CHAPTER
TWENTY-EIGHT:
FRACTURED RESERVOIRS
1
Fracture Identification
Table
of Contents
28.00 Introduction To This Chapter
28.01 Definition of Fractures
28.02 General Methods For Identification Of Fractures
1. Drilling Characteristics
2. Sample Descriptions
3. Inflatable Packers
4. Drill Stem Tests
28.03 Fracture Identification From Core Analysis
28.04 Fracture Identification From Spontaneous
Potential Logs
28.05 Fracture Identification From Caliper Logs
28.06 Fracture Identification From Micro Resistivity
Logs
28.07 Fracture Identification From Dipmeter Logs
28.08 Fracture Identification From Density, Neutron,
and PE Logs
28.09 Fracture Identification From Gamma Ray
Logs
28.10 Fracture Identification From Resistivity
Logs
28.11 Fracture Identification From Temperature
Logs
28.12 Fracture Identification From Sonic Logs
28.13 Fracture Identification From Sonic Waveform
Logs
28.14 Fracture Identification From Formation
Microscanner Logs
28.15 Fracture Identification From Borehole Televiewer
Logs
Case
Histories (These will open in a new page)
28.16 Classic Example
28.17 Austin Chalk Example
28.18 Fractured Shale
28.19 Vertical Fracture in Vertical Hole
28.20 Vertical Fracture in Horizontal Hole
28.21 Overthrust Example
28.22
In Conclusion
28.23 Exercises for Chapter Twenty-Eight
28.24 Bibliography for Chapter Twenty-Eight
Continue to Chapter Twenty-Nine (includes
Fracture Intensity, Porosity, Permeability)
Continue to Chapter Thirty: Dual Porosity
Model for Fractured Reservoirs
Publication
History: This Chapter is an updated version of part of Chapter
Nine of The Log Analysis Handbook - Volume Two, originally self-published
in 1990 as a seminar handout and workbook.
CHAPTER
TWENTY-EIGHT:
FRACTURED
RESERVOIRS
1
Fracture Identification
28.00
Introduction To This Chapter
This Chapter covers fracture location and identification from
conventional open hole logs. Chapter Twenty-Nine
covers straight-forward quantitative and semi-quantitative methods
for evaluating fractured reservoirs. The Dual Porosity Model is
covered in Chapter Thirty. Rock Stress
and Mechanical Properties are the topic for Chapter
Twenty. These four Chapters comprise a mini-course in Fractured
Reservoir Theory and Practice and should be read as a set.
Natural
fractures in reservoir rocks contribute significantly to productivity.
Therefore, it is important to glean every scrap of information
from open hole logs to locate the presence and intensity of fracturing.
This Chapter deals with fracture identification from open hole
logs and calculation of fracture intensity and fracture porosity.
Even
though some modern logs, such as the formation micro-scanner and
televiewer, are the tools of choice for fracture indicators, many
wells lack this data. Thus all known fracture location techniques
are described.
Naturally
fractured reservoirs contain secondary or induced porosity in
addition to their original primary porosity. Induced porosity
is formed by tension or shear stresses causing fractures in a
competent or brittle formation. Fracture porosity is usually very
small. Values between 0.0001 and 0.001 of rock volume are typical
(0.01% to 0.1%). Fracture-related porosity, such as solution porosity
in granite or carbonate reservoirs, may attain much larger values,
but the porosity in the actual fracture is still very small.
Fracture
analysis literature in the 1970’s suggested that fractures
might contribute as much as a few to several percent porosity.
More modern work using fracture aperture calculated from resistivity
micro-scanner logs indicates much lower numbers. To appreciate
this, consider fractures with 1 millimeter aperture spaced 1 meter
apart. This gives a porosity of 0.001 fractional (0.1%). This
is a very large open fracture. Most are only microns in width,
so even 10 fractures of 10 microns each only give 0.0001 fractional
porosity (0.01%).
The
term “secondary porosity” also includes rock-volume
shrinkage due to dolomitization, porosity increase due to solution
or recrystalization, and other geological processes. “Secondary
porosity” should not be confused with “fracture porosity”.
Porosity formed in this way can be determined from modern log
suites without difficulty (see Chapter
Seven), except for porosity formed by fractures, which is
too small to detect with conventional logs.
Fracture
porosity is found accurately only by processing the formation
micro-scanner curves for fracture aperture and fracture frequency
(fracture intensity). All other methods, including the well known
“dual-porosity” model, are extremely inaccurate. These
models either over-estimate fracture porosity by several orders
of magnitude, or cannot be applied because the log data does not
fit the model. All published models are described in this Chapter
and the student or practitioner can decide whether or not to use
them.
The
effect of fracture porosity on reservoir performance, however,
is very large due to its enormous contribution to permeability.
As a result, naturally fractured reservoirs behave differently
than un-fractured reservoirs with similar porosity, due to the
relative high flow capacity of the secondary porosity system.
This provides high initial production rates, which can lead to
extremely optimistic production forecasts and sometimes, economic
failures when the small reservoir volume is not properly taken
into account.
Reservoir
simulation software that accounts for the fracture system is often
termed a “dual porosity” model. While this is strictly
true, it would be better to think of them as “dual permeability”
models, since the fracture permeability fed by the matrix or reservoir
permeability is far more important than the relative storage capacity
of the fractures and matrix porosity. A reservoir with only fracture
porosity is quickly depleted; a decent reservoir in the matrix
rock feeding into fractures will last much longer.
In
order to understand the behavior of naturally fractured reservoirs,
estimates must be made of hydrocarbons-in-place within both the
primary (matrix rock) and secondary (fracture-only) porosity systems.
To do this, we must first be able to detect the existence of fractures.
Therefore, this Chapter covers fracture detection from the usually
available conventional logs, as well as the method used to partition
porosity into primary and fracture components. The effect of this
partitioning on the Archie water saturation equation is also described.
Modern methods for quantifying fracture porosity directly from
micro-scanner logs are also discussed.
28.01
Definition of Fractures
A fracture is a surface along which a loss of cohesion in the
rock texture has taken place. A fracture is sometimes called a
joint and, at the surface, are expressed as cracks or fissures
in the rocks. Figure 28.01 shows the prominent features of a fracture.
The orientation of the fracture can be anywhere from horizontal
to vertical. The rough surface separates the two faces, giving
rise to fracture porosity. The surfaces touch at points called
asperities. Altered rock surrounds each surface and infilling
minerals may cover part or all of each surface. Minerals may fill
the entire fracture, converting an open fracture to a healed or
sealed fracture.

