Pulsar Multifunction spectroscopy service Introducing environment-independent, stand-alone cased hole formation evaluation and saturation monitoring
1 APPLICATIONS FEATURES AND BENEFITS ■■ Stand-alone formation evaluation for diagnosis of bypassed ■■ Environment-independent reservoir saturation monitoring ■■ High-performance pulsed neutron generator (PNG) hydrocarbons, depleted reservoirs, and gas zones in any formation water salinity ●● Optimized pulsing scheme with multiple square and short ●● Differentiation of gas-filled porosity from very low porosity ●● Production fluid profile determination for any well pulses for clean separation in measuring both inelastic and formations by using neutron porosity and fast neutron cross inclination: horizontal, deviated, and vertical capture gamma rays 8 section (FNXS) measurements ●● Detection of water entry and flow behind casing ●● High neutron output of 3.5 × 10 neutron/s for greater ■■ measurement precision Petrophysical evaluation with greater accuracy by accounting ●● Gravel-pack quality determination by using for grain density and mineral properties in neutron porosity elemental spectroscopy ■■ State-of-the-art detectors
■■ Total organic carbon (TOC) quantified as the difference ■■ Metals for mining exploration ●● Near and far detectors: cerium-doped lanthanum bromide between the measured total carbon and inorganic carbon ■■ High-resolution determination of reservoir quality (RQ) (LaBr3:Ce) ■■ Oil volume from TOC and completion quality (CQ) for formation evaluation ●● Deep detector: yttrium aluminum perovskite (YAP)
■■ Hydrocarbon identification in low-resistivity pay of unconventional reservoirs and complex lithologies ●● Compact neutron monitor (CNM), photomultiplier, ■■ Identification of oil zones in freshwater and mixed- on the basis of detailed quantitative mineralogy and counting electronics
●● or unknown-salinity reservoirs Rigless service deployment ●● Excellent spectral energy resolution at high operating ●● Formation evaluation in old wells where modern openhole temperatures (175 degC [350 degF]) logs have not been run ●● Highest count rate capability in the industry
■■ High-fidelity mineralogy and lithology for geochemistry, ●● Elimination of stabilization sources stratigraphy, and rock typing ●● Calibrated measurement of elemental concentrations for Al, Ca, ■■ Carbonates: Ca, Mg, Fe, Mn, and S to differentiate Fe, Gd, K, S, Si, Ti, Ba, Cl, H, Mg, Mn, Na, Br, O, and the metal and determine the volume of calcite, dolomite, anhydrite, Cu, with other elements on request and other carbonate minerals ■■ In situ TOC measurement ■■ Siliciclastic rocks: Si, Al, Fe, K, Ca, and Mg as the primary ■■ Borehole fluid- and completion-compensated sigma and elements to resolve quartz, feldspar, mica, and clay minerals thermal neutron porosity (TPHI) measurements ■■ More than 20 measured elemental concentrations routinely ■■ Simultaneous acquisition of time and energy domain data available to identify specific minerals, with additional elemental standards available on request ■■ Improved elemental precision delivering high-quality data even at faster logging speeds ●● Element logs for well-to-well correlation and sequence stratigraphy ■■ Extensive laboratory and modeling characterization to ensure accuracy in a wide range of environments ■■ Fully combinable hardware with the PS Platform* production services platform, SCMT* slim cement mapping tool, ThruBit* through-the bit logging services, and wireline tractor conveyance ■■ Corrosion-resistant housing qualified per the requirements of NACE MR0175
2 Formation Evaluation Pulsar* multifunction spectroscopy service introduces the industry’s first stand-alone cased hole formation evaluation and the new FNXS measurement for reliably differentiating gas-filled porosity from tight zones—all from a single tool.
