|
CRAIN’S
PETROPHYSICAL
POCKET
PAL

This is the condensed version of Crain's
Petrophysical Handbook. It is designed for practical day-to-day use in
the office or at the wellsite. It can be used as a self-guided short
course or reference manual by individual practitioners. If you
intend to teach a course based largely on this material, please read
the Fine Print.
YOU MAY TAKE
THIS COURSE BY CORRESPONDENCE,
email us FOR
DETAILS.
TABLE
OF CONTENTS
1.00
Introduction Quantitative Log Analysis
1.01
What Is A Log?
1.02
Organizing Your Work
1.03
Calculators and the Math Hierarchy
2.00
The Step by Step Procedure
2.01
The Analysis Model
2.02
The Formation Rock Model with Definitions
2.03
The Log Response Equation
2.04
Using The Log Response Equation – Seismic Modeling
2.05
Integration – Calibrating to Ground Truth
3.00
Eyeball Analysis Of Logs - Crain’s Rules
3.01
General Rules For Picking Log Data
3.02
Selection of Log Interpretation Parameters
4.00
Shale Volume
5.00
Pore Volume
5.01
Porosity From The Sonic Log
5.02
Porosity From The Density Log
5.03
Porosity From The Neutron Log
5.04
Porosity From The Complex Lithology Density Neutron Crossplot
5.05
Porosity From The Dual Water Density Neutron Crossplot
5.06
Porosity From The Photoelectric Density Neutron Crossplot
5.07
Material Balance for Porosity (Maximum Porosity)
5.08
Useful Porosity
5.09
Porosity From The Nuclear Magnetic Resonance Log
5.10
Fracture Porosity
5.11
Porosity from Old ES Logs
6.00
Lithologic Analysis of Matrix Rock Volume
6.01
Two Mineral Lithology From Matrix Density
6.02
Lithology From Sonic Density Neutron Data
6.03
Lithology From PE Density Neutron Log
6.04
Lithology From Spectral Gamma Ray Log
6.05
Lithology From Vp/Vs Velocity Ratio
6.06
Elastic Constants / Mechanical Properties From Logs
7.00
Formation Water Resistivity
7.01
Water Resistivity From Catalog or DST
7.02
Water Resistivity From Water Zone (Rwa)
7.03
Water Resistivity From Spontaneous Potential
8.00
Water and Hydrocarbon Saturation
8.01
Determination of Saturation Parameters A, M, N
8.02
Water Saturation from Archie Method
8.03
Water Saturation from Simandoux Method
8.04
Water Saturation from Dual Water Method
8.05
Water Saturation from Buckles Number
8.06
Irreducible Water Saturation
8.07
Moveable Oil Saturation
9.00
Permeability and Productivity
9.01
Permeability from the Wyllie-Rose Method
9.02
Permeability from Porosity
9.03
Permeability from the Coates Method
9.04
Fracture Permeability
10.00
Summarizing Results
10.01
Cumulative and Average Reservoir Properties
10.02
Fluid Properties and Reserves
10.03
Productivity Index and Water Cut
11.00
Beyond Log Analysis
11.01
Productivity From Drill Stem Tests
11.02
Production Projection and Cash Flow
12.00
Case Histories / Exercises
12.01
Cretaceous Glauconitic Sand
12.02
Triassic Dolomitic Sand
12.03
Devonian Carbonate Reef
12.04
Tar Sands
13.01
List of Abbreviations
CRAIN’S
PETROPHYSICAL
POCKET
PAL
1.00
Introduction To Quantitative Log Analysis
This Handbook is designed to give you a starting point for learning
quantitative log analysis methods. It is a condensed version of
Chapters 4 through 11 of Crain’s Petrophysical Handbook on CD-ROM,
avail able at
www.spec2000.net.
When log analysis is combined with sample, core, test and production
data, it is called Integrated Petrophysics or just plain
“petrophysics”.
You can
use this book as a quick reference to quantitative petrophysical
analysis or as a self-directed study guide. If you wish to take the
exam at the end of this book to earn a certificate of proficiency,
please go to my website at
www.spec2000.net
and click on the Learning Center tab.
To
get maximum benefit from available well data, you must integrate
logs, cores, samples, tests, seismic, geological, and engineering
concepts into a coherent picture. Log analysis performed in
isolation is pointless and can be a career-buster. However, learning
log analysis methods can be done in relative isolation, as long as
we appreciate the contributions available from other disciplines. It
is really important to temper, and sometimes completely revise, the
results of your log analysis by comparison to other sources of
“ground truth”.
Using
productivity analysis based on accurate shale, porosity, lithology,
saturation, and permeability calculations from log data, you can
compare the quality of a zone with known production in your area.
From this, you can decide if the well is worth completing or whether
to drill more similar wells. You can also high-grade your drilling
or completion prospects based on estimated flow capacity as well as
the more usual net pay figures. This handbook provides the methods
to extend conventional well log analysis to cover productivity and
cash flow analysis.
The real
question you must answer is not "What is the porosity and water
saturation?" but "Will the zone produce economically and at what
rate?" This goes considerably beyond conventional log analysis.
That’s why my petrophysical software is called Meta/Log (Meta =
Beyond). There are cases where you cannot get this far, either for
lack of corroborative data or narrow-minded job descriptions, but it
never hurts to try. The full spectrum techniques described here will
help you find oil and gas more effectively from logs, complete
discoveries more economically, and work-over wells with more
confidence.