FIGURE 28.01: Fracture Porosity Definitions
Fractures
are caused by stress in the formation, which in turn usually derives
from tectonic forces such as folds and faults. These are termed
natural fractures, as opposed to induced fractures. Induced fractures
are created by drilling stress or by purposely fracturing a reservoir
by hydraulic pressure from surface equipment (see Chapter
Twenty). Both kinds of fractures are economically important.
Induced fractures may connect the wellbore to natural fractures
that would otherwise not contribute to flow capacity.
Natural
fractures are more common in carbonate rocks than in sandstones.
Some of the best fractured reservoirs are in granite - often referred
to as unconventional reservoirs. Fractures occur in preferential
directions, determined by the direction of regional stress. This
is usually parallel to the direction of nearby faults or folds,
but in the case of overthrust faults, they may be perpendicular
to the fault or there may be two orthogonal directions. Induced
fractures usually have a preferential direction, often perpendicular
to the natural fractures. A schematic diagram of these relationships
is shown in Figure 28.01, bottom right.
A
fracture is often a high permeability path in a low permeability
rock, or it may be filled with a cementing material, such as calcite,
leaving the fracture with no permeability. Thus it is important
to distinguish between open and healed fractures. The total volume
of fractures is often small compared to the total pore volume
of the reservoir.
Most
natural fractures are more or less vertical. Horizontal fracture
may exist for a short distance, propped open by bridging of the
irregular surfaces. Most horizontal fractures, however, are sealed
by overburden pressure. Both horizontal and semi-vertical fractures
can be detected by various logging tools.
The
vertical extent of fractures is often controlled by thin layers
of plastic material, such as shale beds or laminations, or by
weak layers of rock, such as stylolites in carbonate sequences.
The thickness of these beds may be too small to be seen on logs,
so fractures may seem to start and stop for no apparent reason.
To
be an aid in production, fractures must be connected to a reasonable
hydrocarbon bearing reservoir with sufficient volume to warrant
exploitation. If there is no reservoir volume, a lot of fractures
won’t help much unless there is sufficient fracture related
solution porosity to hold an economic reserve. This can be determined
by normal log analysis techniques. In reasonable non-fractured
reservoirs, it is usually possible to estimate permeability, and
hence productivity (see Chapter Ten),
but this is not always possible in fractured reservoirs. Although
both the presence of fractures and the presence of a reservoir
can be determined from logs, a production test will be needed
to determine whether economic production is possible. The test
must be analyzed carefully to avoid over optimistic predictions
based on the flush production rates associated with the fracture
system. Local correlations between fracture intensity observed
on logs and production rate are also used to predict well quality.
Sometimes
the primary reservoir and the fracture system may be so poorly
connected that they are saturated with different fluids. Production
from fractures full of hydrocarbons in a water bearing formation
may initially be very good but very short lived. A more desirable
scenario is a primary reservoir with appreciable hydrocarbon saturation
and a fracture system that is full of water close to the borehole,
showing invasion and hence good permeability, but full of hydrocarbon
in the virgin formation.
This
situation can be recognized with fairly simple log analysis techniques.
Two examples are shown in Figure 28.02. At lower left is a detailed
log of the raw dipmeter curves, showing a conductive streak on
pad one, followed by another on pad 3 as the tool rotates as it
goes up the hole. This is a single simple semi-vertical fracture
filled with conductive drilling fluid in an otherwise non-conducting
rock.
On
the right side of Figure 28.02 is a Laterolog with a shallow resistivity
device (solid curve) showing very conductive streaks on the shallow
curve, not seen by the other curves. This is a good indication
of fractures or washed out borehole, as the crossover would be
the reverse of this in normal porosity. These and other techniques
will be described more fully later in this Chapter.

FIGURE 28.02: Dipmeter and Laterolog conductive streaks indicating
open fractures
28.02
General Methods For Identification Of Fractures
Most well logs respond in some way to the presence of fractures.
Each major log type is discussed in the following sections with
respect to its fracture response. Not all logs detect fractures
in all situations, and very few see all fractures present in the
logged interval. Bear in mind that other borehole and formation
responses will be superimposed on each log. Moreover, it is not
normal to analyze a single log in isolation, but to review all
log curves together to synthesize the best, most coherent, result.
| Logs
used to detect fractures: |
1.
core analysis Section 28.03
2. spontaneous potential Section 28.04
3. caliper Section 28.05
4. micro resistivity Section 28.06
5. dipmeter and fracture identification log Section
28.07
6. density, neutron, and photoelectric effect Section
28.08
7. gamma ray and spectral gamma ray Section 28.09
8. resistivity Section 28.10
9. temperature Section 28.11
10. sonic travel time Section 28.12
11. sonic amplitude, and sonic wave train Section 28.13
12. formation microscanner Section 28.14
13. borehole televiewer Section 28.15 |
|
Because
we are stuck with the existing logs in the well files, this Chapter
covers the assessment of fractures from all these commonly available
logs, even though image logs are usually the tool of choice today.
On new wells in which fractures may be significant, we would run
the correct log suite for fracture identification. Depending on
local experience, this would be one or more of those on the following
list.
Logs
to run today for fractured reservoir evaluation:
1.
Dual laterolog (DLL) or azimuthal resistivity image
(ARI) log with micro-SFLand gamma ray - required for
fracture detection and water saturation, ARIhelpful
for fracture orientation
2. Densityneutron log (CNL-LDT) with photo-electric
effect, gamma ray, and caliper -required for matrix
porosity, lithology, helpful for fracture detection
3. Dipole shear sonic image log (DSI) with gamma ray,
caliper, amplitude, waveform or variable density display
- required for porosity and mechanical properties
calculation, helpful for fracture detection and orientation
4. Natural gamma ray spectral log (NGT) -helpful for
fracture detection, certain areas only, helpful in
granite reservoirs to identify granite type
5. Formation micro-scanner image log (FMI) with gamma
ray plus fracture aperture and frequency post-processing
(FracVue) - strongly recommended, required for quantitative
fracture porosity and permeability, required for fracture
orientation
OR
5A. Ultra-sonic borehole imager (UBI) or televiewer
log with gamma ray plus dipmeter post-processing -
cheaper than micro-scanner but less sensitive, not
quantitative
OR
5B. Stratigraphic high resolution dipmeter (SHDT)
with gamma ray, displayed in fracture identification
mode plus dipmeter post-processing - lowest cost,
not quantitative
|
|
Usually
at least two of these would be run for confirmation, but the microscanner
or televiewer are often sufficient when run alone. Caliper, gamma
ray, porosity, and resistivity logs are usually available as well,
so there is no shortage of data!
There
are a number of mechanical methods for locating fractures, which
will not be discussed further in this Chapter, except for the
brief outline given below. There is extensive literature on the
subject, especially on well testing, which should be referred
to. However, the log analyst needs to be aware of the possibility
and confirmation of fractures from these sources:
1.
Drilling characteristics: occurrence
of lost circulation or mud loss, abrupt drilling breaks, bit bouncing
or torqueing, mud weight reduction, well kicks, oil on the mud
pit surface, large de-gasser volumes, oil or gas shows on mud
logs, calcite in well cuttings coming from fracture incrustations
or veins may be indications of fractures. A review of the well
history file is an important source of knowledge for the log analyst.
2.
Sample descriptions:
observation of fractures, slickensides, calcite in healed fractures,
blocky or fissile texture may indicate fractures.
3.
Inflatable packers:
an impression of the borehole wall can be imprinted on the rubber
when the packer is set in place. If fractures are present, they
will be seen, but there is no way to tell if they were induced
by drilling or were present before drilling.
4.
Drill stem testing:
analysis of pressure transient data from flow and buildup tests
has been used extensively to indicate the presence of fracturing.
28.03
Fracture Identification From Core Analysis
Conventional core analysis can provide much information about
fractures. Visual observation of open and healed fractures, stylolites,
slickensides, fracture density, and fracture dip angle can be
made at the wellsite or in the laboratory. They can also be described
from core photographs under natural light as in Figure 28.03,
and when oil is present, under ultraviolet light.