Challenge: Telling apart intermixed low-porosity Pulsar service also provides the new fast neutron cross gas-filled zones and tight zones in a shaly sand section (FNXS) measurement that reliably differentiates A US land well was drilled with an 8¾-in bit size but gas-filled porosity from liquid-filled zones and tight formations. Case Study completed with 4½-in 11.6-lbm/ft casing. As a result Because the fast neutron inelastic scattering response used of the difference between the hole and casing diameters, to calculate FNXS is not dominated by particular elements, the completion has a relatively large cement volume, with which is the case for conventional neutron logging, the FNXS Differentiating Gas and a cement thickness greater than 2 in. The formation lithology measured values for rock matrix and water are in the same Tight Zones in a Shaly Sand is shaly sand, with alternating low-porosity gas-filled zones and range. This makes FNXS insensitive to variation in liquid-filled very low porosity zones. Although openhole logs had been run, porosity but highly sensitive to variation in gas-filled porosity. Despite Cement Thickness the operator was interested in obtaining an interpretation that Results: Differentiating and quantifying gas-filled would provide greater insight to the formation and its porosity from tight zones Greater Than 2 in fluid contents. Logging the shaly sand with a single run of Pulsar service Solution: Introducing a new measurement to identify revealed two zones of interest at X,160 to X,180 ft and and quantify gas-filled porosity X,270 to X,330 ft. Both the environmentally corrected FNXS New Pulsar multifunction spectroscopy service uniquely curve and the gas ratio curve it is calculated from (Tracks 7 provides operators with a stand-alone petrophysical volumetric and 6, respectively) show that only the lower zone contains gas— interpretation incorporating robust, high-fidelity quantified unlike the very low porosity upper zone that conventional cased mineralogy and lithology for cased holes. No openhole logging hole logging would have assumed was also gas bearing. data is necessary for complete formation evaluation from The stand-alone volumetric interpretation performed using a single run of this one tool. In addition to obtaining highly a linear solver with Pulsar service’s sigma, FNXS, and TPHI accurate elemental concentrations—including total organic measurements (Tracks 10 and 11) is validated by the previously carbon (TOC)—Pulsar service acquires the traditional cased obtained openhole logs (Tracks 8 and 9). hole sigma, porosity, and carbon/oxygen ratio measurements With this one-run, one-tool solution to logging cased wells, but at a higher resolution and significantly faster logging speed. the operator can streamline operations to a single log obtained in the more stable cased wells.
3 9.5 9.5
9 9 Dolomite porosity, % Dolomite porosity, % 0 10 0 10 8.5 20 30 8.5 20 30 40 50 40 50 8 Limestone porosity, % 8 Limestone porosity, % 40 50 40 50 0 10 20 30 0 10 20 30 7.5 0 Sandstone porosity, % 50 7.5 0 Sandstone porosity, % 50 40 40 20 30 20 30 7 0 10 7 0 10
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–1 0 –1 0 6.5 6.5 10 20 10 20 FNXS, m FNXS, m 6 6 20 30 20 30 5.5 5.5 30 40 30 40 5 5 40 40 50 50 4.5 4.5 50 50 Gas-filled porosity, % Gas-filled porosity, % 4 4
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–0.1 –0.05 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 0.55 0.6 0.65 0.7 –0.1 –0.05 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 0.55 0.6 0.65 0.7 The large annular volume of light cement had to be accounted for in TPHI, ft3/ft3 TPHI, ft3/ft3 quantifying the gas-filled porosity. In the left-hand crossplot of Pulsar
10 Sigma 30 10 Sigma 30 service’s FNXS and thermal neutron porosity (TPHI) measurements, FNXS has the standard wellbore correction applied. However, the cement used in developing the characterization database was heavier,
Eective Gas Saturation causing FNXS to clearly read too low compared with the expected Pulsar Fluid Density Pulsar Mineralogy Gas Gas Neutron-Density Water 0 g/cm3 3 4-ft Array Induction Crossover 0 V/V 1 value. An additional offset correction was applied for the effect of the Pulsar Borehole Sigma Openhole NPHI Near/Deep Capture Ratio Near/Deep Burst Count Ratio Resistivity AF90 Openhole Porosity (NPHI) Gas Depth, ft Gas Gas 0 cu 250 0.45 ft3/ft3 –0.15 3 23 9.5 30.5 0.02 ohm.m 2,000 0.45 ft3/ft3 –0.15 0.25 V/V 0 light cement, which adjusted the FNXS value close to the theoretical Pulsar Gamma Ray Pulsar Sigma Pulsar TPHI Near/Far Capture Ratio Near/Far Burst Count Ratio Gas Ratio FNXS 4-ft Array Induction Resistivity AF10 Bulk Density Bulk Density 3 3 –1 3 value for the very low porosity shaly zones. As shown in the right-hand 0 gAPI 150 0 cu 30 0.45 ft /ft –0.15 1 2.6 1.8 2.9 60 45 6 m 8 0.02 ohm.m 2,000 1.95 g/cm 2.95 0.25 V/V 0 Illite Bound Water Quartz Water Gas crossplot, the additional offset produced environmentally corrected FNXS values that are much more consistent with the sandstone envelope and thus are appropriate for use in a quantitative interpretation.
