Presentation is loading. Please wait.

Presentation is loading. Please wait.

Triple Detector Lithology Density

Similar presentations


Presentation on theme: "Triple Detector Lithology Density"— Presentation transcript:

1 Triple Detector Lithology Density
Platform Express* TLD Triple Detector Lithology Density

2 Outline Introduction to Density Measurement Hardware Description
Physics of Measurement Gamma Ray Interactions, Detector response Nuclear Spectrum, Gain stabilization Measurement Analysis Response model, Inversion algorithm, Examples Operations Parameters, Corrections, Calibration Safety LQC Log Examples, Products Sonde Mechanics - Overview

3 Introduction to Density Measurement
Density Tools measure two main properties: DENSITY ==> bulk density of the formation LITHOLOGY==> indicator of formation type POROSITY can be derived from Density Measurement Caliper The tool design also allows a simultaneous caliper measurement Density Logging Schematic

4 Density Tools History PGT - Powered Gamma Tool
LDT - Litho Density Tool TLD - Triple Detector Litho-Density Fundamental Difference in Tool Physics and Detectors have been implemented with each evolution of tool.

5 TLD Measurement Objectives
The main objectives of the Platform Express density measurement are: Give a high resolution estimate of density when pad application is good and mudcake thickness small (<.5”) Provide a robust formation density measurement in bad borehole conditions (rugosity, standoff) Improve the Pe measurement with regard to precision (statistical error) and mudcake effect compensation Reproduce the LDT density estimation when this tool performs well

6 TOOL Hardware: PLATFORM EXPRESS - Density
Highly Integrated Gamma Ray Neutron Sonde GR 24 in. HGNS jN 24 in. Electronics cartridge HRCC rb, Pe 18 in., 8 in., 2 in. PE02 The initial PLATFORM EXPRESS configuration includes a new standard in formation evaluation sensors. The traditional triple-combo suite of resistivity and porosity measurements has been upgraded and expanded to include microresistivity, imaging and tool movement measurements. PLATFORM EXPRESS technology will evolve to include additional sensors in the future. Starting at the bottom, PLATFORM EXPRESS includes a choice of resistivity measurements with either the AIT* Array Induction Imager tool or the High-Resolution Azimuthal Laterolog Sonde. Both tools include the latest advances in resistivity sensor design and specifications. The maximum vertical resolution of the resistivity measurements is 12 in. The High-Resolution Mechanical Sonde has an integrated pad, or skid, that is pressed against the formation. The pad has two new interlaced sensors—the Three-Detector Lithology Density and the MicroCylindrically Focused Log. The TLD log is a backscatter-type density measurement with a vertical resolution of 8 in.; the new MCFL microresistivity measurement investigates the same volume of formation as the density and has a vertical resolution of 2 in. Flex joints are built in above and below the mechanical sonde to greatly improve pad application in rough hole. Above the mechanical sonde is a single power supply and electronics cartridge. Older-generation equipment required one electronics cartridge per tool. This made for extremely long tool combinations that required longer rig-up time and required almost a hundred feet of rathole. We have re-engineered today's gamma ray and neutron porosity measurements into a single Highly Integrated Gamma Ray Neutron Sonde. The gamma ray and neutron porosity measurements have a standard vertical resolution of 24 in. Alpha processing is available to achieve 12-in. vertical resolution of the neutron log. This section of the string also houses the high-speed telemetry electronics and an accelerometer that provides real-time speed correction and automatic depth-matching of the curves. High-Resolution Mechanical Sonde HRMS Rxo, hmc 2 in. Array Induction Imager Tool High-Resolution Azimuthal Laterolog Sonde Rt 12 in. HALS AIT

7 High-Resolution Skid MCFL MicroCylindrically focussed log
TDD Detector Density LS Long Spacing Detector SS Short Spacing Detector BS Back Scatter Detector

8 High-Resolution Skid - inside
Safety !!

9 Detectors - PM/HV/Crystal Integration
TDD Detectors Scintillation Detectors are used Photomultiplier and High Voltage Supply are integrated in one package No Field Disassembly possible - only factory repair EMR Compact PMT with integrated High Voltage Supply Backscatter Detector shown above

10 Density GR Detectors TDD Detectors Long Spacing (LS) Detector
Scintillation Detectors are used Long Spacing (LS) Detector NaI (T) Sodium Iodide,Thallium doped (not colimated) Short Spacing(SS) Detectors NaI (T) Sodium Iodide,Thallium doped (not collimated) Backscatter (BS) Detector GSO - Gadolinium Orthosilicate, Cerium doped, (collimated0 NaI is rated to 350 degf. GSO has lesser temp rating than NaI GSO is more efficient than NaI GSO is very expensive

