Patent Application
20120182017
Not applicable.
Not applicable.
The invention relates generally to the field of marine electromagnetic geophysical surveying. More specifically, at least in some embodiments, the invention relates to electromagnetic survey techniques that take account of electrical inhomogeneity in a body of water in which a survey is conducted.
Marine electromagnetic geophysical surveying is used to infer spatial distribution of electrical conductivity of rock formations below the bottom of a body of water such as a lake or ocean. The spatial distribution of conductivity is used to assist determining the presence of hydrocarbon bearing rock formations in the subsurface, potentially resulting in cost savings by better targeting drilling operations. One type of such surveying is known as “controlled source” electromagnetic surveying (“CSEM”), which generally includes inducing a time varying electromagnetic field in the subsurface formations and measuring one or more parameters related to a response of the subsurface rock formations to the induced electromagnetic field.
Devices for inducing such electromagnetic fields are generally referred to as “sources” or “transmitters” and may include, among other devices, spaced apart electrodes or wire coils disposed along or at the end of a cable. The cable may be towed by a vessel in the body of water. Time varying electric current is imparted across the electrodes or through the coils, generally from a power source located on the vessel, to induce a time varying electromagnetic field in the water and subsequently in the subsurface formations
Response of the subsurface formations is inferred by measuring properties of electromagnetic fields induced in the water as a result of the imparted electromagnetic fields. Such properties may include voltage, magnetic field amplitude, magnetic field gradient, and/or combinations of the foregoing at varying distances (offsets) from the electromagnetic transmitter.
The spatial distribution of electrical conductivity of the formations may be inferred by a technique called “inversion”, in which an initial estimate of the spatial distribution is made, a simulated response of the survey apparatus to such initial estimate is calculated, and differences between the measured response of the survey apparatus and the simulated response are analyzed. The initial estimate is adjusted based on the analysis, and the process is repeated. The foregoing steps may be iteratively repeated until differences between the simulated response and the measured response are minimized.
Inversion techniques known in the art rely on assumptions about the conductivity distribution in the body of water above the subsurface formations being surveyed, e.g., that the conductivity distribution is homogeneous and isotropic. It is desirable to have a technique that improves the accuracy of the inversion technique by improving the accuracy of assumptions of conductivity distribution in the body of water.
A method according to one aspect of the invention for modeling conductivity distribution in a formation below a bottom of a body of water includes measuring electromagnetic response of the formation with an electromagnetic survey system. The method further includes measuring at least one of water conductivity, water dielectric constant, and water temperature with respect to depth in the body of water. The method further includes generating an initial model of conductivity distribution of the formation. The method further includes discretizing the measurements of at least one of water conductivity, water dielectric constant, and water temperature with respect to depth into at least one layer. The method further includes generating a forward model of a response of the electromagnetic survey system to the initial model and the discretized measurements. The method further includes comparing the forward model to the measured electromagnetic response to determine differences. The method further includes adjusting the initial model to reduce the differences. The method further includes repeating generating a forward model, comparing the forward model to the measured electromagnetic response, and adjusting the initial model until the differences fall below a selected threshold, thereby determining a final model of conductivity distribution in the formation.
A method according to another aspect of the invention for modeling conductivity distribution in a formation below a bottom of a body of water includes measuring electromagnetic response of the formation with an electromagnetic survey system by inducing a time varying electromagnetic field in the body of water and measuring at least one electromagnetic field property in the body of water. The method further includes measuring at least one of water conductivity, water dielectric constant, and water temperature with respect to depth by deploying at least one expendable probe from a vessel proximate a location of the measuring electromagnetic response. The method further includes generating an initial model of conductivity distribution of the formation. The method further includes discretizing the measurements of at least one of water conductivity, water dielectric constant, and water temperature with respect to depth into at least one layer. The method further includes generating a forward model of a response of the electromagnetic survey system to the initial model and the discretized measurements. The method further includes comparing the forward model to the measured electromagnetic response to determine differences. The method further includes adjusting the initial model to reduce the differences. The method further includes repeating generating a forward model, comparing the forward model to the measured electromagnetic response, and adjusting the initial model until the differences fall below a selected threshold, thereby determining a final model of conductivity distribution in the formation.
A method according to another aspect of the invention of data processing includes providing measurements from an electromagnetic survey system of electromagnetic response of a formation below a bottom of a body of water. The method further includes providing measurements of at least one of water conductivity, water dielectric constant, and water temperature with respect to depth in the body of water. The method further includes generating an initial model of conductivity distribution of the formation. The method further includes discretizing the provided measurements of at least one of water conductivity, water dielectric constant, and water temperature with respect to depth into at least one layer. The method further includes generating a forward model of a response of the electromagnetic survey system to the initial model and the discretized measurements. The method further includes comparing the forward model to the provided measured electromagnetic response to determine differences. The method further includes adjusting the initial model to reduce the differences. The method further includes repeating generating a forward model, comparing the forward model to the provided measured electromagnetic response, and adjusting the initial model until the differences fall below a selected threshold.
Other aspects and advantages of the invention will be apparent from the following description and the appended claims.