FIGURE 28.03: Core examination and core description show fractures
If
the core itself is not available for direct observation, you may
find clues in the core analysis report or core descriptions, where
the words fractured, frac, rubble, or lost core are clues to the
presence of fractures. Descriptive information may not be transferred
into all data bases, so it pays to check the original documents.
A
high permeability value in an otherwise low permeability environment
is another clue, as is an asterisk in the permeability column,
indicating a fractured core sample in which permeability could
not be measured. Large differences between maximum horizontal,
minimum horizontal, and vertical permeability also may indicate
fractures not seen by eye.
The
dip direction and strike can be determined, if the core has been
oriented with directional data. Cores can also be oriented by
comparing observed bedding plane and fracture dips with those
from a dipmeter analysis or by paleomagnetic orientation. Bedding
plane and fracture plane dip angle and direction are determined
by tracing the visible portion of the plane on the core surface
with a goniometer, a fancy word for a three axis (X-Y-Z) digitizer.
Originally mechanical devices, they are now electronic and interfaced
to computers for calculation of the best fit dip plane and subsequent
presentation of data listings and displays.
Special
core analysis techniques are used in fractured reservoirs, in
addition to those normally performed to obtain porosity, permeability,
and electrical characteristics. The major technique involves epoxy
injection at formation pressure to fill all pores and open fractures.
Whole slabs or thin sections are viewed or photographed under
plane or ultraviolet light. Pore structure, fracture connections
to isolated pores, fracture intensity, width, extent, and direction,
and anhydrite or calcite filled fractures are recorded. Results
are plotted versus depth and on rose diagrams, as illustrated
in Figure 28.04.

FIGURE 28.04: Epoxy filled thin section for fracture location
X-ray
tomography of cores, a non destructive, non invasive technique,
may see fractures not visible to the naked eye. Open fractures
with sufficient width and macro porosity appear as dark (fluid
filled) pixels on the computer screen. Both horizontal slices
and vertical reconstructed slices can be viewed on the computer
screen. Micro porosity and narrow fractures may not be distinctly
visible because the resolution is on the order of a millimeter
or larger, not as good as the photomicrographs described above.
Examples are shown in Figures 28.05 and 28.06.

FIGURE 28.05: X-Ray tomography for fracture detection

FIGURE 28.06: More X-Ray tomography for fracture
Analysis
by color coded partitioning of histograms is commonly used to
highlight particular features, such as porosity, mineralogy, or
invaded fluids. Since the color coding used to represent the X-ray
count rate is proportional to density, healed or filled fractures
are easily identified when the filling mineral is different than
the matrix. Fractures and porosity are shown in black on Figure
28.05, calcite filled fractures as yellow, and dolomite matrix
as orange.
Figure
28.06 portrays an anhydrite filled fracture (blue) with vuggy
porosity (black) and mud invasion (also blue). The matrix, dolomite,
is color coded yellow. Colors will vary under user control, so
be sure you understand where the color break points are and what
they are supposed to represent. Some ambiguity may exist, as in
this last example. Visual examination is used to corroborate problematic
situations.
Invasive
X-ray tomography, using an aqueous sodium iodide solution to fill
pores and fractures, is also used. A pressure sleeve is required,
but resolution is better than the native state method, due to
the high X-ray response of the injected fluid.
28.04
Fracture Identification From Spontaneous Potential Logs
The spontaneous potential normally does not develop well in carbonate
rocks, due to high resistivity and the long distance to a nearby
shale. However, some SP excursion is usually seen opposite very
porous or permeable carbonate zones, or opposite lower porosity
fractured zones. Fracture detection by the SP is possible in a
low porosity or low permeability bed if fracturing has occurred
and if the fractures contain a formation water of a different
salinity than that in the borehole. Development of an SP is not
a direct measurement of porosity or permeability.
The
SP is a voltage generated by electrochemical reactions between
the mud filtrate, formation water, and a nearby impermeable shale
barrier. No fluid movement takes place. In addition, a streaming
potential can be generated when mud filtrate passes through the
mudcake. It is primarily dependent upon mud resistivity and differential
pressure. As differential pressure increases, streaming potential
increases for a constant mud resistivity. Either the normal SP
or the streaming potential can be indicators of permeability and
fractures. A streaming potential only exists while fluid is flowing
and is not normally seen in a stable wellbore.
An
example is shown in Figure 28.06A, left hand side. Depths are
in meters and grid lines are two meters apart. The fracture zone
below 75 meters is indicated by the shallow resistivity reading
significantly lower than the deep. Over the same interval a small
SP development is superimposed on a straight line SP with a slight
drift to the left. When evaluating SP responses for fractures,
remember that the higher the oil saturation (lower water saturation),
the more the SP will be depressed. Very small excursions of the
log curve may be meaningful.
FIGURE
28.06A: Minor SP development in fractured zone
The
SP deflections to the right at 76, 84, and 132 meters may be caused
by a streaming potential due to mud filtrate flow into the formation
at these depths. This is not certain. Usually streaming potentials
are larger and cover longer intervals. These anomalies may be
caused by telluric currents, northern lights, rig power bumps,
or nearby welding.
Another
SP method is to compare the character of the SP to that of a gamma
ray log over the zone. If the SP develops in a zone which shows
relatively high radioactivity on the gamma ray, this could be
an indication of a permeable fractured zone in which uranium salts
have been precipitated.
Many
factors influence the SP and it is difficult to identify fractures
directly using this method alone, but often it aids in confirming
the possibility of a fractured zone. Care must be taken not to
interpret random variations or drift in the SP baseline as evidence
of permeability.
Having
detected the fractures, it is useful to count the footage, or
meters, of the fractured interval. In the example in Figure 28.06A,
the zone from 75 meters to the bottom of the log, or about 95
meters, is fractured. About 16 meters of this shows little resistivity
crossover and little SP deflection, giving a net fractured interval
of 79 meters.
28.05
Fracture Identification From Caliper Logs
In competent formations, the borehole will often become oblong
when it intersects a fracture. This looks like a hole washout
on a two or three arm caliper, but a 4 or 6 arm caliper will show
the oblong shape. The long axis of the hole is usually parallel
to the strike of folds or faults.
This
method is best when a sensitive caliper with sharp wall contacts
is used. Calipers recorded with most surveys are not very sensitive
and serve purposes other than measuring the hole size. Their design
does not allow for detection of small abrupt changes. Examples
are the three arm bow spring type calipers recorded with sonic
and density log which provide centralization as well as hole size
measurements. The caliper logs which are most helpful are recorded
with the dipmeter, microlog, and modern dual axis calipers on
density neutron logs. Special purpose, very sensitive, calipers
are available from most service companies.
The
caliper recorded with the microlog is designed to float on top
of the mudcake. It will respond and measure the thickness of the
mudcake, instead of measuring borehole rugosity. The presence
of mudcake should be more conclusive of permeability and possible
fracturing than rugosity alone. Dipmeter pads are pressured to
cut through mudcake and usually measure the rough hole if it is
present. Other dipmeter curves are also used to identify fractures.
Mud
rings sometimes form even in front of impermeable zones. Therefore,
mudcake indicators of permeability must be confirmed with another
log if possible.
Rough,
large, or irregular borehole in otherwise competent rock usually
indicates fractures. Mudcake opposite very low porosity usually
indicates fractures. Hole caving due to stress release is very
common, but open fractures are not always present. Not all washouts
indicate fractures; shale, salt, and unconsolidated sands often
erode, but their presence can usually be distinguished by other
log characteristics.