Crain’s Petrophysical Pocket Pal
provides quantitative log analysis methods suitable for use by most
geologists, engineers, and geophysicists who need to perform quick,
complete, and accurate calculations of reservoir properties. The
formulas presented are simple but adequate for all but the most
detailed work. Usage rules for each method are described, based on
the log suite available and the rock/fluid mixture expected. More
complex methods are contained in
Crain’s Petrophysical Handbook,
the “big brother” to the Pocket Pal.
Although
visual analysis, crossplots, and log overlay techniques have been
widely used, this handbook provides a step by step numerical method
which has worked reliably in most formations in many parts of the
world. This computational approach minimizes the risk of bypassing
lower quality zones, and improves your ability to estimate the
quality of a zone. Finding zones of interest on a long log does
require some form of visual scanning. This topic is covered in
Section 3.00,
after we review the details of our log analysis model.
1.01
What Is A Log
A log is a record of something versus time or distance, such as a
Ship’s Log or a travelog. In oil and gas wells, a log is a
recording versus depth of physical or chemical properties of the
rocks and fluids penetrated by drilling the well.

FIGURE PP1.01: Recording a wireline log at a well site
The logs
we usually think of are wireline logs run in open or cased hole, or
logs run near the drill bit while drilling. Sample and core
descriptions, core analysis results, as well as drill stem test and
production test results are all forms of well logs.
Wireline
logs are created by remote sensing equipment lowered into a hole
drilled with a rotary or percussion drilling rig. Cased hole logs
are run after the well is cased to assess the current state of the
reservoir, to check the mechanical integrity of the casing, tubing,
or cement, and to monitor fluid flow. Logging while drilling (LWD)
provides many measurements similar to open hole wireline logs and
are used in the same way as open hole logs.
Logs
are created at the well site by a crew specially trained for this
job. The equipment is highly specialized and expensive. A typical
setup is shown in the illustration above.
FIGURE
PP1.02: A Typical Log
The data
is recorded, processed, and displayed by the logging service company
with a specially designed computer graphics system. Here the data is
transformed from the actual measurements into values we can use for
analysis of the rocks and fluids traversed by the log. This
pre-computation step reduces our labor, but introduces assumptions
and procedures over which we have little control.
At right
is a typical log, illustrating the standard three track presentation
with numerous curves, or log traces, in each track and the usual log
header, or scale insert, at the top. The analyst must become
competent in reading, or picking, log values from these curves. This
involves choosing the correct curve and scale combination,
recognizing bed boundaries, and picking log curve values that
appropriately represent the properties of the rocks.
Unfortunately, logs seldom measure directly what we want to know,
like flow capacity or oil volume in place. Therefore, we have to
analyze the values we can measure, and convert them into answers
which will help us determine the quality of a hydrocarbon reservoir.
To do this, the chosen data is put into equations, using charts,
calculators, or computers, to obtain the answers we need.
Logs usually available to the analyst on modern
wells
1. shallow, medium, and
deep resistivity with spontaneous potential (SP) and/or gamma
ray (GR)
2. sonic travel time with GR and caliper
3. density and neutron porosity with GR and caliper, and
photoelectric effect (PE) on newer wells
4. auxiliary logs such as microlog, dipmeter, gamma ray
spectralog, formation microscanner, borehole televiewer, full
wave acoustic, electromagnetic propagation, nuclear magnetic
resonance, ......
The
basic results, or answers, we need from analysis of logs are
porosity, water saturation, and permeability, as well as sums and
averages of these values. The results are called petrophysical
properties or reservoir properties. Geologists, geophysicists,
engineers, managers, and shareholders are all interested in these
quantities. When transformed into productivity and reserves, the
answers become more meaningful to non-professionals.
1.02
Organizing Your Work
The
logical, step by step procedures presented here are simple and
straight forward, and can be used by anyone with a modest knowledge
of logs and reservoir geology.
The analysis style offered prevents circular reasoning, provides
cross-checks of all major steps, assures completeness, and also
significantly reduces labor. Following these steps does not
guarantee a successful log analysis, but does offer the closest
approximation possible.
Quantitative log analysis is mostly a matter of data reduction to
obtain answers that are more manageable than the plethora of raw
data. This process is followed by interpretation of the answers to
obtain an understanding of the rocks and fluids. The concept is
illustrated in Figure PP1.03. You should note the distinction
between LOG ANALYSIS (data reduction to get answers) and LOG
INTERPRETATION (understanding the answers) that is made here.
Analysis
is based on a mathematical model called the Log Response Equation.
It is determined by the complex mixture of rock minerals and fluids
seen by the logging tools.
The most
rational calculation sequence is shown in the test box above. This
sequence has proved itself over the years, and is the most straight
forward solution to a very complex problem. In many cases the
lithology calculation is done concurrently with, or before, the
porosity calculation, but the topics are discussed in the order
shown. Economic calculations usually follow these steps, and are
covered in
Section 11.02.

FIGURE PP1.03: Data reduction
and interpretation are separate entities
There
are many available methods for each calculation step. The analyst
must choose the appropriate method from those presented for each of
the topics. Recommended usage rules for each method are given, and
depend to a large degree on the available log data and the
rock/fluid mixture in the zone being analyzed. These rules may need
to be adjusted to suit local conditions. Rules for calibrating
results to ground truth are also given.
In the
classroom or when starting work in a new area, you may want to try
several methods, and see which matches core porosity the best. In an
office environment, there is seldom enough time to try all methods
on all zones. Unfortunately there is no standard logging program, so
there is no single foolproof log analysis method.
For
fast, practical analysis, pre-programmed methods for the calculator
or computer are essential. The formulas provided in the following
sections are "computer-ready" - if your calculator has round
brackets, ( ), you can enter the equations just as they are printed.
