acoustic pulse. In one embodiment, a path of the first reflected signal intersects the non-stepped face a path of the second reflected acoustic pulse intersects the stepped face. When the acoustic property of the fluid is an acoustic velocity of the fluid, the processor may determine the acoustic velocity of the fluid from a difference between a travel time of the first reflected signal and a travel time of the second reflected signal. The processor may further determine a standoff distance between a member and the wellbore surface using the determined acoustic velocity for the faceplate disposed on the member. A difference between the travel time of the first reflected signal and the travel time of the second reflected signal is related to a difference in a path length of the first reflected signal through the fluid and a path length of the second reflected signal through the fluid. When the acoustic property of the fluid is attenuation of an acoustic signal in the fluid, the processor may determine the attenuation of the acoustic signal in the fluid using an amplitude of the first signal and an amplitude of the second signal. The processor may further determine an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
[0025] In yet another aspect, the present disclosure provides a system for determining an acoustic property of a fluid in a wellbore, the system including: a member disposed in the wellbore; a faceplate disposed on the member, the faceplate having a stepped surface coupled to the fluid in the wellbore, wherein the stepped surface includes a non-stepped face and a stepped face; an acoustic transducer configured to transmit an acoustic signal into the faceplate, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid through the non-stepped face and a second portion of the transmitted acoustic signal passes from the faceplate into the fluid through the stepped face, the acoustic transducer further configured to receive a first reflected acoustic signal related reflection of the first portion of the transmitted acoustic signal from a surface of the wellbore and a second reflected acoustic signal related to reflection of the second portion of the transmitted acoustic signal from the surface of the wellbore; and a processor configured to: receive measurements of the first reflected pulse and the second reflected pulse from the acoustic transducer, and determine the acoustic property of the fluid in the wellbore from the received measurements of the first reflected acoustic pulse and the second reflected acoustic pulse. In one embodiment, a path of the first reflected acoustic pulse intersects the non-stepped face and a path of the second reflected acoustic pulse intersects the stepped face. When the acoustic property of the fluid is an acoustic velocity of the fluid, the processor may determine the acoustic velocity of the fluid from a difference between measured travel times of the first reflected signal and the second reflected signal. The processor may further determine a standoff distance between the member and the wellbore surface. When the acoustic property of the fluid is attenuation of an acoustic signal in the fluid, the processor may determine the attenuation of the acoustic signal in the fluid using an amplitude of the first signal and an amplitude of the second signal. The processor may further determine an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
[0026] While the disclosure has been described with reference to an exemplary embodiment or embodiments, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements thereof without departing from the scope of the disclosure. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the disclosure without departing from the essential scope thereof. Therefore, it is intended that the disclosure not be limited to the particular embodiment disclosed as the best mode contemplated for carrying out this disclosure, but that the disclosure will include all embodiments falling within the scope of the claims.

