Real-Time Correction of Calibration Constants of a Bore-Hole Logging Tool Using a Reference Detector

Abstract

An x-ray based litho-density tool for measurement of formation surrounding a borehole is provided, the tool including at least an internal length comprising a sonde section, wherein said sonde section further comprises an x-ray source; at least one radiation measuring detector; at least one source monitoring detector; a plurality of sonde-dependent electronics; and a reference detector, wherein the reference detector is used to monitor the output of the x-ray source such that the reference detector's output effects corrections to the outputs of the detectors used to measure the density of the materials surrounding the borehole in order to correct for variations in the x-ray source output. Tool logic electronics, PSUs, and one or more detectors used to measure borehole standoff such that other detector responses maybe compensated for tool standoff are also provided. Shielding, through-wiring; wear-pads that improve the efficacy and tool functionality are also described and claimed.

Claims

1. An x-ray based litho-density tool for measurement of formation surrounding a borehole. said tool comprising: an internal length comprising a sonde section, wherein said sonde section further comprises an x-ray source; at least one radiation measuring detector; at least one source monitoring detector; a plurality of sonde-dependent electronics; and a reference detector, wherein said reference detector is used to monitor the output of the x-ray source such that the reference detector's output effects corrections to the outputs of the detectors used to measure the density of the materials surrounding the borehole in order to correct for variations in the x-ray source output.

2. The tool of claim 1, further comprising a plurality of tool logic electronics and PSUs.

3. The tool of claim 1, further comprising a detector used to measure borehole standoff such that other detector responses may be compensated for tool standoff.

4. The tool of claim 1, further comprising a plurality of density measuring detectors.

5. The tool of claim 1, further comprising a tungsten shield.

6. The tool of claim 1, wherein the tool is configured so as to permit through wiring.

7. The tool of claim 1, wherein the tool further comprises a wear-pad disposed such that the source and detector assembly may be pressed against the side of the borehole to reduce borehole effects.

8. The tool of claim 1, wherein the reference detector is used to monitor the output of the x-ray source.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0011] FIG. 1 illustrates an x-ray based litho-density formation evaluation tool deployed by wireline conveyance into a borehole, wherein the formation density is measured by the tool.

[0012] FIG. 2 is a layout view of a practical means of exercising the method within the confines of a borehole tool configured to measure formation density and borehole corrections using an x-ray tube as a radiation source.

[0013] FIG. 3 illustrates a typical reference detector spectrum for a Compton range source, showing Intensity in the y-axis versus photon energy in the x-axis, the windowed region of interest (the region between two specified energies) remains unchanged as the spectrum peak intensity moves.

BRIEF DESCRIPTION OF SEVERAL EXAMPLE EMBODIMENTS

[0014] The invention described herein consists of methods and apparatus to use the detected output of a non-isotope-based radiation source tube within a borehole logging tool to determine the correct calibration constant corrections to be substituted during the computation of detector count-rate output prior to, or during, the computation of formation density itself In borehole formation density logging, it is important to ensure the highest accuracy of data, whereby any variation in that data is a result of the change in scattering and attenuation properties of the formation itself (formation density) or controllable borehole effects. When using electronic radiation emitting source tubes as a replacement for radio-active isotope-based radiation sources, an inherent variability is introduced into the measurement due to the unstable nature of the output of the source tube and its power supply—an issue which is not encountered during the use of highly stable long half-life radio isotopes. Consequently, the variations in the measured data that would normally be attributable to formation density alone can contain a variable component of the instability of the source tube itself This invention teaches of a method and a means to measure the output radiation of a source tube and to use this data as an input to a calibration correction algorithm prior to or during density computation.

[0015] An example method of practicing the invention comprises a combination of known and new technologies embodied in a new application with respect to radiation physics and formation evaluation measurements for use within the oil and gas industry. The method is further embodied by a means, which may be used to practice the method for use in a water, oil or gas well,

[0016] The typical regulatory limit for the amount of .sup.137Cs which may be used during a logging operation is a maximum of 1.3 Curie. During density logging operations, a certain number of photons per second are required to enter into the detectors to ensure a high enough statistic for the purposes of data quality consistency and interpretation.