They do not need translation or modification and can be used in
virtually all algebraic style calculators or any calculator or
computer using Basic or Fortran. “Computer-ready” code may make the
equations a little harder to read, but they are a lot easier to
use.
A
shareware spreadsheet called META/ESP, using identical math to that
contained in this Handbook, us available from the downloads tab at
www.spec2000.net .
Although
a calculator or computer is considered essential to reduce labor and
to improve accuracy, charts are available from logging service
companies for some methods. Unfortunately, most chartbook solutions
ignore shale effects, so results are often inaccurate. Computer
program and spreadsheet solutions to these equations are also widely
used and are commercially available. However, you should be familiar
with hand calculator methods for jobs where no computer is available
and to understand how different parameters influence computer
derived results,
1.03
Calculators and the Math Hierarchy
For consistency, the mathematical notation in this handbook is that
used in many computer languages. This notation is easily translated
into Basic, Fortran, spreadsheet programs, or programmable
calculators. In any case, you must obey the rules of mathematics, in
particular the mathematical hierarchy.
Calculations are performed in a specific order by all mathematicians
and all computers. Analysts using hand calculators or pencil and
paper are obligated to use the same system or will get erroneous
results. The order of the operations is called the mathematical
hierarchy, and is defined as follows:
Highest Priority
( ) brackets
^, exp
*, /, mod
+, -
relational operators
(= , >, <, < =, > =, #)
not
and
or, xor
min, max, sum
Lowest Priority
Operations at the highest priority are performed first, followed by
the next lowest, and so on. If more than one type of operation is
shown at one priority level, they are evaluated from left to right
as found in the equation. The object of the hierarchy is to reduce
the number of brackets needed to indicate the order of calculation.
EXAMPLES:
A = B +
C * D means multiply C by D then add to B
A = B *
C ^ D means take C to the power D then multiply by B
A = (B
+ C) ^ 2 * D means add B and C, square it, then multiply by D
WARNING: YOU
MUST OBEY THE MATH HIERARCHY or your answers will be WRONG.
2.00
The Step By Step Procedure
Log
analysis involves a series of logical steps, each necessary to
proceed to the next step. Like an athlete running to win the 100
meter sprint, log analysis requires training, planning, focus, and
concentration before the race starts. At race time, we proceed to
the starting line, get Ready, Set, Go, and Finish. Then we critique
the results – did we win or finish last?
CRAIN’S STEP LADDER TO SUCCESS
A. Prepare For
The Race:
1. Learn and understand the methods and their limitations
2. Plan your approach to this project
3. Focus on the results required
4. Concentrate on the important issues, reduce the noise
B. Get Ready:
1. Review local well histories and regional geologic
information
2. Correlate offset logs and pick formation tops
3. Mark all known data on logs or data sheet
4. Edit the logs
C. Get Set:
1. Find clean zones and shale zones
2. Pick shale base lines on all logs
3. Find porous zones that are fairly clean
4. Find obvious water zones, if any
5. Look for hydrocarbon indications
6. Identify coal or salt beds
7. Identify the matrix rock from the log response
8. Look for signs of permeability
9. Estimate depositional environment
10. Check for indications of fractures
D. Go:
1. Subdivide cleaner zones into horizontal layers
2. Pick log values in each layer
3. Choose computation method
4. Calculate results
E. Finish:
1. Check results against samples, cores, and tests
2. Rework problem areas
3. Think to a conclusion - IS THE ZONE ANY GOOD?
4. Write a report, present results and conclusions
F. Critique
Your Work:
1. Could the job be better organized or simplified?
2. Did the results satisfy the end-user?
3. What else is needed (data, tools, time) to do a better job?
Log
analysis also may be circular, or at least iterative, since the
results from each step can often be compared to other sources of
data and corrected if differences are found.
This
list looks pretty imposing, and a few steps might be skipped from
time to time, but a consistent, step by step procedure will produce
more reliable results. It tends to remove some of the mystery
involved in log analysis, and reduces effort in the long run. You
might consider the procedure to be a "Step Ladder to Success".
Unfortunately, you may have to climb the ladder more than once if
log analysis results do not compare to ground truth, such as core
analysis, sample descriptions, or test results.
Review
the available data before embarking on detailed analysis. Locate the
well history files or well history cards, look at offset logs,
review sample descriptions, formation tops, tests, cores, and
production histories, and possibly structural or isopach maps of the
target formations. Known gas-oil and oil-water contacts must be
noted. If seismic maps or cross sections are available, review these
as well.
On deep,
remote, or offshore wells, a number of logs may be recorded while
drilling, such as mud and hydrocarbon logs, or even gamma ray,
resistivity, or other quantitative log curves. These should be added
to the "Hopper of Knowledge".
Remember, however, that data from a new well may overturn all
previous analysis results on older wells. Thus, some critical
assessment of the old data is required in addition to that usually
accorded the new data.
A data
retrieval from a computer data base may reduce the labor in locating
much of the needed information. Both commercial and in-house
databases exist and appropriate software is available for most
personal computers and workstations.
2.01
The Analysis Model
Quantitative log analysis is based on a series of mathematical
formulas, or models, derived from the experience of many analysts.
Thus, literally thousands of methods exist. The most universal
applications have been assembled in this handbook. Only a very few
of the equations are original to the author.
The Log
Analysis Model takes into account two distinct problems:
1. Invasion of the formation
by drilling mud filtrate.
2. The complex mixture of rock types and fluids that comprise
the formation.