Claims

CLAIMS What is claimed is:
1. A method of determining an acoustic property of a fluid in a wellbore, comprising:
placing a faceplate in the wellbore with a stepped surface of the faceplate in contact with the fluid, wherein the stepped surface includes a non-stepped face and a stepped face; transmitting an acoustic pulse through the faceplate into the fluid, wherein a first portion of the acoustic pulse passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face;
receiving a first reflected acoustic pulse related to the first portion of the acoustic pulse from a wellbore surface and a second reflected acoustic pulse related to the second portion of the acoustic pulse from the wellbore surface;
obtaining a measurement of the first reflected acoustic pulse and a measurement of the second reflected pulse; and
determining from the obtained measurements the acoustic property of the fluid in the wellbore.
2. The method of claim 1, wherein a path of the first reflected acoustic pulse intersects the non-stepped face of the faceplate and a path of the second reflected acoustic pulse intersects the stepped face of the faceplate.
3. The method of claim 1, wherein the acoustic property of the fluid further comprises an acoustic velocity of the fluid, further comprising determining the acoustic velocity of the fluid using a difference between a travel time of the first reflected signal and a travel time of the second reflected signal.
4. The method of claim 3, wherein the difference between the travel time of the first reflected signal and the travel time of the second reflected signal is related to a difference between a path length through the fluid of the first reflected signal and a path length through the fluid of the second reflected signal.
5. The method of claim 3, further comprising determining a standoff distance between the faceplate and the wellbore surface using the determined acoustic velocity of the fluid.
6. The method of claim 1, wherein the acoustic property of the fluid further comprises acoustic attenuation of the fluid, further comprising determining the acoustic attenuation of the fluid from an amplitude of the first reflected signal an amplitude of the second reflected signal.
7. The method of claim 6, further comprising determining an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
8. An apparatus for determining an acoustic property of a fluid in a wellbore, comprising:
a faceplate having a stepped surface that includes a non-stepped face and a stepped face, wherein the stepped surface is coupled to the fluid in the wellbore;
an acoustic transducer configured to transmit an acoustic signal to pass through the stepped surface of the faceplate into the fluid, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid via the non-stepped face and a second portion of the acoustic pulse passes from the faceplate into the fluid via the stepped face; and a processor configured to:
receive measurements of a first reflected pulse related to reflection of the first portion of the transmitted acoustic signal from a wellbore surface a second reflected pulse related to reflection of the second portion of the transmitted acoustic signal from the wellbore surface, and
determine the acoustic property of the fluid in the wellbore from the received measurements of the first reflected acoustic pulse and the second reflected acoustic pulse.
9. The apparatus of claim 8, wherein a path of the first reflected signal intersects the non-stepped face a path of the second reflected acoustic pulse intersects the stepped face.
10. The apparatus of claim 8, wherein the acoustic property of the fluid further comprising an acoustic velocity of the fluid and the processor is further configured to determine the acoustic velocity of the fluid from a difference between a travel time of the first reflected signal and a travel time of the second reflected signal.
11. The apparatus of claim 10, wherein the faceplate is disposed on a member in the wellbore, further comprising determining a standoff distance between the member and the wellbore surface using the determined acoustic velocity.
12. The apparatus of claim 10, wherein a difference between the travel time of the first reflected signal and the travel time of the second reflected signal is related to a difference in a path length of the first reflected signal through the fluid and a path length of the second reflected signal through the fluid.
13. The apparatus of claim 8, wherein the acoustic property of the fluid further comprises attenuation of an acoustic signal in the fluid and the processor is further configured to determine the attenuation of the acoustic signal in the fluid using an amplitude of the first signal and an amplitude of the second signal.
14. The apparatus of claim 13, wherein the processor is further configured to determine an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
15. A system for determining an acoustic property of a fluid in a wellbore, comprising:
a member disposed in the wellbore;
a faceplate disposed on the member, the faceplate having a stepped surface coupled to the fluid in the wellbore, wherein the stepped surface includes a non-stepped face and a stepped face;
an acoustic transducer configured to transmit an acoustic signal into the faceplate, wherein a first portion of the transmitted acoustic signal passes from the faceplate into the fluid through the non-stepped face and a second portion of the transmitted acoustic signal passes from the faceplate into the fluid through the stepped face, the acoustic transducer further configured to receive a first reflected acoustic signal related reflection of the first portion of the transmitted acoustic signal from a surface of the wellbore and a second reflected acoustic signal related to reflection of the second portion of the transmitted acoustic signal from the surface of the wellbore; and
a processor configured to:
receive measurements of the first reflected pulse and the second reflected pulse from the acoustic transducer, and
determine the acoustic property of the fluid in the wellbore from the received measurements of the first reflected acoustic pulse and the second reflected acoustic pulse.
16. The system of claim 15, wherein a path of the first reflected acoustic pulse intersects the non-stepped face and a path of the second reflected acoustic pulse intersects the stepped face.
17. The system of claim 15, wherein acoustic property of the fluid further comprising an acoustic velocity of the fluid and the processor is further configured to determine the acoustic velocity of the fluid from a difference between measured travel times of the first reflected signal and the second reflected signal.
18. The system of claim 17, further comprising determining a standoff distance between the member and the wellbore surface.
19. The system of claim 15, wherein the acoustic property of the fluid further comprises attenuation of an acoustic signal in the fluid and the processor is further configured to determine the attenuation of the acoustic signal in the fluid using an amplitude of the first signal and an amplitude of the second signal.
20. The system of claim 19, wherein the processor is further configured to determine an acoustic impedance of the fluid using the determined acoustic attenuation of the fluid.
PCT/US2015/031022 2014-05-15 2015-05-15 Acoustic standoff and mud velocity using a stepped transmitter WO2015175905A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US14/278,839 2014-05-15
US14/278,839 US9366133B2 (en) 2012-02-21 2014-05-15 Acoustic standoff and mud velocity using a stepped transmitter

Publications (1)

Publication Number Publication Date
WO2015175905A1 true WO2015175905A1 (en) 2015-11-19