11 Detector Characteristics
Detector LS SS BS Spacing(cm) Crystals Nal Nal GSO Length (mm) Diameter (mm) Resolution Cs 137 line 11.7% 13% 14.5% MAX. Counts CPS outputs 40, ,000 1,200,000 Sensitivity* To density -6.3 to to to To Pe Signal/BKG 1.2 to to to 4

12 DENSITY PHYSICS

13 Gamma Ray Interactions - Review
High Energy GR emitted from chemical source Reacts with matter in formation Type of interaction dependent on GR energy level Source used is Cesium-137, 662 Kev Hence Compton Scattering and P.E. Absorption occur Compton Scattering Photoelectric Absorption GR < 100 Kev GR > 100 Kev Pair Production GR > 1.02 Mev

14 Interaction of Gamma-Rays
Compton scattering Defining (electron density) (for most elements Z/A~1/2) Photoelectric effect Defining (Photoelectric factor) Pair production (electron - positron)

15 Density Physics - Compton Scattering
Electron density index and Bulk Density Ne = Rhob * Z * Na / A Rhoe = Rhob * ( 2 Z / A) ## ( 2 Z / A) ~ 1 Rhoe  Rhob ## 2Z / A almost equal to 1 except for Hydrogen Measuring Rhoe we know Rhob (Ne) Number of electrons in one gram (A) Atomic weight - the mass of an atom (grams/gram-atom). (Z) Atomic number (Z) - the number of electrons in a neutral atom (electrons/atom). (Na) Avogadro's number (Na ) - the number of atoms in a gram-atom (6.02 x 1023 ). (Rhob) Bulk density (Rhoe) Electron density index

16 Density Physics - examples
Properties of common elements in formations

17 rbulk (actual bulk density of formation)
Density Corrections Differences exist between rbulk (actual bulk density of formation) relectron (electron density of formation) rapparent (what the tool measures) Most times the corrections are negligible Correction charts are available Tool is calibrated for water filled LIMESTONE Hence zero correction for Limestone

18 Density Physics - Photoelectric Absorption
Reaction occurs at Low Energy à GR < 100 Kev GR interacts with shell electrons à Absorption Shell electrons related to à Z Atomic number Higher Z means higher PE absorption Count the GR reaching tool after the interactions measure PEF à (PEF = (z/10)3.6) Knowing ... PEF (Z) à LITHOLOGY

19 Density and PEF - common minerals and liquids
** Also see Log examples later in the presentation.

20 Density Physics - Summary
High energy GR emitted from chemical source Source Energy 662 Kev Compton Scattering and Photoelectric Absorption After interactions, GR reaches the Scintillation detectors Density tool measures Electron Density Electron density is related to Bulk Density 2Z/A is almost equal to 1 for common formation Electron density almost equal Bulk Density Heavier the matter higher the Z atomic number Higher Z means higher Photoelectric absorption Tool also measures the absorption factor Knowing PEF (Z) gives indication of formation

21 Density Nuclear Spectrum
GR Detector Electronics Spectrum Energy Count Rate After interaction with the formation, GR reaches crystal Incident GR have different energy levels Both .. Energy and Counts of the GR are of interest Detector pulse height proportional to GR energy The pulses are then sorted and counted by electronics The count rate vs energy distribution is called Spectrum The Spectrum will vary with formation - (GR interactions)

22 Nuclear Spectrum - Regions
Lithology Window Region of Photoelectric Effect ( r & Z Information) Density Window Region of Compton Scattering Count/Sec ( r Information Only) Source Energy 662 keV Energy keV

23 Spectrum Change with Lithology
Region of Photoelectric Effect ( r & Z Information) Count/Sec Region of Compton Scattering (Low Z) ( r Information Only) (Med Z) (High Z) r = constant Source Energy 662 keV Energy keV

24 Spectrum Change with Density
Count/Sec/keV Region of Photoelectric Effect Region of Compton Scattering (Low r) (Med r) Z = constant (High r) Source Energy 662 keV

25 Spectrum Stabilisation
GR Detector Energy Count Rate Spectrum Detector level/gain (e.g. temperature) can shift the spectrum Energy Count Rate PM High Voltage 662 Kev Reference Source Reference R/A source 1 mcu, 662 Kev is used This has a small spectrum centered at 662 Kev Therefore Photomultiplier High Voltage is adjusted. CONTINUOUS FEEDBACK LOOP

26 Spectra Comparison - LS
WATER LIMESTONE DIABASE Attenuative - decreasing count rates with density. This also applies to SS. Two orders of magnitude between counts in water and diabase.