Invasion
is a process whereby drilling mud fluid is forced into the rock due
to differential pressure. The drilling mud is made up of solid
particles and ions dissolved in water. This water displaces the
native formation water to some degree, and mixes with formation
water that is not displaced. The distance to which some displacement
and/or mixing occurs is called the invasion diameter, and the zone
so disturbed is termed the invaded zone.
The zone
nearest the borehole, or flushed zone, is the portion of rock where
the maximum amount of displacement and mixing has occurred. The
balance of the invaded zone is named the transition zone, where the
transition between maximum flushing and no invasion occurs. These
definitions are illustrated schematically in Figure PP2.04.
The
invasion process leaves behind the solid particles of the mud, which
collect on the borehole wall. The resulting material is called
mudcake, and may be anywhere from 3 inches thick to very thin and
difficult to detect. The mudcake thickness by definition, is one
half the difference between the bit size and the borehole diameter.
If the hole is enlarged by erosion beyond the
bit size
during drilling, the mudcake thickness may be impossible to
determine.
Mudcake
is the sealing agent which slows down invasion. As a result, high
permeability zones which allow quick buildup of mudcake, invade the
least, and low permeability zones invade the most or deepest.
Non-permeable zones are not invaded. Since the mudcake is scraped
off each time a drill pipe joint or the bit passes a formation,
invasion of shallow zones may be repeated many times with many
different fluids, thus making such zones difficult or impossible to
analyze.

Figure PP2.04: The drilling
fluid invasion model
Since
the depth of investigation of logging tools varies, knowledge of the
invasion profile is necessary in making assumptions about log
analysis methods or parameters. Resistivity distribution in a radial
direction from the borehole is determined by the invasion profile.
The resistivity log reading in the formation depends on the response
field of the logging tool and varies with the design of each tool.
Resistivity logs which measure different depths into the rock can be
used to estimate the invasion profile. Results are used to judge the
reliability of resistivity data, and to correct the log readings for
the effects of invasion.
For
example, if the ratio of the deep to medium resistivity log values
is between 0.8 and 1.2, invasion effects are minimal and no
correction to the deep resistivity is made. If the ratio falls
outside this range, corrections should be applied using the
appropriate service company "Tornado Chart". These charts are ONLY
useful in water zones – they do VERY BAD THINGS in hydrocarbon
zones.
Sonic,
density, neutron, gamma ray, and spontaneous potential logs see the
invaded zone and are thus influenced by those fluids. Most
mathematical models include terms which account for invasion of mud
filtrate into oil or water zones, but special models are needed for
gas zones. These are noted as special cases in subsequent sections
of this handbook.
2.02
The Formation Rock Model
All log analysis methods are based on a uniform, industry accepted
model of the reservoir rocks and fluids.

IGURE PP 2.05: The Formation Rock/Fluid Model for Log Analysis
Here are the
definitions that derive from the rock/fluid model shown above.
DFN
1: The
formation rock/fluid model is comprised of:
- the matrix
rock (Vrock)
- the
pore space (or porosity) within the matrix rock (PHIe)
- the shale
content of the matrix rock (Vsh)
By
definition, Vrock + PHIe + Vsh = 1.00
DFN 2:
The matrix rock component (Vrock) can be subdivided into two or more
constituents (Vmin1, Vmin2, ….), such as:
- limestone,
dolomite, and anhydrite or
- quartz,
calcite cement, and glauconite
The mineral
mixture can be quite complex and log analysis may not resolve all
constituents.
DFN 3:
The shale component (Vsh) can be classified further into:
- one or
more clays (Vcl1, Vcl2, …)
- silt
(Vsilt)
- water
trapped into the shale matrix due to lack of sufficient permeability
to allow the water to
escape
- water
locked onto the surface of the clay minerals
- water
absorbed chemically into the molecules of the clay minerals
The sum of
the three water volumes is called clay bound water (CBW). CBW varies
with shale volume and is zero when Vsh = 0.
By
definition, Vsh = Vcl + Vsilt + CBW
DFN 4:
Bulk volume water of shale (BVWSH) is the sum of the three water
volumes listed above in the definition of shale and is determined in
a zone that is considered to be 100% shale.
By
Definition, CBW = BVWSH * Vsh
DFN 5:
Total porosity (PHIt) is the sum of:
- clay bound
water (CBW)
- free
water, including irreducible water (BVW)
- hydrocarbon (BVH)
DFN
6:
Effective porosity (PHIe) is the sum of:
- free
water, including irreducible water (BVW)
-
hydrocarbon (BVH)
DFN
7:
Effective porosity is the porosity of the reservoir rock, excluding
clay bound water (CBW).
PHIe = PHIt –
CBW
OR PHIe = PHIt – Vsh * BVWSH
Some of the
“free water” is not free to move - it is, however, not “bound” to
the shale.
DFN 8:
Free water (BVW) is further subdivided into:
- a mobile
portion free to flow out of the reservoir (BVWm)
- an
immobile or irreducible water volume bound to the matrix rock by
surface tension (BVI or
BVWir)
BVI is
sometimes called “bound water”, but this is confusing (see
definition of clay bound water above), so “irreducible water” is a
better term. Note that BVWm = BVW – BVI.
DFN 9:
Hydrocarbon volume (BVH) can be classified into:
- mobile
hydrocarbon (BVHm)
- residual
hydrocarbon (BVHr)
DFN 10:
Free fluid index (FFI) is the sum of BVWm, BVHm, and BVHr. It is
also called moveable fluid (BVM) or useful porosity (PHIuse).