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Pulsar service’s FNXS measurement was environmentally corrected X,300 for the large volume of light cement in the annulus to differentiate the dry tight zone at X,160 to X,180 ft from the gas-filled porosity zone at X,270 to X,330 ft. A conventional cased hole pulsed neutron log, as approximated by the near/deep count ratio in Track 5, would read gas in the upper tight zone.
4 Reservoir Saturation Monitoring Pulsar service delivers environment-independent reservoir saturation monitoring in any formation water salinity and without requiring any openhole logging data input.
Challenge: Difficulties monitoring in fresh response is not dominated by any elements, the FNXS formation water values for rock matrix and water are in the same range, An operator producing a California heavy oil reservoir by which focuses the measurement’s sensitivity on variation Case Study steamflooding wanted to periodically run cased hole logs in gas or steam content. to track changes in the steam front and oil saturation. Prior to Results: Reliably tracking fluid movement being cased, the monitor well had been extensively cored and and saturations Accurately Tracking Steam logged to establish a baseline, which provided the usual open- Pulsar service was run in the monitor well to simultaneously hole logging data that conventional pulsed neutron logging Front and Heavy Oil acquire inelastic gas, sigma, hydrocarbon index, and dual in cased hole requires for determining saturations. However, inelastic and capture spectroscopy data. The TOC computed Saturation in a Freshwater the field’s very fresh formation water meant there would be from spectroscopy and the resulting determination of oil no contrast in a conventionally logged capture cross section saturation were confirmed by the openhole logging by Formation, California between oil and water in the reservoir. Because traditional Litho Scanner* high-definition spectroscopy service. As shown cased hole tools do not have this differentiation capability, in the second log track from the right, Pulsar service’s dry- the operator needed another approach to reliably track weight TOC (black) obtained at 50 ft/h compares favorably with the steamflooding. TOC similarly obtained by the larger-diameter Litho Scanner Solution: Monitoring saturations in cased hole with service (magenta) at 450 ft/h. The oil saturation computed from one tool in one run the cased hole TOC is a good match to the core-measured satura- Pulsar multifunction spectroscopy service overcomes the tion on the far-right track. limitations of conventional pulsed neutron logging tools by The initial openhole neutron density log shows steam- and integrating a high-performance pulsed neutron generator with air-filled sands above X,500 ft. Pulsar service’s sigma, TPHI, multiple advanced detectors in a single 1.72-in-diameter tool. The and FNXS logged in the well completed with 7-in 23-lbm/ft result is a complete petrophysical volumetric interpretation based casing all also show gas (steam or air) in the same interval. on highly accurate elemental concentrations—including carbon In this situation, where openhole porosity logs are available, as the basis for TOC—in addition to traditional sigma, porosity, they can be used to compute gas saturation in conjunction and carbon/oxygen ratio measurements. with any of these gas-responding measurements, usually with The new FNXS measurement introduced by Pulsar service the deeper-reading sigma or TPHI. differentiates gas-filled porosity from liquid-filled zones and tight formations. Because the fast neutron inelastic scattering 5 Pulsar Casing Collar Locator Neutron-Density Crossover Gas
Pulsar Borehole Sigma Openhole Porosity Openhole Porosity FNXS Pulsar Dry-Weight TOC Pulsar TOC-Based Oil Saturation 8.5 0.6 ft/ft 0 0.6 ft/ft 0 0.6 m–1 0 0 ft/ft 0.6 Pulsar Gamma Ray Depth, ft Openhole Bulk Density Pulsar Sigma Pulsar TPHI Gas Ratio Openhole Dry-Weight TOC Core Oil Saturation 1.65 g/cm 2.65 30 cu 5 0.6 ft/ft 0 0 ft/ft 0.6 8.0 Limestone water-filled porosity, % 40 50 0 10 20 30 7.5 Sandstone water-filled porosity, % 50 30 40 20 7.0 10 0 10
–1 6.5 20 10 Fluid-filled sands and siltstones FNXS, m 6.0 20 30 X,250
5.5 30 40 Air- and steam-filled sands 5.0 40 50 4.5 Gas-filled porosity, % 50 –0.05 0 0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40 0.45 0.50 0.55 0.60 TPHI, ft /ft3 10 Sigma 30
X,500 Crossplotting Pulsar service’s FNXS and TPHI responses differentiates gas-filled from fluid-filled zones.