[0017] The operations cannot currently be performed using any radiation source other than harmful radioisotopes as the output of an x-ray tube isn't inherently stable enough over time to provide the statistics necessary for the accuracy required of the log, which is typically an uncertainty in measurement of 0.01 g/cc density.

[0018] By using a reference detector to correct the measured formation density. rather than using a reference detector to attempt to control the variations in the source, the use of x-ray tubes for formation evaluation becomes a real possibility.

[0019] With reference now to the attached Figures, FIG. 1 illustrates an x-ray based litho-density formation evaluation tool [101] is deployed by wireline conveyance [102,103] into a borehole [104], wherein the formation [105] density is measured by the tool [101].

[0020] FIG. 2 is a layout of a practical means of exercising the method within the confines of a borehole tool configured to measure formation density and borehole corrections using an x-ray tube [206] as a radiation [204] source. The x-ray source [206] produces a beam of x-rays [204] that illuminates the formation [202]. The x-ray source output is monitored by a reference detector

[0021] No direct beam path through the shielding [201] that surrounds the source [206] and detectors [207, 208, 211] is necessary as the reference detector [211] uses the shielding [201] to attenuate the radiation emanating directly from the source [206]. The source tube [206] may be energized by a high-voltage generator [205] that, contains a sensing and feedback circuit [209] that provides control input to the high-voltage generator controller [210]. The reference detector [211] provides a spectrum to the density processing unit [203] such that adjustments to the outputs of the formation density detector [208] and borehole correction detector [207] may be made to account for any variations in the output of the x-ray source [206].

[0022] FIG. 3 illustrates a typical reference detector spectrum [305] for a Compton range source, showing Intensity in the y-axis [301] versus photon energy in the x-axis [302], the windowed region of interest [303] (the region between two specified energies) remains unchanged as the spectrum peak intensity [304] moves. The total number of counts within the region of interest form to basis for the calibration coefficient correction computation.

[0023] In one example embodiment, the x-ray based litho-density formation evaluation tool

[0024] is deployed by wireline conveyance [102,103] into a borehole [104], wherein the formation

[0025] density is measured by the tool [101]. The tool [101] is enclosed by a pressure housing [201] which ensures that well fluids are maintained outside of the housing. In a further embodiment, a tool [101] is configured to measure formation density and borehole corrections using an x-ray tube

[0026] as a radiation [204] source. The x-ray source [206] produces a beam of x-rays [204] that illuminates the formation [202]. The x-ray source output is monitored by a reference detector

