Method and device for detection of em waves in a well

Electricity: measuring and testing – Of geophysical surface or subsurface in situ – With radiant energy or nonconductive-type transmitter

Reexamination Certificate

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C324S333000, C166S250010, C175S040000

Reexamination Certificate

active

06525540

ABSTRACT:

FIELD OF INVENTION
This invention relates to a method for using a radar-like device in production wells to detect the oil/water contact in a reservoir rock.
More specifically the invention comprises a method for using a transmitter antenna for electromagnetic waves which is fixedly arranged near a production tubing inside a geological formation, and receiver antennas which also are fixedly arranged near the production tubing, preferably by cement fixation in the well. This method and the application of the radar-like device may enable the user to detect reflectors constituted by electrically conducting surfaces inside the reservoir. Such a surface of particular importance is the oil/water contact, with the water front in most instances constituting a relatively sharp transition between oil filled sand with high resistivity, to water filled sand with low resistivity thereby constituting a reflector.
BACKGROUND OF THE INVENTION
Borehole logging tools utilizing the radar principle is known from U.S. Pat. Nos. 4,670,717, 4,814,768, 4,297,699, 4,430,653 and GB 2 030 414. Some of these patent use methods where it is necessary to estimate a wave propagation speed in order to be able to interpret the radar signals.
Schlumberger's U.S. Pat. No. 5,530,359, “Borehole logging tools and methods using reflected electromagnetic signals”, describe a logging tool with pulsed radar signals being transmitted from a transmitter antenna in a separate vertical section. The logging tool is freely hanging in the borehole in a cable or in a coiled tubing. Linear antenna elements are applied, being arranged parallelly with the long axis z of the tool. Electromagnetic pulses are emitted with a center frequency of 40 MHz and a highest frequency component of 120 MHz. This pulse is emitted in all directions into the formation and reflected from structures in the formation back to the tool in the borehole. The transit time of the pulse out to the structure and back to the tool is used for determining the distance between the reflecting structure and the borehole. Directional information is obtained by the fact that receiver antennas are arranged around the entire circumference of the tool, so that one may find the direction to the reflecting structure by making differences between the reflected signals. These differences may be calculated by means of electronic circuits, or subtraction may be performed by directly differentially coupled receiver antennas. One method to calculate the reflected signals' direction is given. A disadvantage of Schlumberger's U.S. Pat. No. 5,530,359 is that the instrument applies pulsed electromagnetic waves. This entails a spread of the frequency components already in the emitted signal, and thus the emitted signal pulse exhibits a continuously varying group velocity. The reflected signal becomes smeared out and one gets an unclear image of the reflecting structures. Near reflecting structures will also dominate over more remote reflecting structures, so that the more remote structures barely can be detected if the nearer rocks have relatively high conductivity/low resistivity. Another disadvantage of Schlumberger's instrument is that it is not fixedly arranged by the geological formation, so that there is no provision for tracing changes in electrical parameters in the formation during a period of time, e.g. from one date to another. The instrument is also not arranged for being applied neither in production wells nor in injection wells.
Another apparatus is described in U.S. Pat. No. 5,552,786: “Method and apparatus for logging underground formations using radar”, (Schlumberger). U.S. Pat. No. 5,552,786 describes a logging tool which partially solves the problem of the electromagnetic wave propagation speed in the formations which are to be logged. The apparatus emits an electromagnetic pulse in close contact with the borehole wall, into the formation and receives the direct wave in a predetermined distance along the drillstring from the transmitter. Thereby the wave propagation speed for the “direct wave” through the rocks (which may be invaded by drilling mud), and the reflectors separations from the emitter/receiver system may be calculated more exactly than if one had only an estimate of the wave propagation speed.
U.S. Pat. No. 4,504,833 “synthetic pulse radar system and method” concerns a synthetically pulsed radar which generates several signals of different frequencies simultaneously. The response from the subsurface to these different frequencies simulates parts of the Fourier spectrum which would have been measured if one emitted a very short pulse which according to the mathematical background would have been very broad in the frequency spectrum. However, the system is arranged to be used onboard a vehicle, among other things, because according to its claim 1, it shall be able to generate all the component signals simultaneously.
U.S. Pat. No. 4,275,787 “Method for monitoring subsurface combustion and gasification processes in coal seams” describes a radar for detecting a combustion front in a geological formation, e.g. a coal bearing formation. Due to the resistivity generally increasing with the temperature, such a combustion front will provide high resistivity and constitute a very large contrast in relation to the coal bearing formation which normally will show low resistivity.
The attenuation exceeds loo dB/wavelength in the combustion front, and the attenuation of “Pittsburgh coal” is 1 dB/wavelength, for “British coal” the attenuation is 3 dB/wavelength. The applicant (of U.S. Pat. No. 4,275,787) mentions that a detection range for the combustion front is 100 m, an unrealistically long distance when one takes into consideration the conditions in an oil well where the attenuation of the signal is much higher and where it is a very difficult task to detect reflecting surfaces only one to two metres out in the reservoir. A swept signal is emitted and which varies continuously between a lowest and a highest frequency. Because the combustion front is moving, one may by subtraction of the received signals be able to see a change in the difference signal between the observations. However the patent does not take into consideration the need for tuning of the transmitter antennas when the transmitter antennas are lying very close (e.g. within a few millimeters) to a metallic pipe surface (e.g. liner pipe or completion pipe) and the frequency of the emitted signal is changed.
The methods and tools in the known art do not solve the problems arising in the context of petroleum production on the Troll oilfield in the North Sea as described herein, data from the Troll oil field indicate that the resistivities in the actual geological formations are relatively lower with respect to the conditions described in the known art, and therefore it is impractical to perform detection by means of electromagnetic waves by means of the known art.
BRIEF SUMMARY OF THE INVENTION
A preferred embodiment of the present invention comprises a method for detecting electrical properties in a geological formation via a well which has within it a tubing string, comprising the steps of mounting a transmitter antenna outside the tubing string in the well in a fixed position with respect to the geological formation, mounting a receiving antenna outside the tubing string in a fixed position with respect to the geological formation, generating a first series of electrical signals to cause the transmitter antenna to emit a first series of electromagnetic waves at a first time, receiving a first series of reflected electromagnetic waves in the receiving antenna, transforming the first series of reflective electromagnetic waves into a first registration, generating a second series of electrical signals to cause the transmitter antenna to emit a second series of electromagnetic waves, receiving a second series of reflective electromagnetic waves in the receiver antenna, transforming the second series of reflective electromagnetic waves into a second registration. An alternative to th

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