IP Library Granted Patent US 8,612,156
Granted Patent B2
US 8,612,156 · App. 13/042,454 · Granted Dec 17, 2013

Active noise injection computations for improved predictability in oil and gas reservoir discovery and characterization

Inventor: Sandeep Gulati (La Canada Flintridge, CA)
Assignee: ViaLogy LLC
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Quick Facts
Patent No.
US 8,612,156
App. No.
13/042,454
Granted
Dec 17, 2013
Kind
B2
Abstract

Application of nonlinear resonance interferometry is introduced as a new geophysical approach to improve predictability in characterization of subsurface porosity, rock and fluid properties. In contrast to reflection methods that remove random information noise, nonlinear resonance interferometry exploits the full seismic acquisition spectrum to assess how low frequency and high-frequency noise is differentially and directly modulated by varying levels of porosity and hydrocarbon content in the lithologies of interest. In some examples, systems and techniques implement novel computational interactions between acquired seismic wavefield attributes and a nonlinear system in software to amplify distortions in seismic noise and exploits injection of synthetic noise, in software format, to detect hydrocarbon traps and lithology changes at spatial scales below seismic resolution, thereby increasing the information value of low-resolution data. The techniques are broadly applicable to de-risking conventional clastic and carbonate reservoirs and non-conventional shale gas resource prospects.

Claims (19)

1. A computer-implemented method comprising:

obtaining a one-dimensional voxel vector for a voxel from multiple voxels associated with a formation of interest;

obtaining spectral data generated from well-log data associated with an attribute of interest;

coupling the spectral data with the one dimensional voxel vector to determine whether a resonance event occurs;

when a resonance event occurs, producing an output indicating that the voxel has the attribute of interest; and

when the resonance event does not occur, producing an output indicating that the voxel does not have the attribute of interest.

2. The method of claim 1 ,

wherein the obtaining the one-dimensional voxel vector comprises normalizing amplitudes corresponding to the one dimensional voxel vector to fit within a range.

3. The method of claim 1 , wherein obtaining the spectral data generated from well-log data comprises:

obtaining seismic noise data;

obtaining well control voxel data from the well log data; and

combining the seismic noise data and the well control voxel data using a quantum mechanical model to produce the spectral data.

4. The method of claim 3 , wherein obtaining well control voxel data comprises:

determining an energy spectral density voxel from the well-log data for the attribute using wavelets derived from sonic logs in sections of a well with the attribute of interest.

5. The method of claim 3 wherein combining the seismic noise data and the well control data comprises combining the seismic noise data and with well control voxel data for a voxel associated with the well-log data that exhibits the attribute.

6. The method of claim 3 , wherein

obtaining the well control voxel data comprises obtaining a well control voxel data of a voxel not exhibiting the attribute; and

wherein obtaining the seismic noise data comprises generating the seismic noise data based on the well control voxel data of the voxel not exhibiting the noise.

7. The method of claim 1 , wherein coupling the spectral data with the one dimensional voxel vector to determine whether a resonance event occurs comprises using a nuclear magnetic resonance (“NMR”) master rate equation to generate quantum stochastic resonance based on the one-dimensional voxel vector, synthetic noise, and the spectral data.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 6, 2012
From: GULATI, SANDEEP
To: VIALOGY LLC
Reel/Frame 028734/0360 →
Continuity (2)
Provisional Application 61311227 · Mar 5, 2010
Related Publication 20110218737A1 · Sep 8, 2011