Determining shear slowness from dipole source-based measurements aquired by a logging while drilling acoustic measurement tool
Abstract
A technique includes receiving data representing time domain waveforms acquired by receivers of a drilling string-disposed acoustic measurement tool in response to energy emitted by at least one dipole source of the tool. The technique includes processing the data to determine slowness values associated with a plurality of acoustic modes, including a formation flexural acoustic mode and a tool flexural acoustic mode. The technique includes identifying slowness-frequency pairs from the slowness values and determining a shear slowness based at least in part on the identified slowness-frequency pairs.
Claims
exact text as granted — not AI-modifiedWhat is claimed is:
1 . A method comprising:
receiving data representing time domain waveforms acquired by receivers of a drilling string-disposed acoustic measurement tool in response to energy emitted by at least one dipole source of the tool; processing the data to determine slowness values associated with a plurality of acoustic modes including a formation flexural acoustic mode and a tool flexural acoustic mode; identifying slowness-frequency pairs from the slowness values; and determining a shear slowness based at least in part on the identified slowness-frequency pairs.
2 . The method of claim 1 , wherein processing the data to extract the at least one slowness dispersion characteristic comprises:
dividing a relatively larger frequency range into a plurality of relatively smaller frequency ranges, wherein each frequency range is associated with a plurality of frequencies; and for each frequency range of the plurality of frequency ranges:
applying beamforming to determine a spectrum that varies with a phase slowness;
identifying at least one peak of the spectrum; and
using a result of the identifying to determine at least one of the slowness values.
3 . The method of claim 2 , wherein applying the beamforming comprises applying Capon beamforming.
4 . The method of claim 2 , wherein applying the beamforming comprises transforming the time domain waveforms into frequency domain waveforms;
de-dispersing the frequency domain waveforms, wherein the de-dispersing comprises assigning a group slowness to the frequency domain waveforms to remove the mode dispersion in a wavenumber domain; and selectively combining the results of the de-dispersing to spatially smooth the de-dispersed frequency domain waveforms with respect to a receiver offset direction.
5 . The method of claim 1 , wherein identifying the slowness-frequency pairs comprises basing the identification at least in part on an uncertainty versus frequency for at least some of the slowness values.
6 . The method of claim 1 , wherein identifying the slowness-frequency pairs comprises determining at least one frequency range in which some of the slowness values are sensitive to the shear slowness.
7 . The method of claim 1 , further comprising performing the receiving and processing multiple times for multiple dipole source firings, wherein:
identifying the slowness-frequency pairs comprises comparing a consistency of slowness values determined from the firings.
8 . The method of claim 1 , wherein:
the acoustic measurement tool acquires the data in response to measurements in a fast formation; and determining the shear slowness comprises:
constructing a formal flexural dispersion based on at least some of the slowness values; and
determining an asymptote of the constructed formation flexural dispersion.
9 . The method of claim 1 , wherein determining the dipole shear slowness comprises inverting for the shear slowness based at least in part on the identified slowness-frequency pairs.
10 . The method of claim 9 , wherein inverting for the shear slowness comprises performing a one parameter inversion.
11 . The method of claim 9 , wherein inverting for the shear slowness comprises inverting for the shear slowness and a mud slowness.
12 . The method of claim 9 , wherein:
the emitted energy propagates in a fast formation; identifying the slowness-frequency pairs from the slowness values comprises identifying slowness-frequency pairs that are associated with the formation flexural acoustic mode and are not associated with the tool flexural acoustic mode; and inverting for the shear slowness comprises performing model-based inversion to determine the shear slowness based on the identified slowness-frequency pairs.
13 . The method of claim 9 , wherein:
the emitted energy propagates in a fast formation; identifying the slowness-frequency pairs from the slowness values comprises identifying slowness-frequency pairs that are associated with the tool flexural acoustic mode and are not associated with the formation flexural acoustic mode; and inverting for the shear slowness comprises performing model-based inversion to determine the shear slowness based on the identified slowness-frequency pairs.
14 . The method of claim 9 , wherein:
the emitted energy propagates in a fast formation; identifying the slowness-frequency pairs from the slowness values comprises identifying slowness-frequency pairs that are associated with the tool flexural acoustic mode and are associated with the formation flexural acoustic mode; and inverting for the shear slowness comprises performing model-based inversion to determine the shear slowness based on the identified slowness-frequency pairs.
15 . An apparatus comprising:
an interface to receive data representing data acquired by a logging while drilling (LWD) tool in a well in response to energy being emitted by at least one dipole source; and a processor to:
process the data to extract slowness estimates associated with a plurality of acoustic modes including a formation flexural acoustic mode and a tool flexural acoustic mode; and
determine a shear slowness based at least in part on selected slowness-frequency pairs identified from the slowness estimates.
16 . The apparatus of claim 15 , wherein:
the energy propagates in a fast formation; at least some of the slowness estimates are associated with a formation flexural dispersion; and the processor integrates energy associated with the formation flexural dispersion based at least in part on the identified slowness-frequency pairs to determine the shear slowness.
17 . The apparatus of claim 15 , wherein the processor performs a model-based inversion based at least in part on the selected slowness-frequency pairs to determine the shear slowness.
18 . The apparatus of claim 15 , wherein the slowness-frequency pairs are associated with the tool flexural acoustic mode.
19 . A method comprising:
receiving data representing time domain waveforms acquired by receivers of a drilling string-disposed acoustic measurement tool in response to energy emitted by at least one dipole source of the tool propagating through a slow formation; processing the data to determine slowness values associated with a plurality of acoustic modes including a formation flexural acoustic mode and a tool flexural acoustic mode; identifying slowness-frequency pairs from the slowness values; and determining a shear slowness based at least in part on the identified slowness-frequency pairs.
20 . The method of claim 19 , wherein:
identifying the slowness-frequency pairs from the slowness values comprises identifying slowness-frequency pairs associated with the tool flexural acoustic mode; and determining the shear slowness comprises using model-based inversion to determine the shear slowness based at least in part on the slowness-frequency pairs associated with the tool flexural acoustic mode.Join the waitlist — get patent alerts
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