PHIuse = BVM
= FFI = BVWm + BVHm + BVHr
OR PHIuse = PHIe – BVI
OR PHIuse = PHIe * (1 – SWir)
This
definition is needed for the nuclear magnetic log (NMR, CMR, etc),
since it cannot see BVWir. Non-useful porosity also occurs as tiny
pores that do not connect to any other pores. They are almost
invariably filled with immoveable water and do not contribute to
useful reservoir volume or energy. Such pores occur in silt,
volcanic rock fragments in sandstones, and in micritic, vuggy, or
skeletal carbonates. The NMR may see some of this non-useful
porosity – the jury is still out.
DFN 11:
Total water saturation (SWt) is the ratio of:
- total
water volume (BVW + CBW) to
- total
porosity (PHIt)
SWt = (BVW + CBW) / PHIt
DFN 12:
Effective water saturation (Sw) is the ratio of:
- free water
volume (BVW) to
- effective
porosity (PHIe)
Sw = BVW /
PHIe
This is the
standard definition of “water saturation”. Older books use this term
to define total water saturation. Since all interpretation methods
described here correct for the effects of shale, we are not normally
interested in the total water saturation, except as a mathematical
by-product. As effective porosity approaches zero, the water
saturation approaches one (by edict, if not by calculus).
DFN 13:
Useful water saturation (SWuse) is the ratio of:
-
useful water volume (BVW - BVI) to
- useful
porosity (PHIuse)
SWuse = (BVW – BVI) / PHIuse
DFN 14:
Irreducible water saturation (SWir) is the ratio of:
- immobile
or irreducible water volume (BVI) to
- effective
porosity (PHIe)
SWir = BVI / PHIe
DFN 15:
Residual oil saturation (Sor) is the ratio of:
- immobile
oil volume (BVHr) to
- effective
porosity (PHIe)
Sor = BVHr / PHIe
DFN 16:
The water saturation in the flushed zone (Sxo) is the ratio of :
- free water
in the flushed zone, to
- effective
porosity, which is assumed to be the same porosity as in the
uninvaded zone.
The amount of
free water in the invaded zone is usually higher than in the
uninvaded zone, when oil or gas is present. Thus Sxo >= Sw. The
water saturation in the invaded zone between the flushed and
uninvaded zone is seldom used.
DFN 17:
Further constraints that should be remembered are:
PHIt >= PHIe >= PHIuse
SWt >= Sw >= SWuse.
PHIt = PHIe when Vsh = 0
SWt = Sw when Vsh = 0
All volumes
defined above are in fractional units. In tables or reports, log
analysis results are often converted to percentages by multiplying
fractional units by 100.
2.03 The Log Response Equation
The response of an individual log to the model described above is
defined by the Log Response Equation, which takes the form:
THE LOG RESPONSE EQUATION
LOG =
PHIe * Sxo * Lw (water
term)
+ PHIe * (1
– Sxo) * Lh (hydrocarbon term)
+ Vsh * Lsh
(shale term)
+ (1 – Vsh –
PHIe) * Lma) (matrix term)
WHERE: Lh = log reading in 100% hydrocarbon
Lma = log reading in 100% matrix rock
LOG = log reading
Lsh = log reading in 100% shale
Lw = log reading in 100% water
PHIe = effective porosity (fractional)
Sxo = water saturation in invaded zone (fractional)
Vsh = volume of shale (fractional)
This response
equation will work for sonic travel time, density, or density
porosity, neutron porosity, gamma ray (and the spectrolog curves -
uranium, thorium and potassium), resistivity (if Sxo is replaced by
Sw for deep resistivity logs), the electromagnetic propagation log,
the thermal decay time log, and the photoelectric effect (if PE *
DENS is used). It will also work for various derived logs described
in later chapters of this handbook.
The response
equations can be used in several ways. One is to find out what a log
would read under a hypothetical set of circumstances. This is called
forward modeling of log response, and is used to generate synthetic
logs or to verify log analysis results. If the reconstructed log
doesn’t match the recorded log, then something in the analysis model
is wrong and must be fixed.
Another way
is to calculate one unknown in the equation, for example porosity or
shale volume, by using a log reading and assuming the other terms to
be known or derivable from some other response equations. A third
approach is to use sets of response equations simultaneously to
determine as many unknowns as possible from the available log data.
Some terms in
the response equation for certain logs go to zero. This is what
makes it possible, for example, to calculate the shale volume from
the gamma ray response. Both the water and hydrocarbon terms go to
zero, since neither of these components has any gamma ray
contribution. By re-arranging terms and further assuming that
porosity is small, we get:
The Gamma Ray Response Equation Solved for Shale Volume
VSHgr = (GRlog – GRmatrix) / (GRshale – GRmatrix)
Here GRlog,
GRshale, and GRmatrix are read from appropriate places on the gamma
ray log to calculate shale volume.
In other cases,
we sometimes lump two terms together, as for water and oil in the
sonic log equation for porosity. This strategy eliminates the need
to know water saturation prior to knowing porosity. This approach
will fail if gas is present because the water and gas contributions
are too dissimilar. The algorithms in following chapters attempt to
resolve as many of the unknowns as possible using these piecewise
techniques. Where this is inappropriate, sets of two or three
simultaneous equations are solved, with the final solution being
given. It will not always be obvious that simultaneous response
equations were used, but ALL log analysis methods rely on this
approach. What we have done here is eliminate the repetitive
derivation of the solution, and present instead the finished
product, ready for inclusion in a calculator or computer program.