27 BS Spectrum - behaves differently
Positive - increasing count rates with density. Factor of two between counts in water and diabase.

28 BS Spectrum The BackScatter Spectrum differs from LS and SS
Count rates are much higher Therefore GSO crystal is used Increasing density results in increasing counts This is mainly due to detector design The Backscatter detector is COLLIMATED Formation

29 Processing Outputs Standard resolution High resolution (main)
Resolution of 18” Output sampling rate: 2” LDT like output RHOZ, PEZ, UZ, ROMZ, PEMZ, DSOZ High resolution (main) Resolution of 8” RHO8, PE8, U8, ROM8, PEM8, DSO8 Very high resolution Resolution of 2” Output sampling rate: 0.5” RHOI, PEI, UI, DSOI

30 Density Hole Correction
Bit Size Apparent Bit Size

31 Density Hole Correction
Bit Size

32 Density Hole Correction
Bit Size Apparent Bit Size

33 Density Hole Correction
Bit Size Caliper Reading

34 Density Hole Correction
Bit Size Apparent Bit Size

35 SAFETY

36 TDD - Safety HRMS is heavy - back injury hazard - Plan the lifting
HRGD skid is heavy- When caliper is open look out for finger crushing Depleted Uranium Shield in the HRGD- do not dismantle the HRGD skid Beryllium Window is highly poisonous - do not scratch /puncture the BS or SS cover Be careful during Q-check Detector Reference source is CS-137 9 mCi for BS and LS, 0.6mCi for LS Cs-137 is toxic, Use tweezers while handling Thallium doped NaI crystal - handle with care. Mildly poisonous Dessicant in electronics causes irritation Use gloves for handling, Wash hands, Do not ingest, or contact with eyes High voltages present in the tool 250V head voltage 3000 V (max) for PM tube. GSR-J source used for logging All R/A precautions and rules to be followed

37 SAFETY - GSR-J Source 2 mrem/hr 17 metres The GSR-J source is collimated - Do not Stand in front 2 mrem/hr distance is 17 metres in front of skid Source Handling Tool and Safety Clip must be used Radiation Badge must be worn Only the Engineer is allowed to transfer a Radioactive Source

38 LOG QUALITY CONTROL

39 Quality Indicators Hardware quality flags
Tau loop error /Offsets /Crystal resolution /Low energy noise /Total count rate /P.M high voltage/ Form Factor Density Detector Quality Flag Processing quality indicators Density Computation Quality Flag Pe computation Quality Flag Based on reconstruction errors (W - W )/W and database limits Cal Rec Density correction curve (r - r ) LOW LS

40 Hardware - LQC

41 Processing - LQC

42 DENSITY LOG RESPONSE and EXAMPLES

43 Density - Porosity Calculation
Density response model rf rma 1-f f Volumetric Contribution rb = rma (1-f ) + rf f f = (rma- rb) (rma- rf) Bulk Density is measured. Matrix Type and the Fluid Type from Lithology identification Porosity can be derived from Bulk Density if matrix known

44 Density Log Example - 1... Lithology Identification
Shale Sand - Hydrocarbon Bearing Sand - Water bearing X800

45 Density Log Example - 2.. Sandstone Shale Limestone Shale

46 Density Log Example SALT Shale Sand- shaly

47 Density Log Example Dolomite Limestone

48 Density Log Example Anhydrite

49 Answer Product - example ... (unreleased example)
LITHOCOLUMN Carbonate Reservoir AIT Resistivity Image Resistivity Logs Nuclear Logs RHOZ NPHI PEFZ SP Caliper GR PEX ANSWER Product with Lithology Analysis from TDD measurements is shown above. Correct PEF reading is crucial The TDD provides formation PEF measurement corrected for heavy mudcake (barite) effects , previously not available.

50 Summary - TDD Measurement
High resolution density measurement (BS-SS) Formation Pe compensated for mudcake effect (non-barite environment) Good statistics in hard formations Mudcake thickness estimation Co-located Rxo measurement

51 HRMS Overview - Mechanical Design

52 Flex Joint Advantage - Rugosity
Hinge Joints Good Pad Contact in Rugose Holes

53 HRMS - Short Radius Logging
PEX is useful for deviated wells with short radius, due to the high flexibility of HRMS Good Field examples No tools stuck or seriously damaged Minimum Dogleg Radius: metres Max Build Rate: deg/30m average 72 deg/30m Bit Size: 6 1/4” - 8 1/2” Depths: m Need to convey on Drill Pipe 30 metres measured depth Build Angle


Download ppt "Triple Detector Lithology Density"

Similar presentations


Ads by Google