However, if openhole logs are not available, the difference between the crossplotted FNXS and TPHI responses can be used to not only solve for the gas saturation but also the total porosity after gas correction. The overlay on the crossplot of FNXS and TPHI shows the expected response of various lithologies. The subhorizontal upper boundaries are where 100% water-filled porosity plots, and the subvertical boundaries to the left represent where 100% gas-filled porosity plots. The responses of TPHI and FNXS significantly differ because TPHI is a hydrogen-dominated measurement, whereas FNXS is not dominated by any element. X,750 Without the new FNXS measurement or openhole logs, solving both gas saturation and porosity from pulsed neutron logs is underdetermined. In openhole, an accurate formation porosity in gas-filled formations is usually computed from a combination of density and neutron porosities. In cased hole, FNXS plays a role similar to that of density because its response contrasts with the traditional neutron porosity–type response, which is dominated by hydrogen. As a result, the response for air- and steam-filled sands is in the gas region of In the second-from-right track, openhole logging of TOC (magenta curve) confirms Pulsar service’s spectroscopic determination of TOC for identifying oil saturation, which similarly matches the core-measured saturation (green points) the crossplot and the fluid-filled sands and siltstones plot along the 100% fluid line. in the far-right track. Both the open- and cased hole logs in Tracks 2–5 indicate gas-filled sands above X,500 ft.
6 Unconventional Reservoirs Pulsar service’s detailed quantitative mineralogy resolves the complex lithology of unconventional reservoirs for the high-resolution determination of reservoir quality (RQ) and completion quality (CQ).
Challenge: Streamlining resource-intensive In addition to traditional sigma, porosity, and carbon/oxygen openhole characterization ratio measurements, Pulsar service also provides the new FNXS To evaluate a complex shale gas reservoir in Pennsylvania, measurement that reliably differentiates gas-filled porosity from Case Study USA, an operator had run a full suite of openhole logs in the liquid-filled zones and tight formations. 8¾-in borehole, including triple-combo, nuclear magnetic Results: Flagging the transition from gas to low porosity resonance (NMR), and an advanced spectroscopy tool. The that conventional cased hole logging would overlook Replacing an Entire Openhole high-definition spectroscopy data was critical in quantifying Because the well had been comprehensively logged prior to the complex mineralogy, including the spectroscopy dry-weight Logging Program for a completion with 5½-in 23-lbm/ft casing, there was extensive TOC as a key input for determining the kerogen volume openhole data from the freshwater-filled well for comparison Shale Gas Reservoir with for evaluating RQ. Having both density and NMR (Track 7) to Pulsar service’s interpretation. Three separate passes of was necessary to compute the gas volume and total porosity Pulsar service were made at 300 ft/h in hybrid GSH-lithology One Cased Hole Tool because they have contrasting responses to kerogen and gas. mode, which simultaneously acquires data for gas, sigma, The operator wanted to learn if the accurate, detailed and hydrocarbon index (GSH) in addition to elemental interpretation provided by an openhole logging program spectroscopy including TOC and the carbon/oxygen ratio. could be achieved with cased hole logging, which would The data were stacked, and a stand-alone volumetric interpretation streamline well construction