The borehole
environment, invasion, and rock model define the log analysis
problem. Logging tools define most of the data available to analyze
the model. With many analysis methods to choose from, there are
usually many possible answers. It is the analyst's job to select the
method and model that best describe the problem to be solved.
Adjustments to the basic model presented here are therefore
plausible, and may be essential.
Calibration
of log analysis results to “ground truth” is a normal step in
checking your work, modifying parameters, or choosing alternate
mathematical models..
2.04
Using The Log Response Equation – Seismic Modeling
The usual petrophysical application of the log response equation is
to solve for shale volume, porosity, lithology, and water saturation
from well log data recorded in open or cased holes. This is called
inverse modeling, or more simply, plain ordinary “log analysis”.
A common log analysis calculation is to calculate
apparent porosity from density and sonic logs, as here:
1: PHID = (DENSMA – DENS) / (DENSMA – DENSW)
2: PHIS = (DELTMA – DELT) / (DELTMA – DELTW)
WHERE: PHI = total porosity (including any clay bound water), DENS =
density log values, DELT = sonic log values, and the subscripts MA
and W represent values for matrix rock and water respectively.
These equations are very widely used in the industry,
but cause many problems because the shale term in the response
equation is missing, and the choice of matrix rock values are often
poorly selected. Log analysis methods described in this Handbook
will show you how to use the response equation correctly, in order
to handle these two concerns.
An alternate use is to calculate what a log should have read. By
using the log response equation in this forward model, we can
reconstruct bad logs – logs that failed due to bad hole condition or
other problems. We could also create a synthetic log to replace a
missing log curve. All we need is a satisfying log analysis result
from the good log curves and, from this, calculate the missing or
faulty data. Many modern log analysis software packages have this
capability for editing and repair of logs.
Be careful to use flushed zone water saturation (Sxo)
while creating these synthetic logs.
Geophysicists have a similar but subtly different
application. They need to reconstruct the logs for bad hole and
missing data, but they also need to replace the invaded zone fluids
with the native reservoir fluids. Since the seismic signal sees
uninvaded reservoir properties, there is not much sense using
invaded zone log data to calibrate seismic sections, seismic
inversions, or offset versus amplitude interpretations. The problem
is most serious in shallow gas sands, but may be important in
thicker light oil zones as well. The process of correcting for
invasion is called “fluid replacement editing”.
The important but subtle difference between
petrophysical log modeling and geophysical log modeling is that the
geophysical model needs the actual water saturation (Sw) instead of
the flushed zone saturation (Sxo).
Another use of forward modeling is to create
hypothetical logs, sometimes called “rock replacement editing”.
Sometimes this can be done by cut and paste of existing log data,
for example thinning out a reservoir to a pinchout or adding a reef
to a known geological sequence. Other hypothetical models merely
change a water bearing reservoir to a gas or oil zone, or change the
porosity or shale volume, to see “what if?” scenarios.
The
log response equation is the best way to do fluid or lithology
replacement. A spreadsheet to perform this math, called META/MODL,
is available from the Downloads tab at
www.spec2000.net
.
1. Density Log Response
The response of
a density log can be described rigorously by a volume weighted
summation of the densities of the individual components in the rock.
The usual form of this equation is:
0: DENS = Sum (DENSi *
Vi)
The
expansion for well logging situations is:
1: DENSmod = PHIe * Sw
* DENSW
+ PHIe * (1 - Sw) * DENSHY
+ Vsh * DENSSH
+ (1 - Vsh - PHIe) * DENSMA
FIGURE
PP2.06: Density of gas at reservoir conditions – default
approximation
This
equation can be used to calculate what a density log would read
given a hypothetical rock/fluid mixture, thus modeling of various
formation alternatives is a straight forward mathematical process.
It is preferable to guessing or estimating from previous experience.
This equation is rigorous and can be used with real hydrocarbon
densities based on the temperature, pressure, and phase relationship
of the fluid in question. A chart showing approximate gas density
versus depth is shown in Figure PP2.06, based on average pressure
and temperature data for the western Canadian basin. No correction
for vuggy porosity is needed.
Corrections for the fact that density logs respond to electron
density, and not bulk density, can be made, and may be necessary
especially in the case of coal or salt beds. We usually do not make
these corrections, because the accuracy needed for computing seismic
response does not warrant the effort.
2. Sonic Log Response
An equation
similar to that for density can be generated for sound velocity of
mixtures. However, it is a summation of travel time weighted by
volume and not a summation of velocity components:
0: DELT = Sum (DELTi * Vi)
This
is called the Wyllie time average equation and is true for many
situations where the components are not very compressible, such as
water, sandstone, and shale. It does not work too well with gas
under low pressure. It is an empirical relationship and is not
rigorous. However, the Biot model for sound velocity in mixtures is
rigorous, and reduces to Wyllie's equation in most situations (ie:
compressibility is very
low).
The
expansion of this formula for log analysis parallels the density
formula:
1: DELTmod = PHIe * Sw
* DELTW
+
PHIe * (1 - Sw) * DELTHY
+ Vsh * DELTSH
+ (1 - Vsh - PHIe) * DELTMA
FIGURE
PP2.07: Sonic “pseudo” travel time in gas at reservoir conditions –
default approximation
The
Wyllie equation provides the opportunity to compute the sonic travel
time (and the seismic velocity) of any hypothetical formation by
describing the quantity of rock matrix, shale, water, and
hydrocarbon. The equation works for either compressional or shear
waves, as long as the appropriate fluid and rock properties are
used.
