# US 2014/0195160 A1 · Formation property determination apparatus, methods, and systems > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2014/0195160 A1 - Document ID: US20140195160A1 - Status: Published application - Kind: A1 - Application number: 13/878,727 - Filed: 2012-08-28 - Published: 2014-07-10 - Earliest claimed: 2011-09-12 - Assignees: Halliburton Energy Services, Inc. - Inventors: Mark V. Collins; Arthur Cheng - Web page: https://patentgrep.com/patent/US20140195160A1 ## CPC - G01V 1/50: Analysing data - G01V 1/36: Effecting static or dynamic corrections on records, e.g. correcting spread; Correlating seismic signals; Eliminating effects of unwanted energy - G01V 2210/1299: Subsurface, e.g. in borehole or below weathering layer or mud line - G01V 2210/27: Other pre-filtering - G01V 2210/67: Wave propagation modeling - G01V: GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS (means for indicating the location of accidentally buried, e.g. snow-buried, persons A63B29/02) ## Abstract In some embodiments, apparatus and systems, as well as methods, may operate to record a plurality of acoustic waveforms comprising cross-dipole waveforms and corresponding to acoustic waves received 5 at azimuthally orthogonal dipole receiver arrays surrounded by a geological formation, the waves being generated by azimuthally orthogonal dipole transmitter arrays. Further activity may include defining an objective function dependent on the cross-dipole waveforms, eigenvalues, an azimuth angle corresponding to an 10 orientation of the transmitter and receiver arrays; minimizing the objective function with respect to said angle and the set of auxiliary parameters; and determining at least one property of the geological formation based on the global minimum. Additional apparatus, systems, and methods are disclosed. ## Claims ### Claim 1 An apparatus, comprising: azimuthally orthogonal dipole receiver arrays and azimuthally orthogonal transmitter arrays; logic to record a plurality of acoustic waveforms corresponding to acoustic waves received at the azimuthally orthogonal dipole receiver arrays, the acoustic waves being generated by the azimuthally orthogonal transmitter arrays; and a signal processor to estimate a global minimum of an objective function with respect to an azimuth angle and a set of auxiliary parameters, wherein the azimuth angle corresponds to an orientation of the transmitter arrays and the receiver arrays relative to fast and slow principal flexural wave axes, with the signal processor configured to estimate fast and slow principal flexural waves propagating along the axes and characterized by the waveforms as ordered complex eigenvalues of a waveform matrix diagonalized by a unitary similarity transformation at each data point of the waveforms, and the objective function depending on the waveforms, the ordered eigenvalues, the azimuth angle, and the set of auxiliary parameters, wherein the signal processor is also configured to remove existing ambiguities associated with the fast and slow principal flexural wave axes. ### Claim 2 (depends on 1) The apparatus of claim 1, further comprising: a memory to receive and store values associated with the global minimum of the objective function, to include at least the azimuth angle. ### Claim 3 (depends on 1) The apparatus of claim 1, further comprising: a telemetry transmitter to communicate values associated with the global minimum of the objective function to a surface logging facility. ### Claim 4 A system, comprising: a down hole tool; azimuthally orthogonal dipole receiver arrays and azimuthally orthogonal transmitter arrays, each of the arrays attached to the down hole tool; logic to record a plurality of acoustic waveforms corresponding to acoustic waves received at the azimuthally orthogonal dipole receiver arrays, the acoustic waves being generated by the azimuthally orthogonal transmitter arrays; and a signal processor to estimate a global minimum of an objective function with respect to an azimuth angle and a set of auxiliary parameters, wherein the azimuth angle corresponds to an orientation of the transmitter arrays and the receiver arrays relative to fast and slow principal flexural wave axes, with the signal processor configured to estimate fast and slow principal flexural waves propagating along the axes and characterized by the waveforms as ordered complex eigenvalues of a waveform matrix diagonalized by a unitary similarity transformation at each data point of the waveforms, and the objective function depending on the waveforms, the ordered eigenvalues, the azimuth angle, and the set of auxiliary parameters, wherein the signal processor is also configured to remove existing ambiguities associated with the fast and slow principal flexural wave axes. ### Claim 5 (depends on 4) The system of claim 4, wherein the downhole tool comprises one of a wireline tool or a measurement while drilling tool. ### Claim 6 (depends on 4) The system of claim 4, further comprising: a surface computer comprising the signal processor. ### Claim 7 A processor-implemented method of estimating an azimuth angle, to execute on one or more processors that perform the method, comprising: recording a plurality of acoustic waveforms corresponding to acoustic waves received at azimuthally orthogonal dipole receiver arrays surrounded by a geological formation, the waves being generated by azimuthally orthogonal transmitter arrays, the azimuth angle corresponding to an orientation of the receiver arrays and the transmitter arrays relative to fast and slow principal flexural wave axes, wherein fast and slow principal flexural waves propagating along the axes and characterized by the waveforms being estimated as the ordered eigenvalues of a waveform matrix diagonalized by a unitary similarity transformation; defining an objective function dependent on the waveforms, the ordered eigenvalues, the azimuth angle, and a set of auxiliary parameters; minimizing the objective function with respect to the azimuth angle; and determining at least one anisotropy angle of the geological formation based on the