and reduce the risk posed was conducted using sigma, TPHI, FNXS, and spectroscopy by wellbore instability in the shale reservoir. data, all from Pulsar service. At this relatively slow logging speed, Pulsar service’s spectroscopy data, including dry-weight Solution: Efficiently conducting formation evaluation TOC, has very good precision and compares favorably with in cased hole—without openhole input the openhole data from the larger-diameter advanced Introduced to fill the measurement gaps for cased holes, innovative spectroscopy tool. Pulsar multifunction spectroscopy service obtains a standard formation evaluation suite with a single slim-diameter tool for A stand-alone cased hole interpretation was performed next conducting a complete petrophysical volumetric interpretation. using all the Pulsar service data in a weighted linear solver By employing the state-of-the-art cerium-doped lanthanum with standard end-point values. Again, the interpreted volume
bromide (LaBr3:Ce) gamma ray detector proven by Litho Scanner compares quite favorably, including the gas volumes and total high-definition spectroscopy service, Pulsar service similarly porosity, even though no openhole logs were used in the obtains highly accurate elemental concentrations for a robust interpretation, as would be required if a conventional pulsed determination of mineralogy, including TOC. neutron logging tool had been run. 7 Pulsar CCL AT90 Resistivity Open Hole Neutron-Density –4 V 1 0.2 ohm.m 2,000 Crossover Pulsar Borehole Sigma AT60 Resistivity Magnetic Resonance Porosity Openhole Mineralogy Pulsar Mineralogy 0.2 ohm.m 2,000 0.45 ft3/ft3 –0.15 Measured 0 cu 250 0 V/V 1 0 V/V 1 Depth, ft Pulsar Gamma Ray AT30 Resistivity Bulk Density Openhole Gas Volume Openhole Kerogen Volume Gas Gas TOC TOC 0 gAPI 250 0.2 ohm.m 2,000 1.95 g/cm3 2.95 0.1 V/V 0 0.1 V/V 0 Cable Speed Pulsar Sigma Pulsar TPHI Gas Ratio FNXS AT20 Resistivity Neutron Porosity Openhole Dry-Weight TOC Pulsar Dry-Weight TOC Pulsar Gas Volume Pulsar Kerogen Volume
3 3 Illite Bound Water Quartz Dolomite Aragonite Pyrite Kerogen Gas 0 ft/h 2,000 0 cu 50 0.45 ft3/ft3 –0.15 60 40 6 m–1 8.5 0.2 ohm.m 2,000 0.45 ft /ft –0.15 –0.03 0.12 –0.03 0.12 Illite Bound Water Quartz Dolomite Aragonite Pyrite Kerogen Gas 0.1 V/V 0 0.1 V/V 0
X,500
Where the openhole density and dry-weight TOC logs responded to a transition at ~X,550 ft from low porosity, low kerogen, and low gas volume to higher values below, Pulsar service’s FNXS and dry-weight TOC similarly respond to the low porosity–gas transition at that depth. The lack of change in the sigma and TPHI measurements shows that if conventional pulsed neutron cased hole logs had been run instead of Pulsar service, the transition would not have been obvious.
The operator was pleased that the comparison confirms that Pulsar service’s single-tool performance in cased hole is equivalent to a full suite of openhole logs. Having this reliable, accurate option for X,600 thoroughly evaluating complex unconventional reservoirs in cased hole will simplify future operations and significantly reduce wellbore stability risks.
Comparison of the volumetric interpretation from a full suite of openhole logs (Tracks 10 and 12) with that exclusively from cased hole data acquired with Pulsar multifunction spectroscopy service (Tracks 11 and 13) demonstrates the quality and accuracy of Pulsar service. Total porosity and gas volume, which conventional pulsed neutron logging could not provide without additional openhole input, are particularly well matched. Pulsar service’s new FNXS measurement (Track 5) enables stand-alone computation of an accurate gas volume.