Family

ID=54480759

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/US2015/031022 WO2015175905A1 (en) 2014-05-15 2015-05-15 Acoustic standoff and mud velocity using a stepped transmitter

Country Status (1)

Country Link
WO (1) WO2015175905A1 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2020185776A1 (en) * 2019-03-12 2020-09-17 Baker Hughes Oilfield Operations Llc Self-calibrated method of determining borehole fluid acoustic properties

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050034530A1 (en) * 2002-05-15 2005-02-17 Halliburton Energy Services, Inc. Acoustic doppler downhole fluid flow measurement
US7364007B2 (en) * 2004-01-08 2008-04-29 Schlumberger Technology Corporation Integrated acoustic transducer assembly
US20120170406A1 (en) * 2005-08-01 2012-07-05 Baker Hughes Incorporated Early Kick Detection in an Oil and Gas Well
US20120285232A1 (en) * 2011-03-16 2012-11-15 Baker Hughes Incorporated Sample channel for a sensor for measuring fluid properties
US20130192359A1 (en) * 2010-06-09 2013-08-01 Halliburton Energy Services, Inc. Formation evaluation probe set quality and data acquisition method

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050034530A1 (en) * 2002-05-15 2005-02-17 Halliburton Energy Services, Inc. Acoustic doppler downhole fluid flow measurement
US7364007B2 (en) * 2004-01-08 2008-04-29 Schlumberger Technology Corporation Integrated acoustic transducer assembly
US20120170406A1 (en) * 2005-08-01 2012-07-05 Baker Hughes Incorporated Early Kick Detection in an Oil and Gas Well
US20130192359A1 (en) * 2010-06-09 2013-08-01 Halliburton Energy Services, Inc. Formation evaluation probe set quality and data acquisition method
US20120285232A1 (en) * 2011-03-16 2012-11-15 Baker Hughes Incorporated Sample channel for a sensor for measuring fluid properties

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2020185776A1 (en) * 2019-03-12 2020-09-17 Baker Hughes Oilfield Operations Llc Self-calibrated method of determining borehole fluid acoustic properties
GB2596687A (en) * 2019-03-12 2022-01-05 Baker Hughes Oilfield Operations Llc Self-calibrated method of determining borehole fluid acoustic properties
US11359488B2 (en) 2019-03-12 2022-06-14 Baker Hughes Oilfield Operations Llc Self-calibrated method of determining borehole fluid acoustic properties
GB2596687B (en) * 2019-03-12 2022-12-28 Baker Hughes Oilfield Operations Llc Self-calibrated method of determining borehole fluid acoustic properties

Similar Documents

Publication Publication Date Title
US9891335B2 (en) Wireless logging of fluid filled boreholes
US9651709B2 (en) Distributed acoustic sensing system with variable spatial resolution
US8181535B2 (en) Flow measuring apparatus using tube waves and corresponding method
US9109433B2 (en) Early kick detection in an oil and gas well
RU2607826C2 (en) Downhole tool for determining flow velocity
US20040003658A1 (en) Acoustic doppler downhole fluid flow measurement
US9366133B2 (en) Acoustic standoff and mud velocity using a stepped transmitter
WO2010102109A2 (en) Early kick detection in an oil and gas well
US8978481B2 (en) Simultaneous ultrasonic cross-correlation and transit time measurements for multiphase flow rate analysis
US9726014B2 (en) Guided wave downhole fluid sensor
US9587485B2 (en) Methods and apparatus to detect fluid distributions
NO318894B1 (en) Method of a estimates the hydraulic conductivity of a petrophysical discontinuity in the sidewall of a borehole
US11098583B1 (en) Method for determining the integrity of a solid bonding between a wellbore and a casing
WO2013126388A1 (en) Early kick detection in an oil and gas well
US10254438B2 (en) Adaptive feedback for phase estimation and adjustment
US20090240436A1 (en) Data processing method for determining acoustic velocities from acoustic well logging instruments
US8077545B2 (en) Method for detecting gas influx in wellbores and its application to identifying gas bearing formations
WO2015175905A1 (en) Acoustic standoff and mud velocity using a stepped transmitter
US20150122479A1 (en) Time of flight through mud
WO2012068205A2 (en) Method and apparatus for determining the size of a borehole
Zhang et al. An ultrasonic flowmeter in production boreholes of oilfields
Elahifar et al. Accuracy of ultrasonic sensor in caliper log

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 15792092

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 15792092

Country of ref document: EP

Kind code of ref document: A1