FIGURE 28.07: Dipmeter dual axis caliper shows oblong hole
in fractured reservoir
A
good example is shown in Figure 28.07. Zone A has a round hole,
roughly in gauge, indicated by the four arm caliper, and the dipmeter
curves show no fractures. Zones B and C show significant hole
elongation on the caliper. Fractures are inferred from this and
confirmed by the dipmeter curves. Fracture orientation is roughly
NE - SW. This information would help determine well spacing; offset
wells to the NW or SE would have to be closer than those in line
with the fracture orientation.
Remember
that a two arm caliper would probably see the long diameter. The
enlarged hole is a clue for fractures if the other log curves
indicate competent rock. A three arm caliper would average the
two diameters, and the hole enlargement may not be as obvious.
Zone
E again shows a round hole, this time oversize, indicating a washout
in un-fractured rock. This is probably a shale zone, which would
easily be confirmed by a gamma ray or SP log. Shales can erode
to an oblong hole, especially in deviated holes or in folded or
faulted areas.
28.06
Fracture Identification From Micro Resistivity Logs
Micro resistivity logs, such as microlog and micro SFL, indicate
fractures by showing low resistivity spikes opposite open fractures,
and high resistivity spikes opposite healed fractures and tight
or highly cemented layers. In older wells, the microlog, caliper,
and an ES may be the only logs available for use in fracture detection,
and for porosity and permeability for that matter.
The
microlog is one of the most conclusive indications of permeability.
When the dotted curve (2 inch micro normal) reads higher than
the solid curve (1 inch micro inverse), there is some permeability.
This effect is called “positive separation”. The caliper
curve accompanying the microlog resistivity measurements is also
available for mudcake location and thickness determinations. Mudcake
is another indication of permeability.
 
FIGURE 28.08: Micrologs show fracture location
In
Figure 28.08, left, there are three porous and permeable layers
with positive separation and mudcake, one near the top and one
near the bottom of the log section, and another just below the
7300 foot grid line. The lower layer has a single sharp, low resistivity,
spike. This is a fracture or a thin conductive shale streak. The
balance of the logged interval is impermeable and probably shale,
which could be confirmed by the SP or GR logs.
A
newer microlog run in combination with a proximity log is shown
in Figure 28.08, right. The permeable zone contains three distinct
fractures with several more tiny conductive spikes that could
indicate fractures. Only one is seen by the proximity log.
If
the micro resistivity curves are smooth, permeability is due to
porosity; if low resistivity spikes are present, fractures are
indicated. The microlog is a very reliable fracture indicator,
but like all single pad devices, it only sees a few of the fractures.
If the zone is known to be a carbonate or tight sand, and the
hole size is larger than bit size, an elongated hole and probable
fractures are indicated.
28.07
Fracture Identification From Dipmeter Logs
High resolution dipmeters with 4, 6, or 8 micro-conductivity log
curves, 2 or 3 opposed calipers, plus directional and orientation
data can indicate fractures by visual observation of log curve
characteristics and from individual dip magnitude and direction
calculations. Hole enlargement in a preferential direction discussed
in the previous Section, usually caused by fractures, is easily
displayed from the multi-arm caliper data, as illustrated in Figure
28.07.
Each
dipmeter pad provides a recording of changes in resistivity which
occur along the borehole, usually related to porosity variations,
bedding planes, or fractures. One pad is selected as reference
and its position relative to north is continually recorded. The
other pads are numbered clockwise looking from the top down. This
determines the orientation of all the pads. Dipmeter tool design
is described in more detail in Chapter
Twenty-Six.
The
log is analyzed in a similar fashion to a micro resistivity log.
However, four, six, or eight pads and better focusing make the
dipmeter a popular choice in modern wells, because it is more
sensitive and covers more of the borehole wall. The more elaborate
micro-scanner log has superceded the dipmeter log in many areas
and most comments about the dipmeter also apply to the micro-scanner.

FIGURE 28.09: Dipmeter curves show horizontal fractures or
bedding planes
Semi-horizontal
fractures appear as a short conductive anomaly on all four curves.
Examples of these sharp conductive spikes are shown on a 4-pad
dipmeter in Figure 28.09. Individual spikes represent bedding
planes or semi-horizontal fractures. Fracture intensity counts
are made by counting the number of spikes per unit length. Modern
thought now suggests that there is no such thing as a horizontal
fracture; they are considered to be poorly indurated laminations.
Regardless of their proper name, they often contribute to well
performance and are easily found with the dipmeter.

FIGURE 28.10: Dipmeter curves show semi-vertical fractures
Semi-vertical
fractures usually cause a relatively long conductive anomaly on
two opposite pads, or on one pad if the fracture is off axis enough
to be missed by the opposite pad. A typical vertical fracture
is shown by the shaded portions of Figure 28.10. Additional examples
are on Figure 28.07. This kind of analysis is normally done on
expanded scale playbacks of the raw dipmeter curves. Notice that
the grid lines in these examples are two feet apart, displayed
at 1:20 or 1:40 depth scales. Total length of vertical fractures
compared to total interval is a useful measure of vertical fracture
intensity.
The
fracture anomaly may disappear or jump from one curve to the next
as either the fracture or the tool rotates around the borehole.
An example was shown earlier in Figure 28.02, lower left, where
a single vertical fracture appears first as an anomaly on curve
1, then on curve 3 twelve feet above, after the sonde rotated
180 degrees. Remember that the pads see less than 50% of the borehole
wall, so the gap in coverage makes the fracture look like two
unconnected ones. Because of this, repeat passes should be made
in zones of scattered fracturing to provide better detection.
When
all four pads show conductive streaks over a long vertical interval
as in Figure 28.11, right side, a badly broken, rubble zone can
be inferred.

FIGURE 28.11: Fracture Identification Log (FIL) presentation
of dipmeter curves
To
amplify the fracture detection capability, the dipmeter curves
may have to be rerun or replayed with a different scale to show
all non-fractured zones as saturated (ie., displaying a constant
maximum resistivity). The log should be recorded in the usual
way to get the best dipmeter data. Then with the aid of the computer
in the logging truck, the curves can be displayed in different
formats to emphasize fractures. On existing logs, this can be
done in the computer center if the data tapes can be located.
An
easy way to analyze fractures with the dipmeter consists of comparing
the values of one pad to values of the other pads by replaying
adjacent curve pairs on top of each other. The curves are normalized
in tight, high resistivity zones. The magnitude of the separation
of the curves provides a qualitative indication of the fracture
intensity. This visual overlay technique has been dubbed the Fracture
Identification Log (FIL) by Schlumberger. An example is given
in Figure 28.11, left side, where the shaded areas represent vertical
fractures. Many other semi-horizontal fractures and permeable
bedding planes are also present, and contribute to production.