8 Unconventional Reservoirs
Challenge: Lacking high-quality cased hole logging Result: Augmenting accurate RQ and CQ with data for RQ and CQ in lateral wells geomechanical modeling from a single logging run Through-casing measurements, necessary for formation evaluation A single run of a sourceless toolstring comprising Pulsar Case Study and as an input to hydraulic fracture stimulation design, have and ThruBit Dipole services was deployed on the TuffTRAC* been historically difficult to obtain, particularly with sufficient cased hole services tractor to acquire key petrophysical and quality and in lateral sections. An operator in the Niobrara Shale geomechanical formation properties data. Building a Comprehensive was facing this challenge of acquiring high-quality data to Petrophysical Model in One properly evaluate RQ and CQ in two lateral wells. The only available The Pulsar service measurements were spectrally processed interpretation to date was an MWD evaluation based on total with the Quanti.Elan* multicomponent inversion solver to Cased Hole Logging Run to gamma ray measurements obtained during construction of the build a petrophysical model of formation properties, including wells that was not of sufficient resolution to guide completion. mineralogy, porosity, and saturation. The model also provided Guide Niobrara Shale Completions the bulk density required for accurate processing of the Solution: Logging unconventional reservoirs in cased formation elastic properties. In addition to supporting a high- hole with the precision and range of openhole services confidence assessment of RQ and CQ, the model revealed the In addition to running Pulsar multifunction spectroscopy service to presence of marl beds and related subseismic faulting that provide a complete, stand-alone cased hole petrographic volumetric were not identified by the MWD interpretation. interpretation, including TOC and gas-filled porosity, as the basis for reliable RQ and CQ, key geomechanical properties for enriching Dipole sonic data from ThruBit Dipole service was paired with the model would be obtained with ThruBit Dipole* through-the-bit the bulk density to define the elastic properties Young’s modulus acoustic service on the same string. Well suited for cased hole and Poisson’s ratio. These values were key to solving the logging in shale reservoirs, ThruBit Dipole service provides a detailed anisotropic closure stress profile for evaluating potential sonic investigation of the formation, classifying the formation as completion challenges along the lateral and further refining isotropic or anisotropic and determining whether the anisotropy is the CQ. intrinsic or caused by drilling-induced stress. In turn, the bulk density derived from Pulsar service’s volumetric interpretation refines the acoustic processing for mechanical properties, providing critical information for guiding well completion, designing fracturing stages, understanding wellbore stability aspects, and planning trajectories for future wells. 9 Anisotropic closure stress Anisotropic moduli Slow shear Fast shear Compressional Bulk density Petrophysical model XX,120 XX,130 XX,140 XX,130 XX,150 XX,150 XX,160 XX,150 XX,170 XX,150 XX,180 XX,150 XX,150 XX,190 XX,150 X,X60 X,X70 X,X80 X,X90 XX,100 XX,110 XX,200 XX,150 XX,210 XX,220 XX,150 XX,150 XX,230 XX,240 XX,150 XX,150 XX,250 XX,150 XX,260 XX,150 XX,270 XX,150 XX,280 XX,150 XX,290 XX,300 XX,150 XX,150 XX,310 XX,150 XX,320 XX,150 XX,330 XX,150 XX,340 XX,150 XX,350 XX,150 XX,360 XX,370 XX,150 XX,380 XX,150 XX,390 XX,150 XX,150 XX,400 XX,410 XX,150 XX,420 XX,150 XX,150 XX,430 XX,440 XX,150 XX,450 XX,150 XX,150 XX,460 XX,150 XX,470 XX,480 XX,150 XX,490 XX,150 XX,150 XX,500 XX,510 XX,150 XX,520 XX,150 XX,530 XX,150 XX,540 XX,150 XX,550 XX,150 XX,560 XX,150 XX,570 XX,150 XX,580 XX,150 XX,150 XX,590 XX,150 XX,600 XX,610 XX,150 XX,620 XX,150 XX,630 XX,150 XX,640 XX,150 XX,650 XX,150 XX,660 XX,150 XX,670 XX,150 XX,680 XX,150 XX,690 XX,150 XX,700 XX,150 XX,710 XX,150 XX,720 XX,150 XX,730 XX,150 XX,740 XX,150 XX,750 XX,150 XX,760 XX,150 XX,770 XX,150 XX,780 XX,150 XX,790 XX,150 XX,800 XX,150 XX,810 XX,150 XX,820 XX,150 XX,830 XX,150 XX,840 XX,150 XX,850 XX,150 XX,860 XX,150 XX,870 XX,150 XX,880 XX,150 XX,890 XX,150 XX,900 XX,150 XX,910 XX,150 XX,920 XX,150 XX,930 XX,150 XX,940 XX,150 XX950 XX,150 XX,960 XX,150 XX,970 XX,150 XX,980 XX,150 XX,990 XX,150 XX,150
The petrophysical interpretation of Pulsar service measurements in Well B provides mineralogy, bulk density, and fluid analysis. The compressional and fast and slow shear slownesses are obtained from ThruBit Dipole service’s sonic measurements. The slownesses are paired with the bulk density to compute the horizontal and vertical Young’s modulus and Poisson’s ratio. The anisotropic moduli are then used as inputs to the hydraulic fracture stimulation design.