An example embodiment of a marine electromagnetic survey system is shown schematically in
The survey vessel 18 may include thereon equipment, shown generally at 20 and referred to for convenience as a “recording system,” that may include devices (none shown separately) for navigation, energizing electrodes, coils, or other types of transmitters for inducing an electromagnetic field in the formations below the water bottom 23, and for recording and processing signals generated by the various sensors 12 on the sensor cable 10. The electromagnetic survey system shown in
The electromagnetic transmitter 17 as configured in
In the illustrated embodiment, one or more expendable conductivity, temperature, and depth (“xCTD”) probes 24 may be deployed from the survey vessel 18 during survey operations while the survey vessel 18 is moving. Each xCTD probe 24 includes sensors (not shown separately) for measuring electrical conductivity, temperature, and depth of the water 22. Each xCTD probe 24 is typically deployed by releasing the xCTD probe 24 over the side or stern of the survey vessel 18 at the end of a probe cable 25. Measurements made by the one or more xCTD probes 24 may be communicated over the associated probe cable 25 to the recording system 20. Alternatively, one or more of the xCTD probes may be deployed without associated probe cable 25 to measure and record electrical conductivity, temperature, and depth for later retrieval and uploading of data. Electrical conductivity and temperature measurements may be correlated to depth in the water by depth estimation based on a known rate of descent of the xCTD probe 24 and the elapsed time from the initial release of the xCTD probe 24. Alternatively, depth may be inferred by an included pressure sensor (not shown) on the xCTD probe 24. A non-limiting example of such an xCTD probe is made by The Tsurumi-Seiki Co., Ltd., 2-20, 2-Chome, Tsurumi-Ku, Yokohama, 230-0051, Japan and sold under model designation “XCTD-3.” Another example of such an xCTD probe is sold under product designation “Digital XCTD” by Lockheed Martin Maritime Systems & Sensors, Seven Barnabas Road Marion, Mass. 02738.
Signals detected by the sensors 12 may be recorded in the recording system 20 and later entered into a data processing technique known in the art as “inversion” in order to estimate distribution of electrical conductivity of the rock formations 26 below the water bottom. The detected signals may also be entered into such procedure as they are acquired. One such inversion technique is described, for example, in International Patent Application Publication No. WO 2003/023452. Typically, electromagnetic survey signal inversion techniques include generating an initial model of conductivity distribution in the subsurface formation, generating a simulated electromagnetic survey system response (often called a “forward model”), and comparing the forward model of the survey system response to the electromagnetic survey system response actually measured (“measured system response”). If the comparison indicates excessive difference between the forward model and the measured system response, one or more parameters of the initial model may be altered, perturbed, or adjusted, and the forward modeling and comparing repeated. Such procedure may be iteratively repeated with the one or more parameters being altered, perturbed, or adjusted until the differences between the forward model and the measured system response reach a minimum, or at least fall below a selected threshold. At such time, the adjusted forward model is considered to most closely represent the conductivity distribution in the subsurface formation. Parameters that may be adjusted include, for example and without limitation, the number of formation layers, thicknesses of each of the formation layers, and electrical conductivity and lateral extent of the formation layers.
Techniques known in the art for inversion of marine electromagnetic survey data include using certain assumptions about the electrical properties of the body of water. In such techniques, an electrical conductivity of a sample of the water may be measured at a known temperature or a measured temperature. The conductivity of the water is then estimated from the water surface to the water bottom using a predetermined temperature profile of the particular body of water in the geodetic location of the survey being conducted. Some techniques may estimate dielectric constant of the water using the predetermined temperature profile. The actual electrical properties of the water, e.g., conductivity and dielectric constant, may differ from those estimated using the foregoing techniques because of localized variations in water temperature and salinity with respect to depth.
In an example embodiment of a method according to the invention, data from the xCTD probe 24 are measured as the survey vessel 18 moves along each of a plurality of survey “lines.” Such survey lines may include the lines along which either or both the electromagnetic transmitter 17 and sensors 12 move through the body of water, or just the lines along which the electromagnetic transmitter 17 moves when ocean bottom deployed sensors are used, e.g., ocean bottom cables or nodes.
The xCTD probe 24 data may be used to construct a profile with respect to water depth of the electrical properties (conductivity and/or dielectric constant) and temperature. For example, the profile may comprise data points along each survey line. The profile may be used as input to the inversion technique. Such input may take the form, for example, of discretizing the probe data into one or more “layers” in the body of water 22 from the surface to the water bottom. Each such layer may have a unique thickness, electrical conductivity, dielectric constant, and/or temperature. The number of such layers into which the water is discretized may depend on, for example, the amount of change in conductivity, dielectric constant, and/or temperature of the water 22 from the surface to the water bottom. In some embodiments, only the temperature measurements may be used; the conductivity may be inferred from the temperature measurements. In some embodiments, only the conductivity measurements may be used. In some embodiments, the thickness of one or more water layer may vary along the survey line.
After the water 22 is discretized into one or more individual layers having unique thickness, conductivity, dielectric constant, and/or temperature, the discretized water layers may be entered as part of an initial model of the conductivity structure of both the subsurface formations 26 and the water 22. Then an inversion technique as described above may be performed. In such inversion technique, however, the properties of the layer(s) in the body of water 22 may remain unchanged in each iteration of the inversion, because their values have been substantially determined by the measurements from the xCTD probe 24. The remainder of the inversion technique, however, may be performed as it would be ordinarily performed with respect to layers in the rock formations 26 below the water bottom 23.
An example embodiment of an inversion technique according to certain embodiments of the invention may be better understood with reference to the flow chart in
Methods according to the invention may provide more accurate results in determining conductivity distribution of formations below the bottom of a body of water by more accurately characterizing the effects of the body of water on electromagnetic measurements made therein. The more accurate conductivity distribution may be used to assist determining the presence of hydrocarbon bearing rock formations in the subsurface, potentially resulting in cost savings by better targeting drilling operations. These methods might be especially advantageous for shallow water electromagnetic geophysical surveys.
While the invention has been described with respect to a limited number of embodiments, those skilled in the art, having benefit of this disclosure, will appreciate that other embodiments can be devised which do not depart from the scope of the invention as disclosed herein. Accordingly, the scope of the invention should be limited only by the attached claims.
