Well integrity analysis using sonic measurements over depth interval
US-2019055830-A1 · Feb 21, 2019 · US
US11714209B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11714209-B2 |
| Application number | US-202016839842-A |
| Country | US |
| Kind code | B2 |
| Filing date | Apr 3, 2020 |
| Priority date | Apr 11, 2019 |
| Publication date | Aug 1, 2023 |
| Grant date | Aug 1, 2023 |
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In a method to transform logs, an acoustic logging tool inserted into a borehole includes a source and an array of receiver stations. Each station includes a receiver spaced along the tool from the source by successively greater distances. In the method, the source emits energy (I) to cause the propagation towards the stations of plural signals exhibiting paths characteristic of first and second respective modes and (II) to stimulate a receiver of each station to generate an output signal per station that indicates the signal packets and represents the modes in combination with one another. In the method, the output signals are transformed into transformed signals containing phase/amplitude information of each mode. The phase/amplitude are linked by an operator to the slowness and attenuation of the mode and the transmitter-receiver distance of the station. The phase/amplitude are used to extract slowness and attenuation information for each mode.
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The invention claimed is: 1. A method of invertibly transforming acoustic log signals comprising the steps of: a) inserting into a borehole, forming part of a borehole-formation system in which the borehole penetrates a rock formation, an elongate acoustic logging tool, the acoustic logging tool including at least one acoustic source and, spaced from the acoustic source along the logging tool, a sequential array of two or more acoustic signal receiver stations, the receiver stations each including at least one receiver and being spaced along the logging tool from the acoustic source by successively greater known transmitter-receiver distances whose minimum separation is greater than the minimum detectable wavelength corresponding to a formation slowness range of interest; b) causing the acoustic source to emit acoustic energy in a manner (I) effecting the propagation in the borehole-formation system towards the receiver stations of plural signal packets exhibiting paths characteristic of at least first and second respective modes one or more of which is dispersive and (II) stimulating at least two receivers of respective, sequential, spaced receiver stations to generate at least one output signal per receiver station that is indicative of the signal packets, received at the at least one receiver of each respective receiver station, representing the modes in combination with one another; c) transforming the output signals into respective transformed mode signals containing phase and amplitude information of each respective mode across the array and in which estimated phase and amplitude information are linked by an operator to the slowness and attenuation characteristics of the respective mode and the transmitter-receiver distance of the respective receiver station; d) using the estimated phase and amplitude information for each mode from each receiver in the acoustic array to extract slowness and attenuation information for each mode from the output signals and generating signals indicative of the slowness and/or attenuation characteristics; and e) using the signals indicative of the slowness and/or attenuation characteristics in plotting, storing; transmitting, displaying, printing or further processing the slowness and/or attenuation characteristics, wherein the Step d) of using the estimated phase and amplitude information for each mode to extract slowness and attenuation information for each mode from the output signals includes f) generating complex spectra information from the receiver array signals and taking the real and imaginary parts of the transformed mode signals containing respective amplitude and phase components of the respective modes; wherein the method includes the steps of: g) in cases where the number of receivers exceeds the minimum necessary to determine slowness and amplitude values for each frequency and mode of interest, solving for mode amplitude and slowness by minimizing in a least squares sense the differences between real and imaginary mode amplitudes and the real and imaginary amplitudes of the combined modes observed in the spectra of received signals for each frequency, and h) representing the real and imaginary parts between estimated and received signals as objective function signals and summing the squares of the objective function signals over the two or more receiver stations; and wherein the Step g) includes minimizing the error between terms representing the amplitude and phase detected at the receivers and terms representing amplitude and phase components in the real and imaginary parts, including using initial estimates of the amplitude and phase components of the respective modes, and using a search method to minimize the said error. 2. A method according to claim 1 wherein the step of transforming the output signals into transformed mode signals is performed using an electronic circuit or using a processing device. 3. A method according to claim 1 wherein the inter-receiver distance along the logging tool between each adjacent pair of the receiver stations is the same. 4. A method according to claim 1 wherein the Step g) of minimizing the error between terms representing the amplitude and phase detected at the receivers, and terms representing amplitude and phase components in the real and imaginary parts includes seeding expressions representing the signals with estimated values of the slownesses of the respective modes, and solving for values of the respective amplitudes that minimize the said error. 5. A method according to claim 1 wherein the Step c) of transforming the output signals into respective transformed mode signals includes representing the transformed mode signals in the form C n cos(c n )−(A cos(a n )+B cos(b n ))=0, in which C n is the amplitude of the signal stimulated at receiver n of the array; c n is the corresponding phase; A is the estimated amplitude of the first mode stimulated across the array at a given frequency; a n is the estimated phase of the first mode stimulated at receiver n of the array; B is the estimated amplitude of the second mode stimulated across the array at the given frequency; and b n is the estimated phase of the second mode stimulated at receiver n of the array; and wherein the Step d) of using the estimated phase and amplitude information for each mode to extract slowness and attenuation information for each mode includes using the error expressions to minimize the error between the terms C n and c n on the one hand, and the terms A, B, a n and b n on the other. 6. A method according to claim 1 including repeating at least Steps c) and d) in respect of a range of frequencies of the respective output signals. 7. A method according to claim 1 including the step of constructing respective mode signals in respect of each receiver within the array. 8. A method according to claim 1 wherein the first and second modes respectively are flexural and Stoneley acoustic modes. 9. A method according to claim 1 wherein the first and second modes respectively are flexural and Stoneley acoustic modes; and including the step of creating a reconstructed array signal from the constructed respective mode signals in order to permit comparison between the reconstructed array signal and the output signals. 10. A borehole-apparatus system comprising: (A) a borehole penetrating a rock formation; (B) an elongate acoustic logging tool, the acoustic logging tool including at least one acoustic source and, spaced from the acoustic source along the logging tool, a sequential array of acoustic signal receiver stations, the receiver stations each including at least one receiver and being spaced along the logging tool from the acoustic source by successively greater known transmitter-receiver distances, the acoustic source being capable of emitting acoustic energy with linear or non-linear phase characteristics in a manner (i) effecting the propagation in the borehole-formation system towards the receiver stations of plural signal packets exhibiting paths characteristic of at least first and second respective modes one or more of which is dispersive and (ii) stimulating at least one receiver of each sequential receiver station to generate at least one output signal per receiver station that is indicative of the signal packets, received at the at least one receiver of each respective receiver station, representing the modes in combination with one another; and (C) one or more processing devices that is operatively connected to the acoustic logging tool and is capable of carrying out in respect of the output signals at least Steps (c), (d), (f), (q) and (h) according to the method of claim 1 . 11. A computer-readable storage medi
Analysing data · CPC title
using acoustic waves · CPC title
for determining seismic attributes, e.g. amplitude, instantaneous phase or frequency, reflection strength or polarity · CPC title
Slowness, e.g. tau-pi · CPC title
Seismic attributes, e.g. amplitude, polarity, instant phase · CPC title
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