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0 The clay volume, obtained from the petrophysical model built with 0 0.05 0.1 0.15 0.2 0.25 0.3 Pulsar service measurements, exhibits abrupt changes along the Clay volume, V/V well path where transected by marl as the result of faulting. Tool depth Because some of the faults are at the subseismic level, they had not been previously identified. The marl in the toe half of Well A (III) was also not previously identified because there was no correlation between the clay volume and MWD total I II III gamma ray measurement. Identifying the presence of marl is important for anticipating production challenges because marl often contains ash beds that can pinch off production. 10 The next generation in formation evaluation and reservoir monitoring in cased hole
Pulsar multifunction spectroscopy service integrates significant advances in spectroscopy in a slim OD of only 1.72 in for ready through-tubing access in cased hole environments. Building on technologies first introduced to the industry by Litho Scanner high-definition spectroscopy service, Pulsar service pairs a pulsed neutron generator with four detectors: ■■ Compact neutron monitor, primarily sensitive to fast neutrons, adjacent to the high-output PNG for accurate and precise measurement of the source output ■■ Three scintillation gamma ray detectors for near, far, and deep detection
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Near and far detectors are closest to the source and have cerium-doped LaBr3:Ce scintillators. ●● Deep detector is the farthest-spaced detector from the PNG source and uses a YAP scintillator. All three gamma ray detectors are coupled to high-temperature photomultiplier tubes with integrated low-noise power supplies. | | | | | | | | | | | | | | | | | | Detector pulses are counted with specialized electronics matched to the high counting rate capabilities and high resolution of the LaBr3:Ce scintillators and ruggedized to operate at high Elemental standard spectra measured with Pulsar service’s LaBr3:Ce gamma ray detector (blue) on the left panel have better resolution, with sharper, better defined temperatures. features that improve the accuracy of deconstructing each measured spectrum into its components, in comparison with the spectra from conventional BGO detectors (red). The right panel compares performance at elevated temperatures. At 150 degC [350 degF], LaBr3:Ce (blue) maintains its high light output, whereas the BGO The slim tool profile enables fitting through most completion (red) decrease in light output significantly degrades the elemental standard spectra at only 60 degC [150 degF]. restrictions. Detector resolution is only minimally degraded at high temperatures to 175 degC, avoiding conventional use of a flask, or in the neutron generator output. However, these two causes output normalization, a solid-state diamond detector is incorporated which would increase the tool diameter. The housing is corrosion cannot be rigorously separated without resorting to taking a ratio in Pulsar service’s tool architecture. This detector is highly sensitive resistant and qualified per the requirements of NACE MR0175, of different detector or timing-window count rates to provide to fast neutrons yet largely insensitive to low-energy neutrons and enabling deployment in corrosive well environments such as those insensitivity to source output variations. A common practice gamma rays. in the presence of H2S or CO2. with previous-generation measurements, such as neutron porosity, was to use a ratio of a farther-spaced detector count rate to In addition to its dual sensitivities, the CNM’s diamond detector Compact neutron monitor that of a nearer-spaced one. Although this is an effective way to has several other advantages. It has a high 5.5-eV bandgap, which Unlike radioisotopic neutron sources, PNGs have a neutron output normalize for source output variations, the nearer detector’s count minimizes the dark current, leakage current, and noise while that can vary with time. This means that count-rate variations in rates are generally more sensitive to the borehole environment supporting good stability at high temperatures. The detector’s excellent a pulsed neutron tool can be caused by a change in the formation than the farther-spaced ones, and not all environmental effects radiation hardness means that its sensitivity to fast neutrons does are reduced by taking a ratio. To enable more-effective neutron not significantly deteriorate over the tool’s operating life. Most