FIGURE 28.12: Fracture Identification Log (FIL) in Austin
Chalk
Another
example, from the Austin Chalk (Figure 28.12), shows the heavily
fractured upper zone, the poorly fractured lower zone, and an
intervening zone with no fractures. Notice that the bedding planes
in the shales look a lot like fractures, so a preliminary screening
to identify shale zones is absolutely necessary. People looking
for oil or gas in fractured shale can use this technique to great
advantage.
The
FIL presentation can be made for most types of dipmeters if the
data tapes can be located. For older, pre-tape, dipmeters eyeball
techniques must be used. The Stratigraphic High Resolution Dipmeter
(SHDT), with 8 conductivity curves, is a little more difficult
to use than standard high resolution tools. Vertical fractures
may influence both electrodes on a single pad. An FIL presentation
can be made by turning off one curve from each pad or by presenting
two sets of FIL overlays. The GEODIP presentation (see Chapter
Twenty-Six for details) may show numerous unconnected bed
boundaries in fractured zones. SYNDIP will often show non planar
dips or no dip correlations at all (bubble coding).
Since
pad orientation is known from the directional data, the fracture
azimuth can be determined. This will indicate the preferential
permeability direction. The azimuth of pad 1 is recorded directly
on low angle dipmeters, but the magnetic declination must be taken
into account.
DIPMETER MATH
For
low angle dipmeter
1: PAZ = AZ1 + MAGD
For
high angle dipmeters:
2: PAZ = AHD + RBR + MAGD
Calculate
fracture azimuth:
3: FAZ = PAZ + 90 * (PAD# - 1)
Adjust
angle to fit between 0 and 360 degrees:
4: FAZ = 360 * Frac ((FAZ + 360) / 360)
|
|
Where:
AHD = azimuth of hole deviation (degrees)
AZ1 = azimuth of pad number one on log (degrees)
FAZ = azimuth of fracture (degrees)
MAGD = magnetic declination (degrees)
PAZ = azimuth of pad one relative to true north (degrees)
PAD# = pad number on which fracture anomaly occurs
RBR = relative bearing azimuth on log (degrees)
Under
normal conditions, it is easy to read AZ1 on the log opposite
the fracture, add the magnetic declination, and put the result
in the range 0 to 360 degrees, using mental arithmetic. Figure
28.11, left side, shows the pad azimuth for a number of fractures
showing the preferential direction to be in the range 170 to 200
degrees, or roughly south. Fractures to the north are expected
also, but are not as obvious. This may be due to off axis fractures
or poor pad pressure in that direction caused by hole deviation
or bad tool maintenance.
28.08
Fracture Identification From Density, Neutron, and PE Logs
If
the density log shows high porosity spikes that are not seen by
the neutron log, usually fractures, large vugs, or caverns exist.
Broken out borehole also causes the same effect, but fractures
are often present when this occurs. Both cases are shown in Figure
28.13.
Because
the density tool only looks at a small fraction of the borehole
circumference, only a few of the fractures present will be logged.
The depth of investigation is rather shallow, so mudcake and borehole
rugosity can have an appreciable effect on the total measurement,
despite the fact that it is a pad type contact device with some
borehole compensation applied.
FIGURE
28.13: Density log spikes show fractures
Large
density correction values in competent rock, especially when weighted
muds are used, is a fracture indicator. The fracture network usually
does not increase the total porosity appreciably, but the resultant
increase in compensation, due to the rugosity, mudcake, or fluid
in the fractures, provides an indication of fracturing. See Figure
28.13 again.
Both
density and density correction curves show fractures better if
the log is recorded with a short time constant. This makes the
log look noisy and possibly useless for its normal purpose. The
time constant on existing logs can only be changed by reprocessing
raw count rate data from the original data tape.
Large
PE values, greater than 5.0 cu., especially when weighted muds
are used, is a fracture indicator. Barite has a very large photoelectric
cross section, 267 as compared with 5.0 for limestone and 3.1
for dolomite. Thus the PE curve should exhibit a very sharp peak
in front of a fracture filled with barite loaded mud cake. In
Figure 28.14, two very sharp peaks on the PE curve correspond
to fractures. The density correction curve also has a bump for
the presence of heavy mud. Corroboration from other sources is
essential. In light weight muds, an abnormally low PE value, less
than 1.7, indicates, fractures, bad hole condition, or coal.
FIGURE
28.14: PE curve shows fractures in barite weighted mud
The
compensated neutron log looks at the entire circumference of the
well bore, but is usually decentralized to minimize borehole effect.
It is not a useful fracture indicator by itself. However, neutron
porosity values are often compared with other sources to indicate
either lithology or the possibility of fractures.
The
sidewall neutron log sees only a small portion of the borehole
wall and may be affected by borehole break out in the same way
as the density log. Break out is often associated with fractures.
No
one would go out of their way to run a density neutron log combination
to identify fractures. However, it is the most common log suite
run today, and must be used if no other fracture logs have been
run. Fortunately the resistivity log, which is nearly always available,
can also help identify fractures and this helps confirm density
and PE anomalies.
28.09
Fracture Identification From Gamma Ray Logs
The natural gamma ray spectral log provides a quantitative measurement
of the three primary sources of natural radioactivity observed
in reservoir rocks: potassium, uranium, and thorium. The usual
gamma ray log records the sum of these three radioactive sources.
This log should not be confused with the (induced) gamma ray spectral
log, which is a form of pulsed neutron log run in cased hole to
evaluate lithology and water saturation.
Most
productive formations show a low content of all three radioactive
isotopes. The radioactivity associated with potassium and thorium
is normally attributed to clays in the formation. Since uranium
salts are soluble in both water and oil, zones of high uranium
content indicate fluid movement, subsequent mineral deposition,
and thus a probable zone of permeability, usually a fractured
zone.
An
Austin Chalk example is given in Figure 28.15. Here the upper
section is heavily fractured, the middle is not fractured, and
the bottom fractured in a few places. In nearly all cases the
uranium curve shows high radioactivity at the same depths as the
sonic amplitude and sonic variable density log indicate fractures.
In some cases, uranium may be present in the porosity without
a fracture, as in the shaded portions of the example. In others,
there may be fractures with no uranium (see arrow in Figure 28.15).
Just as with any fracture location method, there is no absolute
guarantee of identifying all fractures.
FIGURE
28.15: Natural gamma ray spectral log (KUT log) shows fractured
zones in Austin Chalk
If
uranium data is not available, the apparent shale volume from
SP, gamma ray, and density neutron crossplot are compared. If
the gamma ray derived shale volume is higher than the others,
uranium in fractures may be suspected.
Sandstones
are sometimes radioactive because of clay or feldspars, not fractures.
This can be confirmed by sample descriptions.
In
thinly laminated sand-shale series, the zone will appear radioactive
due to the shale, but may also contain uranium in fractures. To
locate fractures in these beds using the gamma ray method, calculate
shale volume independent of the natural radioactivity, then compare
this to the actual radioactivity, some of which may be due to
uranium in fractures. If a spectral log is available, the assessment
is easier.
The
natural gamma ray spectral log is one of only three methods that
can be used in cased hole to locate fractures. The others are
the array sonic and temperature logs, to be described later.
CAUTION:
In some areas, fractures are never radioactive, so this method
is not always suitable.
28.10
Fracture Identification From Resistivity Logs
On older wells that do not have porosity, caliper, or gamma ray
logs, the shallow resistivity log is used to help find fractures.
The shallow resistivity log may read the resistivity of drilling
mud in washed out borehole sections caused by the presence of
fracturing. Check the log heading and compare the mud resistivity,
corrected for the temperature of the borehole, with the actual
log reading. If they are similar in clean formations, a large
borehole may be suspected. Use the SP to find clean zones and
use the deep resistivity to check the resistivity of shales or
water zones.
Another
method, applicable to both old and new logs, is to look for cross
over of the shallow and deep resistivity. If mud resistivity is
less than the formation resistivity, as is true in many cases,
then the shallow resistivity curve will cross over the deep resistivity
in a fractured interval and read lower resistivity, due to invasion
of the fractures. Normally the shallow curve reads higher than
the deep, except in salt mud systems. The shallow curve may also
appear noisy or spiky. Review the example in Figure 28.02, right
side, and Figure 28.16.
FIGURE
28.16: Shallow resistivity cross over shows fractures
Remember
that the deep resistivity logs are averaging 5 or more vertical
feet of rock and that the shallow sees about 1.5 feet, so the
differences between the two logs is subdued by this. In thinly
laminated shaly sands, the cross over is probably due to shale,
not fractures. Check the sample descriptions.
For
improved resolution, an even shallower focused measurement can
be made with a proximity, microlaterolog, or micro spherically
focused log, and compared with the deep resistivity log.
All
are pad type instruments and survey a smaller portion of the borehole,
but all have been successfully used to aid fracture detection.
Pad type devices do not see the entire borehole, so only a few
of the fractures are logged. However, if the borehole is oval
because of fractures, most of them will be seen because they are
located on the long axis of the hole, where the pad rides. The
sharp conductivity anomalies may, at first be confused with a
loss of pad contact. Check to see that the tool is reading higher
than mud resistivity.
The
dual laterolog has been designed to provide resistivity measurements
in wells drilled with highly conductive drilling fluids. However,
it is the contrast between the resistivity of the formation, and
the resistivity of the drilling mud that is most important. When
the ratio of formation to mud resistivity is greater than about
50, better results can be expected from the laterolog than with
induction or electrical surveys. Due to the high resistivity of
most tight fractured reservoirs, the dual laterolog microlaterolog
combination is the preferred resistivity log for such zones.
Focused
logs such as the laterolog, spherically focused log, and even
the 16 inch normal on old ES and induction logs read resistivity
vertically through the formation. Induction logs read horizontally.
Therefore there can be a significant difference between the two
log readings when vertical fractures are present and invaded with
low resistivity drilling fluid. Normally, the induction log ignores
any vertical fractures and hydrocarbon filled horizontal fractures.
On the other hand a horizontal fracture filled with conductive
mud or formation water may produce a rather large conductivity
anomaly. When a laterolog or micro device reads less than an induction
resistivity in the same zone, vertical fractures are indicated.
The induction and ES are not useful in salt mud, so the technique
is not available in that case.
If
the dual laterolog is used, as recommended above, we lose the
advantage of being able to compare the horizontal measurements
with the vertical measurements, but the crossover effect due to
invasion is still common. Note that recent resistivity literature
states that all these tools actually measure vertically, contrary
to previous conventional wisdom. The newest induction logs, dubbed
3-D resistivity logs, truly measure both vertical and horizontal
resistivity. Comparisons of curve response assists in solving
anisotropic resistivity problems, as in laminated shaly sands,
and may help determine fracture orientation.
Both
methods are more conclusive in thick beds. Since invasion improves
the responses, any fracture system detected should be permeable.
Thin or high angle beds, along with the normal effects of borehole
fluid and size changes on the resistivity measurements, should
be considered when using this method.
28.11
Fracture Identification From Temperature Logs
Mud
fluid invasion into a fractured zone can lower its temperature.
If logged before it can return to the geothermal temperature,
the presence of fractures or, at least, invasion can be confirmed.
It is possible that the invasion is merely a function of porosity,
but usually the effect is smaller than for fractures. Figure 28.17
shows two clear anomalies opposite two fractured zones.
Gas
evolving into the mud system, often from tight fractured reservoirs,
may be seen if the mud system is static and under balanced for
sufficient time. The cooling anomaly should disappear above and
below the fracture zone, and will disappear everywhere in a few
hours if no additional flow or invasion takes place.
FIGURE
28.17 Temperature log may locate fractures
In
perforated cased holes, and in open hole or barefoot completions,
an injection profile can be run by increasing pressure on the
well head and then logging several passes with a temperature log
spaced over a few hours. The pressure will force fluid above the
zone downward, injecting cooler fluid into the formation. The
larger temperature anomalies are often associated with fractures
or the best permeability zones.
28.12
Fracture Identification From Sonic Logs
There is much literature concerning the effect of fractures on
acoustic wave propagation in porous and fractured rock. Unfortunately,
much of it is theoretical and not always supported by field examples;
often it is contradictory. Nevertheless, the sonic log is the
best fracture finder in older wells because other, more modern,
methods were unavailable at the time.
Today,
dipmeter and formation micro-scanner images provide more information,
but at higher cost, so sonic logs are still used extensively for
fracture identification. The modern full wave or array sonic and
dipole shear sonic tools provide much new information, including
shear wave travel time and amplitude plus full wave-train digitization
This allows the wave train to be further processed.
In
theory, the normal compressional interval transit time is little
affected by fractures so long as there is a free matrix path between
transmitter and receivers, as would be expected for vertical fractures.
In practice, large vertical and most sub-horizontal fractures,
create cycle skipping on the compressional transit time curve
on all sonic logs that rely on detection of the first energy arrival.
This is due to reduction in amplitude of the sound pulse by reflection
at the fracture face, and by destructive interference caused by
other propagation modes generated at the fracture. In addition,
refraction caused by near vertical fractures diverts energy from
the receivers, again reducing amplitude.
Cycle
skipping makes the sonic travel time too long. Thus simple theory
is overwhelmed by the complexity of sound transmission in a heterogeneous
medium.
28.18:
Sonic log cycle skips may indicate fractures
On
the array and dipole shear sonic logs, travel time is found by
waveform correlation and not by first arrival detection. Therefore,
it is less likely to skip a cycle due to low amplitude. Amplitude
curves are presented as a matter of routine, so fractures can
be identified by low compressional and shear amplitudes. Sonic
curves on the array or dipole sonic can disappear or be shown
as straight lines where amplitude is too low to obtain a waveform
correlation.
Cycle
skipping is an excellent fracture indication in hard formations.
The example in Figure 28.18 is a good illustration of what to
expect. Shallow resistivity crossover might help confirm fractures
in a typical well with only an induction and sonic log.
Gas
in the formation or in the mud, poor borehole conditions, and
poor tool condition or recording parameters, especially on older
logs, may also cause skipping. Tool centralization is also important;
compressional amplitude can be reduced to less than 20% of normal
with the tool only 1 inch off center. This can cause skipping
(see Figure 28.19, bottom). Note that most modern sonic logs are
designed to avoid cycle-skipping so this identification technique
may not be useful in many newer wells.