global minimum. ### Claim 8 (depends on 7) The method of claim 7, wherein the matrix represents a set of data points in a space defined by receiver ring index position and time. ### Claim 9 (depends on 7) The method of claim 7, wherein the matrix represents a set of data points in a space defined by receiver ring index position and frequency. ### Claim 10 (depends on 7) The method of claim 7, further comprising: diagonalizing the waveform matrix by a unitary similarity transformation at each data point of the waveforms, by computing a unitary matrix having columns comprising complex eigenvectors of the waveform matrix at each of the data points of the waveforms; and computing the eigenvalues of the eigenvectors. ### Claim 11 (depends on 10) The method of claim 10, wherein diagonalizing the waveform matrix is accomplished using an analytical method or a numerical method. ### Claim 12 (depends on 7) The method of claim 7, further comprising: ordering the eigenvalues by ordering eigenvectors and corresponding ones of the eigenvalues across data points of the waveforms such that a difference in angle between the eigenvectors across the data points is minimized, and ordering the eigenvectors and the corresponding ones of the eigenvalues across the data points using a parameter correlated in a known way with the difference in the angle. ### Claim 13 (depends on 7) The method of claim 7, further comprising: ordering eigenvectors and corresponding ones of the eigenvalues across receiver rings at each frequency in a space defined by data points in the waveforms; estimating eigenvalue propagators across the receiver rings from the ordered eigenvalues at each frequency in the space; and ordering the eigenvectors, the corresponding ones of the eigenvalues, and the propagators over frequency by comparing relative phases associated with the estimates of the eigenvalue propagators at one frequency to relative phases associated with the estimates of the eigenvalue propagators at another frequency. ### Claim 14 (depends on 7) The method of claim 7, wherein the objective function is defined by utilizing all combinations of receiver rings by estimating eigenvalues at receiver ring index m from application of estimated propagators to eigenvalues at receiver ring index n. ### Claim 15 (depends on 7) The method of claim 7, wherein minimizing the objective function is accomplished analytically or by using a numerical search algorithm. ### Claim 16 (depends on 7) The method of claim 7, minimizing the objective function by estimating eigenvalue propagators from the eigenvalues, without minimizing the objective function over a set of auxiliary parameters. ### Claim 17 (depends on 8) The method of claim 8, wherein determining at least one anisotropy angle of the geological formation comprises: implementing the defining, the minimizing, and the determining for a data point space defined over multiple frequency bands having different starting frequencies or by multiple different time periods having different starting times. ### Claim 18 (depends on 17) The method of claim 17, further comprising: adding 90° to the anisotropy angle estimated for the one of the bands or time periods if its eigenvectors and associated ones of the eigenvalues have a different ordering than other ones of the bands or time periods across the bands or time periods. ### Claim 19 (depends on 13) The method of claim 13, wherein ordering the eigenvectors and corresponding ones of the eigenvalues comprises: switching the eigenvectors, the corresponding ones of the eigenvalues, and the propagators; and adding 90° to an anisotropy angle estimated for a frequency band at a first start frequency if a relative phase of the propagators has opposite sign when compared to a relative phase of the propagators at a second start frequency. ### Claim 20 (depends on 7) The method of claim 7, further comprising: removing global ambiguities of the axes is accomplished according to a sign of aligned relative phases. ### Claim 21 An article including a machine-accessible medium having instructions stored therein, wherein the instructions, when accessed, result in a machine estimating an azimuth angle by performing: recording a plurality of acoustic waveforms corresponding to acoustic waves received at azimuthally orthogonal dipole receiver arrays surrounded by a geological formation, the waves being generated by azimuthally orthogonal transmitter arrays, the azimuth angle corresponding to an orientation of the receiver arrays and the transmitter arrays relative to fast and slow principal flexural wave axes, wherein fast and slow principal flexural waves propagating along the axes and characterized by the waveforms being estimated as the ordered eigenvalues of a waveform matrix diagonalized by a unitary similarity transformation; defining an objective function dependent on the waveforms, the ordered eigenvalues, the azimuth angle, and a set of auxiliary parameters; minimizing the objective function with respect to the azimuth angle; and determining at least one anisotropy angle of the geological formation based on the global minimum. ### Claim 22 (depends on 21) The article of claim 21, further comprising: displaying the global minimum in conjunction with the at least one anisotropy angle. ### Claim 23 (depends on 21) The article of claim 21, further comprising: displaying an indication of stress induced anisotropy when an estimated version of the azimuth angle exhibits approximately a 90° jump as a function of start frequency, and dispersion curves for fast and slow principal flexural waves propagating along the axes, wherein the dispersion curves are created from the estimated version of the azimuth angle and the waveforms at each one of the start frequencies. ### Claim 24 (depends on 21) The article of claim 21, wherein the instructions, when accessed, result in the machine performing: detecting and characterizing formation fractures and a formation ambient stress field, based on the at least one anisotropy angle and an absolute orientation of a downhole tool carrying the transmitter arrays and the receiver arrays.