MRIL OVERVIEW Team One NUMAR / HALLIBURTON. Crucial Formation Evaluation Questions What is the storage capacity (  e and  t ) in a Complex Lithology.

Slides:



Advertisements
Similar presentations
Pulse Timing parameters & Weighting
Advertisements

Title Petrophysical Analysis of Fluid Substitution in Gas Bearing Reservoirs to Define Velocity Profiles – Application of Gassmann and Krief Models Digital.
The analytical measurement principle
Contrast T1 weighted – (MPRAGE-anatomical) T2 weighted – (fmri)
MRI Phillip W Patton, Ph.D..
BE 581 Lecture 3- Intro to MRI.
PHYSICS OF MAGNETIC RESONANCE
Geological and Petrophysical Analysis Of Reservoir Cores
Tim Armitage.  Shale Gas Reservoir's  The problems with Shale Reservoirs  What is needed to Create a usable model  Possible solutions to Porosity.
1 Laboratory MR Measurements and MRIL ® Integration by Dave Marschall.
EAS 430: Petroleum Geology
Formation Evaluation (Lecture) Subsurface Methods 4233
Features u 9 discrete measurement volumes u Accelerated polarization - 12 sec in 6 sec u more robust electronics and new sonde Benefits u Single-pass,
Inferring Axon Diameter Sizes using Monte Carlo Simulations of Magnetic Resonance Oscillating Gradient Spin Echo Sequences ME Mercredi 1, TJ Vincent 2,3,
Relaxation Exponential time constants T1 T2 T2*
FMRI: Biological Basis and Experiment Design Lecture 5: non-BOLD MRI Equilibrium and excitation Relaxation rates Image contrast –TE –TR.
Psy 8960, Spring ‘07 Inversion Recovery1 Exponential decay  = 30 ms.
Nuclear Magnetic Resonance (NMR) Magnetic Resonance Imaging (MRI)
Basics of Magnetic Resonance Imaging
NMR Core-Analysis in Unconventional Resource Plays Rice University Consortium on Processes in Porous Media Department of Chemical & Biomolecular Engineering.
Magnetic Resonance Imaging Basic principles of MRI This lecture was taken from “Simply Physics” Click here to link to this site.
Psy 8960, Spring ’07 Introduction to MRI1 Introduction to MRI: NMR Physics reminders –Nuclei and atoms –Electromagnetic spectrum and Radio Frequency –Magnets.
Physics of Magnetic Resonance Chapter 12
대구가톨릭대학병원 영상의학과 이 영 환 M M R R Basic Physics. MR Signal T1-, T2-weighted TR, TE MR Signal T1-, T2-weighted TR, TE.
COMPRESSIBILITY OF RESERVOIR ROCKS.
Ron Cherry, Maged Fam and Emiliano López
Principles of Magnetic Resonance
ELEG 479 Lecture #12 Magnetic Resonance (MR) Imaging
Chapter 4 Mark D. Herbst, M.D., Ph.D.. Magnetization MRI depends on magnetization of tissues Temporary magnetization occurs when the hydrogen nuclei are.
Super Combo The previous generation CNT, LDT, NGT.
International Shale Development Optimization
Geology 5660/6660 Applied Geophysics 26 Feb 2014 © A.R. Lowry 2014 For Fri 28 Feb: Burger (§8.4–8.5) Last Time: Industry Seismic Interpretation.
Petroleum Engineering 406 Lesson 4 Well Control. Read Well Control Manual –Chapter 9 Homework 2 Due Feb. 3, 1999.