The
relationship is usually not true when gas fills the pore space, or
is even a small fraction of the pore space. For this reason, we use
a "pseudo-travel-time" in gas zones to reaffirm that it represents a
velocity which may not be the same as the velocity of the gas at the
temperature and pressure of the formation.
The
hydrocarbon "pseudo-travel-time" is derived empirically by comparing
results from synthetic seismograms and properly processed field
data. A very rough approximation of hydrocarbon "pseudo-travel-time"
versus depth, which has given reasonable results in the western
Canadian basin, is shown in Figure PP2.07.
Proper editing of density and sonic data for fluid replacement and
bad hole condition is an absolute prerequisite before using the log
for any seismic application. Appropriate values for water, oil, and
matrix rock are found in sections
5.02
and
5.01
of this Handbook.
2.05
Integration – Calibrating to Ground Truth
All log
analysis methods depend on numerous assumptions made by the analyst
and on parameters derived by observation or statistical analysis of
the available log data. Assumptions and parameters may be adjusted
by comparing log analysis results to “ground truth”, such as sample
descriptions, core analyses, well tests, and production histories
from the zone of interest in the current well or in offset wells.
This is called “Integrated Petrophysics” when all sources of data
are combined to obtain a clear reservoir description.
The coarsest
log available is merely a list of formation names and their top
depths from a well history file. The formation names are often clues
to their basic lithology. For example, the Halfway Sand, Leduc Reef,
Austin Chalk, Ardlee Coal, Delaware Shale suggest a lot, even to a
novice. In time, we “know” that the Rex and Sparky are sandstones,
and the Doig and Charlie Lake formations are mostly dolomite.
Sample
descriptions provide the basic framework for developing a model of
the formations to be analyzed. The primary sedimentary rocks
(sandstone, limestone, dolomite, anhydrite, shale, salt, coal) and
accessory minerals (calcite, siderite, glauconite, pyrite, etc.) are
usually described in some detail, in words or as a descriptive log.
Visual porosity, hydrocarbon shows, fluorescence, porosity type,
rock texture, and layer boundaries give the petrophysicist valuable
insights into what to expect from analysis results.
Sample
descriptions are provided at a coarse sample rate of 1 to 10 meters,
so there is some need to exercise good judgment when comparing logs
to samples. Samples may be contaminated by cavings from above the
current sample depth. Core descriptions are also used, but here the
depth increment of the data is finer than the log resolution.
Core analysis
porosity and permeability are used directly to calibrate
petrophysical results. The finer sample rate needs to be considered,
but a good log analysis should match the core data, within reason.
Bear in mind that the core analysis is performed on a piece of rock
the size of a soda-pop can (whole core) or the size of a pill bottle
(core plugs or sidewall cores). Logs see a piece of rock the size of
a 45 gallon barrel.
Special core
data, such as capillary pressure relative permeability, and
electrical properties measurements are used to calibrate water
saturation calculations from logs.
Gas logs,
sometimes called mud logs or measurements while drilling (MWD),
record gas shows in the drilling mud. Good shows on this log
sometimes indicate a hydrocarbon bearing interval that ought to be
visible on the log analysis results. Gas shows in the mud are not
very quantitative indicators so there are many false-positive and
false-negative indications.
The driller’s
log is often combined with the gas and sample description logs. It
shows rate of penetration, weight on bit, torque, and drilling mud
properties. Lost circulation zones are noted here. All of this
“stuff” can help untangle difficult interpretations or narrow the
focus to specific zones of interest.
Drill stem
tests (DST), run in open hole either before or after logging, may
assist in predicting production characteristics. Many tests fail to
produce anything, so log analysis shows may be completed, even in
the face of a negative test result. If a test produces water or
hydrocarbons, it is usual to see the same prediction on the log
analysis. However, formation damage, natural fractures, and depth
control problems may give a false show that cannot be confirmed by
the log analysis. Production tests through casing are also aids to
log analysis calibration – it is always nice to have a good
hydrocarbon show on the logs when the test makes oil-to-surface!
Production
history data shows the rates and cumulative values for oil, gas, and
water, giving a view of how these change over time. If productivity
predictions are made from petrophysical analysis, they can be
loosely calibrated to the first 90 or 120 days of production.
Petrographic
data from thin section photography, X-ray diffraction, scanning
electron microscopy, and other petrology methods are used to
understand pore geometry, diagenetic history, and mineralogy. This
can often explain differences in interpretation between test
results, core data, and log data.
Where this
data is available, it is provided as part of the Case Histories and
Exercises in this Handbook.
3.00
Eyeball Analysis Of Logs – Crain’s Simplified Rules
You should know the basic rules for eyeball analysis of log curves
to help you climb the “Ladder to Success”. The common rules are
described below with reference to Figures PP3.06A through PP3.06D. A
more elaborate set of rules follows in Section 3.01. Lets start the
race.
GET READY: SEE
WHAT YOU HAVE

FIGURE PP3.06A: Raw logs for
Shaly Sand Example
The left
half of this image shows a resistivity log with spontaneous
potential (SP) in Track 1 and shallow, medium, and deep resistivity
(RESS, RESM, RESD) on a logarithmic track to the right of the depth
track. The right half of the image shows a density neutron log with
gamma ray (GR) and caliper (CAL) in Track 1. Photo electric effect
(PE) is in Track 2 with neutron porosity (PHIN) and density porosity
(PHID) spread across Tracks 2 and 3.
Crain’s Rule # Minus 1:
Identify log curves available, and determine their scales.