FIGURE 28.19: Compressional and shear sonic amplitude versus
fracture orientation and tool centering
The
cause of the skipping can be checked; if the skips occur only
in a competent zone and not in the surrounding shales, gas in
the formation or fractures are the only possibilities. Cycle skipping
is more common on long spaced than on short spaced sonic logs
in hard formations, because of lower sound amplitude on longer
tools. The reverse is often true in softer sands and shales, due
to rock alteration near the wellbore.
In
contrast, shear energy is, theoretically, strongly reduced by
both horizontal and vertical fractures, but not much by fractures
between 35 and 75 degrees (see Figure 28.19, top left). In practice,
fluids and fluid filled fractures do not conduct shear waves,
and shear arrivals are strongly attenuated in fractured zones
(Figure 28.19, right). On full wave or array sonic presentations,
the absence of shear arrivals or straight line segments on shear
travel time logs are sure signs of fractures. The Stoneley wave
amplitude is also strongly reduced by fractures.
To
differentiate between fractures and other causes of skipping,
a number of different logging tool designs and presentations of
sonic data have been developed. Special presentations include
the sonic amplitude, sonic wavetrain, and variable intensity (variable
density) displays, discussed below.
The
sidewall acoustic instrument was introduced to improve the bed
resolution and measurement of acoustic properties, but it was
not widely available or used. It is an acoustic pad device containing
one transmitter and two receivers designed to reduce attenuation
in the borehole and through the rock. The distance from the transmitter
to the first receiver is 9 inches, and the spacing between the
receivers is 6 inches. These dimensions allow for better bed definition
for porosity measurements and improved wave forms for fracture
studies.
Fractures
are more readily identifiable from this short spaced measurement
than from devices which measure and average a longer distance.
However, the measurement is affected by borehole rugosity and
only surveys a small portion of the borehole circumference. It
is best suited for thin bedded formations.
28.13
Fracture Identification From Sonic Waveform Logs
The elastic constants of rocks determine the velocity of sound
waves (see Chapter Twenty). Compressional
waves travel faster than shear waves and theoretically can be
seen separately on a display of sonic waveforms. Waveforms are
a record of sonic energy level versus arrival time. In practice
the two waves, and others, interfere with each other to some extent.
The
amplitude of both waves are affected by the rock type, porosity,
borehole rugosity, tool centralization, formation fluid, and fracture
size and orientation. The fractures may be only those induced
near the borehole wall by drilling or may be in-situ. Closed fractures
reduce the amplitude less than open fractures. Refracted waves
traveling other than direct ray paths can also reduce amplitude
and give false impressions of fracturing.
The
usual way to record these amplitude values is to present the amplitude
of the first energy arrival, which is from the compressional wave,
in the form of a log curve, or to present the entire wavetrain,
or both. On the newer array and dipole shear sonic, the shear
amplitude is also displayed. On older logs, some attempts were
made to measure shear travel time and amplitude by adjusting gate
times and trigger levels on the instrument panel. These logs were
not too reliable, so take care if trying to use them.
FIGURE
28.20: Sonic amplitude log may indicate fractures
Numerous
versions of these logs have been developed over the years, with
little standardization. Names such as Micro-seismogram, Fracture
Finder, 3-D Velocity, Acoustic Parameter, Shear Sonic, Variable
Density, and Frac Log were used by various suppliers. We will
use the generic term sonic amplitude log to cover all of these.
The
sonic amplitude log is a curve representing the first arrival
energy, measured in milli-volts. Energy varies with many factors,
so absolute values mean little, but low amplitude often means
fractures. All the things that cause cycle skipping, described
above, cause low amplitude, so fractures are only one possibility.
A sample is shown in Figure 28.20. This log is usually combined
with a gamma ray, caliper, and a wavetrain presentation, as shown.
The
sonic wavetrain log is a display of the recorded energy presented
as wiggly trace signatures, usually one for every 6 inches to
2 feet of borehole. The variable intensity display, sometimes
called a variable density log, displays the same waveform information,
but the amplitude of the positive peaks are shaded gray or black
and negative peaks are white. When plotted continuously, dark
and light bands representing peaks and valleys are displayed versus
depth. Conventions have varied, and arrival time has been plotted
increasing right to left or left to right, with the latter used
today.