February 20, 2003Francisco M. Martinez Magnetic Resonance for BME 458 Francisco (Paco) Martinez.
Basic Concept of MRI Chun Yuan. Magnetic Moment Magnetic dipole and magnetic moment Nuclei with an odd number of protons or neutrons have a net magnetic.
September, 2003BME 1450 Introduction to NMR 1 Nuclear Magnetic Resonance (NMR) is a phenomenon discovered about 60 years ago.
1 4 Geology and Groundwater Introduction –Geology complexities are reflected in hydrogeology –Geology is the basis for any groundwater investigation Topics.
Improved Permeability Measurement using T 2 Bin-Distribution and Bulk Volume Irreducible from Nuclear Magnetic Resonance Tools Case Study: Granite Wash,
Nuclear Magnetic Resonance I Magnetization properties Generation and detection of signals.
Low–field NMR (or MRI) Images of Laser polarized Noble Gas.
1 SPE Distinguished Lecturer Program Primary funding is provided by The SPE Foundation through member donations and a contribution from Offshore Europe.
POROSITY DETERMINATION
Magnetic Resonance Imaging – Basic Principles –
MRI Physics Dr Mohamed El Safwany, MD.. MRI Magnetic Resonance Imaging Magnetic Resonance Imaging.
Lecture items - Compositions of the Uphole- Downhole Instruments. - Field Operation (Data Acquisition, Processing and Transmission) - Log Runs - Borehole.
BME1450 Intro to MRI February 2002 The Basics The Details – Physics The Details – Imaging.
Uncertainty in AVO: How can we measure it? Dan Hampson, Brian Russell
Study of T 1 relaxation time A proposal to test T 1 using a dilution fridge and SQUID NMA at Royal Hollow University,London.
DSI* Dipole Shear Sonic Imager
Magnetic Resonance Imaging Glenn Pierce, King’s College London, Department of Physics Introduction Edward Purcell and Felix Bloch were both awarded the.
MRI: Contrast Mechanisms and Pulse Sequences
Geology 5660/6660 Applied Geophysics 26 Feb 2016 © A.R. Lowry 2016 For Mon 29 Feb: Burger (§8.4) Last Time: Industry Seismic Interpretation Seismic.
University of Kerala, India.
What is Well Logging?
MRI Physics in a Nutshell Christian Schwarzbauer
Where Mt is the magnetization at time = t, the time after the 90o pulse, Mmax is the maximum magnetization at full recovery. At a time = one T1, the signal.
Magnetic Resonance Imaging: Physical Principles
Basic NMR Physics and MRIL® Tool Physics
Physics of Magnetic Resonance Imaging
Lecture items * Theory of measurement of other resistivity logs.
Well Logging Gly 326.
MRIL Applications Mechanisms of Relaxation Interpreting NMR T2 Spectra
Seismic Response What causes a seismic response?
A Geologic Model 1m 75 m Perm 250 mD Sand Shale 0.1 mD 50 m Slide 16
Presented by: Brad Cross, ERM October, 2018
Electrical Properties
Electrical Properties
(4)ELECTRONIC SUPPORT SYSTEM
T2 Relaxation Time T2 relaxation time is defined as the time needed to dephase up to 37% of the original value. T2 relaxation refers to the progressive.
Presentation transcript:

MRIL OVERVIEW Team One NUMAR / HALLIBURTON

Crucial Formation Evaluation Questions What is the storage capacity (  e and  t ) in a Complex Lithology Environment ? Are there hydrocarbons, ï what types of hydrocarbons and, ï how are they distributed? What is the permeability (deliverability)? Will the formation produce water free? (what is irreducible saturation (BVI)) MRIL answers them all

Only Fluids are Visible “Thin Slice” Image H Medical MRI

hydrocarbon hydrocarbon Oilfield MRI (Relaxation Time Spectrum) Fluids Solids….invisible to MRI time, sec ……. irreducible movable water movable water movable water irreducible clay bound T 1 Magnetization no measurement T 2 relaxation times the measurement rock matrix dry clay

Magnetic Dipole Proton H Hydrogen N S NMR works with Protons - Hydrogen -> H 2 O and C x H y +++

N S N S N S N S N S N S N S N S N S N S N S N S N S N S t = 0 Random Orientation in Natural State Bo

N S N S N S N S N S N S N S N S N S N S N S N S N S N S t = 0.75 sec M Bo=External Field M=Bulk Net Magnetization Wait time (sec) Magnetization Buildup Bo

N S N S N S N S N S N S N S N S N S N S N S N S N S N S t = 6.0 sec M Bo=External Field M=Bulk Net Magnetization Wait time (sec) Buildup at 95 % polarization Bo

Polarization Time T2T2 Decay Time T1T1 Magnetization T 1 characterizes the rate at which longitudinal magnetization builds up T 2 characterizes the rate at which transverse magnetization decays B0B0 MLML MTMT T 1 build-up and T 2 decay

NMR Experiment Timing MoMo 0 M  to B o (longitudinal component) M  to B o (transverse component) MoMo 0 RF field 0 B1B time, seconds TWTW TETE TXTX adapted from Murphy, D.P., World Oil, April 1995 T 1 = 400 msec T 2 = 250 msec

3 * T 1 = Tw 95% Polarization % Polarization *  = Measured Porosity t (s) % Polarization Gas: T 1 = 3s Water: T 1 = 0.33s T 1 Magnetization build up Light Oil: T 1 = 2s

T 1 Build-up T 2 decay Low Porosity Clean Cgr Sandstone Low Porosity Shaly Fgr Sandstone Higher Porosity Shaly Cgr Sandstone Time, sec. Effects of Chemistry and Texture on T 1 and T 2 (water filled)

MRIL ProbeBorehole Sensitive Volume Cylinders (each 1 mm thick at 1 mm spacing) 24 “  16” Permanent Magnet and Field Pulsing RF and receiving RF Antenna MRIL in Wellbore

MRIL Diameter of Investigation Multi - Frequency Series C Tool Frequency 3  NUMAR Corp., 1995 Formation 16” Frequency 1 6” Borehole Wall Mud Sonde Sleeve Magnet RF Antenna N S Frequency

time (ms) Amplitude (pu) Decay rate (1 / T 2 ) => rock & fluid information Measured signal decay TETE TETE Amplitude = Porosity

3 Relaxation Mechanisms Bulk Relaxation - T 2B Intrinsic Property of fluid Diffusion - T 2D Molecular Movement Surface Relaxation - T 2S Pore-walls cause rapid dephasing Effect of Each Mechanism is Additive Time, msec. Amplitude Echo Amplitude vs Time

T2T2T2T2 T2T2T2T2 T2T2T2T2 T2T2T2T2 T2T2T2T2 time time time time time Pore Size and T 2 (Water) T 2 = relaxation time constant. S = surface area of the pore. V = volume of the pore.  2 = relaxation rate constant.

Surface Relaxation Mechanism Water Filled Pores Time, msec. T 2 -1  S/V) Small Pore Sizes = Rapid Decay Rate Large Pore Sizes = Slow Decay Rate

Data Processing - Inversion T 2i are pre-selected: T 2i = 4, 8, 16, 32, 64, 128, 256, 512, MAP “Inversion” Processing T 2 [ms] Incremental Porosity [pu] T 2 Spectrum “Best Fit” Water-saturated rock:  2 = V/S  NUMAR Corp., 1995 BVI FFI

phi- NMR (pu)

Permeability Chart E S wir Porosity E (  x Swirr) increases k (md)

MRIL Permeability MPERM = ((MPHI/10) 2 (MFFI/MBVI)) 2 MPHI - MRIL Porosity (porosity units) MBVI - MRIL Bulk Volume Irreducible MFFI - MRIL Free Fluid Index MPERM - Permeability (millidarcies)

Differential Echo / Spectrum Method

Effect of Diffusion on T 2

Diffusion - Shifted Spectrum Method

Pay Recognition from EDM The Effect of Long T E

Density Porosity Neutron Porosity Effective Porosity Variable Density (milliseconds) T2 Distribution 20482

What’s new ? Pick your choice Low resistivity pay Extra pay identified Shale, Huh ? Integrating core data and MRIL data