GET SET: FIND
SHALE VOLUME

FIGURE PP3.06B: Raw logs
showing shale baselines
To find
clean zones versus shale zones, examine the spontaneous potential
(SP) response, gamma ray (GR) response, and density neutron
separation. Low values of GR, highly negative values of SP, or
density neutron curves falling close to each other usually indicate
low shale volume. High GR values, no SP deflection, or large
separation on density neutron curves normally indicate high shale
volume.
On
Figure PP3.06B, shale base lines and clean sand lines are drawn on
the SP and GR curves. Shale base lines can be drawn on RESD, PE,
PHIN, and PHID curves as well. This allows us to define shale beds,
clean (non-shaly) reservoirs, and shaly sands.
Crain’s Rule #0:
Gamma ray or SP deflections to the left indicate cleaner sands,
deflections to the right are shaly. Draw clean and shale lines,
then interpolate linearly between clean and shale lines to
visually estimate Shale Volume (Vsh).
Very
shaly beds are not “Zones of Interest”. Everything else, including
very shaly sands (Vsh < 0.50) and even obvious water zones, are
interesting. Although a zone may be water bearing, it is still a
useful source of log analysis information, and is still a zone of
interest at this stage.
GO: ESTIMATE
POROSITY

FIGURE PP3.06C: Raw logs
showing bed boundaries for “Interesting Zones”
For
zones of interest, draw bed boundaries (horizontal lines). Then
review the porosity logs: sonic, density, and neutron. All porosity
logs deflect to the left for increased porosity. If density neutron
data is available, estimate porosity in clean sands by averaging the
two log values.
In shaly
sands, read the density porosity. IMPORTANT: This is just an
estimate and not a final answer. Scale the sonic log based on the
assumed matrix lithology. Mark coal and salt beds, which appear to
have high apparent porosity. Identify zones which show high medium,
low, or no porosity. Low porosity, high shale content, coal, and
salt beds are no longer interesting.
Crain’s Rule #1:
The average of density and neutron porosity in a clean zone
(regardless of mineralogy) is a good first estimate for
Effective Porosity (PHIe).
Crain’s Rule #2:
The density porosity in a shaly sand is a good first estimate
for Effective Porosity (PHIe), provided logs are on Sandstone
Units.
GO
FURTHER: FIND HYDROCARBON ZONES

FIGURE PP3.06D: Raw logs
showing resistivity porosity overlay
To find
hydrocarbon indications and obvious water zones, compare deep
resistivity to porosity, by mentally or physically overlaying the
density porosity on top of the resistivity log. High porosity
(deflections on the density log to the left) and high resistivity
(deflections to the right) usually indicate oil or gas, or fresh
water. See cross-hatched area on resistivity track of Figure
PP3.06C.
Crain’s Rule #3:
Tracking of porosity with resistivity on an overlay usually
indicates water or shale.
OR
Low
resistivity with moderate to high porosity usually undicates
water or shale.
Crain’s Rule #4:
Crossover of porosity on a resistivity log overlay usually
indicates hydrocarbons.
OR
High
resistivity with moderate to high porosity usually undicates
hydrocarbons.
Zone A
on Figure PP3.06 is a shaly sand and has medium porosity. Zone C is
a clean sand and has high porosity. Zones B and D are shale with no
useful porosity.
The
average of density and neutron porosity in Zone C is 24 %. This is
close to the final answer because there is not much shale in the
zone. The average in Zone A is 16 % - much higher than the truth due
to the influence of the shale in the zone. The density porosity is
about 11%, pretty close to the core data. Therefore all our analysis
must make use of shale correction methods.
Low
resistivity and high porosity usually means water, as in the bottom
half of Zone C. Known DST, production, or mud log indications of oil
or gas are helpful indicators.
The top
half of Zone C and all of Zone A show crossover when the porosity is
traced on the resistivity log, so these zones remain interesting. In
fresher water formations, it is often difficult or impossible to
spot hydrocarbons visually. If it was easy, log analysts would be
out of work!
Crossover on the density neutron log usually means gas. Watch for
rough hole problems, sandstone recorded on a limestone scale, or
limestone recorded on a dolomite scale, which can also show
crossover – not caused by gas.
Water
zones with high porosity and low resistivity are called “obvious
water zones”. Fresh water may look like hydrocarbons, particularly
in shallow zones. The lack of SP development will often help
distinguish fresh water zones. Low porosity water zones may not be
obvious.
KEEP GOING:
ESTIMATE WATER SATURATION
Water
saturation is usually calculated from the Archie equation or a shale
corrected version of it. This is not easy to do with mental
arithmetic. An easier estimate of water saturation can be made in
obvious hydrocarbon zones by using a method attributed to Buckles,
and it is commonly used by reservoir engineers in a hurry.
Crain’s Rule #5:
Approximate Water Saturation (SWa) in an obvious hydrocarbon
zone is estimated from: SWa = Constant / PHIe
where
Constant is in the range from 0.0100 to 0.0800. Use 0.0400 as a
first try .
IT”S A LONG
RACE: ESTIMATE LITHOLOGY
Visual
determination of lithology (in addition to identifying shale as
discussed earlier) is done by noting the quantity of density neutron
separation and/or by noting absolute values of the photo electric
curve. The rules take a little memory work.
You must
know whether the density neutron log is recorded on Sandstone,
Limestone, or Dolomite porosity scales, before you apply Crain’s
Rule #5. The porosity scale on the log is a function of choices made
at the time of logging and have nothing to do with the rocks being
logged. Ideally, sand-shale sequences are logged on Sandstone scales
and carbonate sequences on Limestone scales. The real world is far
from ideal, so you could find any porosity scale in any rock
sequence. Take |