11 New hardware for new measurement capabilities and higher accuracy importantly for this slim tool, the detector is sufficiently compact integral and low thermal capture cross section). This results in Signal processing to be placed in proximity to the neutron source point without a lower background signal from neutron capture in the detector Higher neutron output and fast detection of gamma rays are taking space away from the gamma ray detectors or affecting and an enhanced relative contribution from formation gamma rays of no value unless the pulse processing electronics in the tool the inline shielding. to enable better separation of the inelastic gamma ray counts from can handle the resulting signals. Pulsar service has adapted the simultaneous epithermal and thermal capture counts that Litho Scanner service’s proprietary pulse processing electronics YAP deep detector occur during the neutron burst. Good separation is important that produce high-quality spectra at high count rates. For good Different materials were considered for the scintillator of the for the measurement of FNXS. Another advantage of YAP is spectral response, each pulse must be distinguished from its deep, farthest-spaced gamma ray detector. The purpose of that its relatively high density of 5.37 g/cm3 is good for detector neighbors. At high count rates, pulse pileup can distort the the deep detector is to collect information about the formation efficiency. Because it is nonhygroscopic, it requires no hermetic measured spectrum if not accounted for. To achieve a high count beyond what can be obtained from the near and far detectors. packaging, which allows using the maximum possible crystal rate but a low fraction of pileup counts, Pulsar service uses The near and far detectors are close enough to the neutron source diameter, in turn giving the highest count rate possible. YAP an improved pileup rejection technique, which, in combination that they have very high peak count rates, nominally 1.0 × 106 is also mechanically robust, which reduces the risk of breakage with the increased energy resolution and excellent temperature and 0.7 × 106 cps, respectively, for typical conditions. LaBr :Ce 3 during transportation and operation. In addition, the scintillation performance of the very fast crystal and pulse processing electronics, was chosen for those scintillators because of its high speed and properties of YAP in the temperature range from –40 to 175 degC makes the inelastic spectral quality much better than that of any excellent spectroscopy performance. For the farther-spaced deep remain almost constant, which supports an exceptionally stable deep- other pulsed neutron tool at any tool diameter. The situation is even detector, the gamma ray flux is much lower, and spectroscopy detector response at any operating temperature of Pulsar service. better for the capture measurement. would add little additional precision to the formation measurement. Therefore, the deep-detector scintillator material was optimized The gain regulation of the YAP detector does not require the use for the fast neutron cross section (FNXS) measurement. of a radioisotopic source. Rather, it is based on spectral features in the neutron-induced gamma ray spectrum. Similar methods of YAP (YAlO3) has several advantages as a scintillator material for gain regulation are used for the LaBr3:Ce detectors. This approach the FNXS. One of the most appealing properties of YAP is that eliminates all radioactive material from the tool with the exception its constituents (Y, Al, and O) have a very low cross section for of the tritium contained in the PNG. epithermal and thermal neutron capture (i.e., a low resonance
12 The science of spectroscopy
The neutrons emitted by Pulsar service’s PNG induce the emission of gamma rays from the formation via two primary interactions: inelastic SpectralSpectral Acquisition Acquisition SpectralSpectral Stripping Stripping ClosureClosure InterpretationInterpretation scattering and thermal neutron capture. Each • Inelastic• Inelastic • 14 inelastic• 14 inelastic yields yields • Elemental• Elemental weight weight fractions fractions • Minerals• Minerals of these interactions produces gamma rays 1 1 2 2 3 3 4 4 • Capture• Capture • • • • with a specific set of characteristic energies. 19 capture19 capture yields yields MatrixMatrix properties properties • TOC• TOC The coupling of the LaBr :Ce detector to the 3 InelasticInelastic InelasticInelastic high-temperature spectroscopy photomultiplier produces signals that are integrated, digitized, and processed by a high-performance pulse-height Corrected forCorrected TOC for TOC Al CaAl S Ca Fe S Fe analyzer. The analyzer determines the pulse 2 g /cm 23 g /3cm 3 3 height (proportional to energy) of each detected Matrix D eMnastirtyix D en s ity T O C T O C 3 3 gamma ray and accumulates pulse-height Chlorite IIlite Montmorillonite Chlorite Quartz IIlite K-Feldspar Montmorillonite Na-Feldspar Quartz Calcite K-Feldspar Dolomite Na-Feldspar Anhydrite Calcite Pyrite Dolomite Kerogen Anhydrite Pyrite Kerogen 2 g /cm 2 g /3cm 3 histograms (spectra) that tally counts versus O O pulse height. Spectra are acquired during and C C after each neutron burst, which enables separation Si Si of the inelastic and capture gamma rays. SulfurMg SulfurMg Iron Iron