FIGURE 28.21: Sonic waveform presentation
Two
waveform logs, with associated gamma ray logs are shown in Figure
28.21. Compressional amplitudes are lower than shear in most cases,
but two areas on the left hand log show reduced amplitude on both
compressional and shear waves, indicating fractures. Notice that
waveform arrival time increases from left to right.
In
Figure 28.20, a standard variable density (VDL) presentation is
given. Arrival time increases from right to left in this example.
Fractured intervals have low compressional amplitude on the amplitude
curve, and dark patterns on the waveform at the onset of energy
(arrows). The amplitude log also exhibits cycle skipping (S symbol
on log).
Reflections
from fractures cause changes in amplitude and travel time of the
main signal, and some waves arrive at later times, out of phase,
thus causing irregular interference patterns on the waveform.
Usually chevron patterns spanning several feet can be seen, indicating
reflections from near horizontal fractures. Chevrons are difficult
to see at best, and are not necessary diagnostic tools. Low amplitude
is all that is needed. Other interfering effects, such as Stoneley
waves and rough borehole cause jittery patterns. Vertical fractures
create less disturbance.
Normal
presentation of older sonic amplitude log includes:
1.
3 ft. spacing borehole compensated compressional travel
time
2. 3 ft. spacing compressional amplitude curve
3. 5 ft. spacing variable density display of entire
wave train amplitude
4. 3 ft. spacing single receiver compressional travel
time
|
|
On
modern logs, the shear travel time and shear amplitude are recorded,
along with complete waveform displays and other diagnostic curves.
Stoneley wave travel time and attenuation are also shown. Colour
images of the waveform correlation amplitude or colour versions
of the waveform display are now common (see Chapter Three for
tool details).
Fractures
are indicated when:
1.
amplitude of compressional first arrivals is low
2. single receiver travel time skips or does not track
compressional travel time
3. high frequency chevron patterns are seen on variable
intensity display
4. amplitude of shear wave arrivals is low |
|
Note
that single receiver travel time may vary, often indicating poor
tool centralization.

FIGURE 28.22: Circumferential sonic log for fracture detection
is a rare commodity
A
circumferential sonic log has also been developed but was not
widely available. Sound pulses travel around the borehole wall
and are attenuated most by vertical fractures, due to reflection
at the fracture surface. Few examples exist outside the well logging
literature. Both the sidewall and circumferential sonic rely on
waveform analysis for fracture identification. By alternating
between the two transmitters, four separate wavetrain or variable
intensity displays are created, one for each quadrant around the
hole. Figure 28.22 displays the geometry and output log for this
tool.
Evaluation
of any acoustic measurement is still complicated because many
factors other than a fracture system can cause attenuation or
distortion of the wave. Washout zones should be identified before
a fracture interpretation is made because they give similar responses.
In some shales, the compressive amplitude is larger than the shear
amplitude, which again looks like a fractured zone. A gamma ray
or SP log should be used to identify such zones.

FIGURE 28.23: Dipole shear sonic logs offer many display options
On
the full wave or array sonic log, we can measure travel time and
attenuation of the compressional, shear, and Stoneley wave energies,
instead of merely the compressional energy as on conventional
sonic logs.
FIGURE
28.24: Shear attenuation may locate fractures or vuggy porosity
These
attenuations result primarily from the large contrast in acoustic
impedance between the rock matrix and the fluid in the fractures
and in porosity. As compressional and shear waves traverse a fracture
their energies are significantly attenuated with the greatest
attenuation occurring to the shear wave. This is illustrated in
Figure 28.23 and 28.24. Remember that high attenuation is equivalent
to low amplitude. Attenuation is measured in decibels per foot
or per meter (db/ft or db/m).
Another
cause of energy reduction is poor acoustic coupling in zones with
vuggy porosity. This attenuation is due to acoustic wave scattering
as it is being transmitted through the vuggy porosity. Analysis
of acoustic energies must be supported by porosity information
to distinguish this situation. Acoustic energy is not severely
attenuated by normal intercrystalline porosity.