[0027] . No direct beam path through the shielding [201] that surrounds the source [206] and detectors [207, 208, 211] is necessary as the reference detector [211] uses the shielding [201] to attenuate the radiation emanating directly from the source [206]. The source tube [206] may be energized by a high-voltage generator [205] that contains a sensing and feedback circuit [209] that provides control input to the high-voltage generator controller [210]. The reference detector [211] provides a spectrum to the density processing unit [203] such that adjustments to the outputs of the formation density detector [208] and borehole correction detector [207] may be made to account for any variations in the output of the x-ray source [206]. In a further embodiment, the reference detector [211] is made of a scintillator crystal, such as Sodium Iodide, Cesium Iodide or Lanthanum Bromide, with an embedded micro-isotope, to be used in detector gain stabilization, and is located in the radiation shielding [201] surrounding a source tube [206] . The output spectrum [305] is analyzed and a region of interest [303] applied to the spectrum [305]. The total number of counts within the region of interest [303] form the basis of an input to a calibration coefficient correction computation. In a further embodiment, the borehole logging tool [101] would function such that the source tube [206] illuminates a volume of formation [202], wherein the formation-facing detectors [207,208], which are also gain stabilized by an embedded micro-isotope technique, would record the resultant spectra by collecting the scattered photons emanating from the formation. The number of counts logged by the formation-facing detectors [207,208] would be modified, either as a computational step prior to, or during the computation of formation density based on the reference detector's [211] output. This would be achieved by comparing the reference detector's [211] output variance to a software table for the specific ambient temperature in which the tool [101] is operating. The table would be created during the initial factory-based characterization testing of the tool [101], wherein the tool [101] would be placed against volumes of materials of known density, such as magnesium and aluminum, which contain a detector placed within the volume of the known density block, within the illumination volume of the source tube. The tool would be operated during these characterization tests and the count rate from within the region of interest [303] of the reference detector [211] and the calibration block detector would be recorded as the temperature of the tool is increased in discrete steps up to the highest anticipated wellbore temperature. The variation between the absolute detector located in the calibration blocks and the reference detector [211] as a function of ambient temperature would then be tabulated and included in the firmware for that specific tool [101]. This table of calibration coefficients can then be used during density computation to correct the formation-facing detectors' [207,208], output for any variations in the source-tube's [206] output as a function of temperature based upon the known ‘absolute’ source output relative to the tabled, reference output. In a further embodiment, the density processing is performed within the tool [101]. In a further embodiment, the raw count data from the region of interest [303] of the gain-stabilized formation-facing detectors [207,208] would be sent to topside in addition to the computed calibration coefficient corrected count rate for each detector, along with the count rate data from the reference detector. The correction computation would be performed within the logging control unit located on topsides.

[0028] In a further embodiment, the resultant data can be utilized to form a log stability quality index parameter during the final production of the density log versus borehole depth.

[0029] In a still further embodiment, the tool [101] is located within a logging-while-drilling (LWD) string, rather than conveyed by wireline.

[0030] In a further embodiment still, the LWD provisioned tool [101] would be powered by mud turbines.

[0031] In yet another embodiment, the tool [101] is combinable with other measurement tools such as neutron-porosity, natural gamma and/or array induction tools.

[0032] Additionally, the invention allows for the inherent physical differences between all manufactured photo-multiplier tubes and the stabilization gain control voltages necessary to produce identical spectral outputs—as the output of the reference detector sub-system and radiation source and power supply are all functionally characterized as a whole system, rather than individual parts, the statistical output of the formation-facing detectors can be modified against a system-specific temperature dependent calibration table to ensure that all manufactured systems have identical statistical output.

[0033] Furthermore, the inherent stability of the traditional embedded micro-isotope technique for formation-facing detector gain stabilization is not affected by this measurement. As a result, the raw output count data would be logged/recorded un-altered. The tabled coefficient amendments to the data would only be applied to the data prior to or during the final density calculation—if any apparent discrepancy or out-of-bound data were to be produced by the reference detector, it can be filtered by the operator as the raw unaltered' detector data would be available.

[0034] Moreover, the invention does not require the complexities of a channel between the source tube and the reference detector to permit, the passage of radiation. The reference detector can be located within a void within the radiation shielding material surrounding the source tube such that the distance between the source tube and the reference detector is such that there is enough radiation to produce a reasonable statistical count rate but is attenuated enough to ensure that the reference detector does not saturate from too many incoming photons.

[0035] Also, the invention does not require the monitoring of energy peaks, other than what is inherent to the traditional embedded micro-isotope technique for formation-facing detector gain stabilization in the detector electronics. As a result, the necessity for beam-hardening or spectrum modifying filters is avoided.

[0036] Additionally, as a region of interest is employed while analyzing the output spectrum of reference detector, any undesirable effects associated with the modification of the form of the beam spectrum due to the radiation shielding can be circumvented as the region of interest can be tuned to select a spectral region above that of any major spectrum-clipping or hardening materials within the shielding.

[0037] The foregoing specification is provided only for illustrative purposes, and is not intended to describe all possible aspects of the present invention. While the invention has herein been shown and described in detail with respect to several exemplary embodiments, those of ordinary skill in the art will appreciate that minor changes to the description, and various other modifications, omissions and additions may also be made without departing from the spirit or scope thereof.