FIGURE 28.25: Waveform correlation map shows attenuation in
fractures
Suitable
processing of the digitally recorded waveforms can enhance the
visibility of fractures. One example is to plot the velocity cross
correlations to observe the compressional, shear, and Stoneley
energy on a time versus velocity crossplot. The peaks of the contoured
correlation amplitudes show where the sonic energy is located
. Figure 28.26 illustrates a comparison of a fractured and un-fractured
zone, showing the loss of shear energy as fracture intensity increases.
Note also that the log curve disappears (see left hand track)
because no energy is being received at the tool. The gap in the
log can be drawn as a straight line. This loss of data is equivalent
to cycle skipping on older logs.
Another
method involves filtering the waveforms to enhance the chevron
patterns caused by mode conversion interference. This is similar
to F-K or velocity filtering on seismic data. The dipole array
sonic sharpens the chevron patterns naturally, due to the different
propagation path of the directional acoustic beam compared to
the omni-directional pattern of the monopole array sonic (Figure
28.23, right). Stoneley reflection coefficients, computed from
adjacent Stoneley velocities, also help to pinpoint fractures.
28.14
Fracture Identification From Formation Micro-scanner Logs
The formation micro-scanner (FMS) or the newer formation micro-imager
(FMI) is an array of electrodes on pads used to produce an electrical
image of the formations seen on the borehole wall. On earlier
tools, the image arrays were on only two of the four pads, so
several logging passes of the tool had to be merged together for
better borehole coverage. Using this technique, from forty to
eighty percent wellbore coverage could be achieved. Newer tools
now have four or eight active imaging pads, reducing the need
for repeat passes to obtain 100% coverage of the borehole wall.
In
addition to the array electrodes, the tool also has ten standard
dipmeter electrodes (8 measure electrodes plus 2 speed buttons)
as well as a directional cartridge containing accelerometers and
magnetometers for orientation input to the standard dip computations.
The
electrical images are made by applying a gray scale to the resistivity
wiggle-traces produced from the electrodes on the tool. In this
way, low resistivity zones appear dark and high resistivity, low
porosity intervals appear white. Since the array on each pad is
two and a half inches wide, irregular features, such as vugs and
fractures, show up as dark spots and lines on the images. Colour
tones may be used instead of grey.

FIGURE 28.26: Formation micro-scanner shows fractures and bedding
planes
The
image depth scale is usually 1:20 or 1:40, and the X axis is scaled
from -180 to +180 degrees around the borehole, putting North in
the middle of the track. Examples are provide in Figures 28.26
and 28.27. A dramatic near vertical fracture can be seen in the
image at the top of Figure 28.26. Two vertical scales are used:
one for reconnaissance and one for detail evaluation. Fracture
orientation is roughly NNW - SSE dipping at more than 80 degrees.
Other images on these two figures illustrate induced fractures,
borehole breakout, inter-bedding laminations, slump brecchia,
vugs with fractures, and stylolites.

FIGURE 28.27: Formation micro-scanner shows porosity features
sometimes
Fractures
or bedding planes can be identified by connecting the linear features
to form a sinusoid on the image. The sinusoid can be analyzed
to find the angle of dip:
Fracture
or bedding dip from micro-scanner or televiwer
1:
Angle of Dip = Arctan (Y / D) |
|
Where:
Y = peak to peak distance of the sinusoid (millimeters)
D = hole diameter (millimeters)
Since
Y is measured on a plot or CRT, it must be transformed into actual
wellbore distance by multiplying the measured distance by the
plot scale. Note also that near vertical fractures will appear
near vertical on the plot and do not form sinusoids. Fracture
orientation is determined by the azimuth of the sinusoid troughs,
read from the scale at the top of the image.
Fractures
should produce a higher contrast anomaly than other porosity features
because the fractures are flushed with conductive borehole fluid
and there is exaggeration of the anomaly due to breakout of the
wellbore on the fracture. The fractures are sometimes masked,
however, by extremely conductive vugs, so both the gray scale
images and the electrical wiggle-trace data are analyzed to identify
fractures. Resolution of the micro-scanner is about 10 mm, but
contrast between fractures and rock is so good that thinner events,
as thin as a few microns, can often be seen.
Micro-scanner
images give a very good visual correlation to core and allow the
interpretation of small and large scale sedimentary features in
the formations. The identification of fractures, along with fracture
orientation, and the ability to differentiate them from high angle
bedding features is possible.

FIGURE 28.28: FMI log in fractured granite reservoir showing
computed dip angle and direction
Further
processing of the images to generate fracture frequency and fracture
aperture is now routinely applied to the newest formation micro-imaging
(FMI) logs. Older logs can be reprocessed for frequency and aperture
only if data tapes still exist. The product of frequency and aperture
is fracture porosity.
28.15
Fracture Identification From Borehole Televiewer Logs
The borehole televiewer image is similar in appearance to a formation
micro-scanner, but uses an ultrasonic derived, directionally oriented,
360 degree view of the borehole wall. Such an image, created by
a conventional televiewer, has sufficient resolution to see major
fracture systems in good hole conditions. The hole must be round,
smooth, and filled with light weight mud to get really good images.
The tool must be well centered. These requirements are not met
in most fractured zones, but logs are still run for fracture identification
and they are useful in many cases. Trade names for these tools
are not as well known as others: CBIL (pronounced Cybill) stands
for Continuous Borehole Image Log and UBI for Ultrasonic Borehole
Imager. Versions of these tools are also used for cement evaluation
in cased holes.
The
televiewer log of the wellbore is a representation of the amount
of acoustic energy received at the transducers, which is dependent
upon rock impedance, wall roughness, wellbore fluid attenuation,
and hole geometry. For example, a smooth surface reflects better
than a rough surface, a hard one better than a soft one. A surface
perpendicular to the transducers reflects better than one that
is skewed. Therefore, any irregularities such as fractures, vugs
and irregular porosity will reduce the amplitude of the reflected
signal.

FIGURE 28.29: Older acoustic televiewer log (left) and interpretation
image (right)
The
resolution of the tool allows us to determine events of about
10 mm in width. Fractures are often accentuated in the wellbore
by the drilling process, which breaks out the fracture on both
sides of the opening. If it were not for this breakout, most fractures
would not be seen by the televiewer as their width is commonly
less than 1 mm. An example of an actual image from an older televiewer
log, and an interpretive sketch with artificially enhanced resolution,
is shown in Figure 28.29. The formation microscanner is much more
sensitive to fractures than the televiewer. The electrical conductivity
of the fluid in the fracture is 1000 or more times higher than
the surrounding rock, compared to about 4 times for acoustic televiewer
signals.
In
addition to the amplitude image, the travel time image is also
recorded on modern logs. This is the travel time from tool to
wellbore wall and back to the detector through the mud. This image
is effectively an acoustic caliper log, and is used to locate
breakouts.
Considerable
research is being conducted to enhance the televiewer images,
using both arrival time and amplitude of the sound waves, plus
computer methods for image enhancement, especially edge enhancement
to resolve fractures and bed boundaries. Modern televiewer logs
can be used effectively in more rugged boreholes than older versions
because of the new processing techniques. Be aware of the age
of the log before you start your analysis.
Since
the televiewer image is oriented to magnetic north, we can determine
the dip direction of a fracture or bedding plane from the azimuth
of the troughs of the sinusoid. The dip angle can be calculated
from the same equation as given for the microscanner.
Fracture
or bedding dip from micro-scanner or televiewer
1:
Angle of Dip = Arctan (Y / D) |
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CAUTION:
The direction scale on the top of the image varies between service
companies. One uses a scale with North in the center of the image
(same as for FMS and FMI), another puts South in the center.
Figure
28.30 provides a televiewer and core photo of the same fracture.
The sinusoidal shape of the fracture trace is very obvious. In
this image, South is in the center of the track and the fracture
is oriented N 70 E, with a thinner, steeper fracture at N 45 W.
FIGURE
28.30: Core photo (left) and televiewer image (right) of fractured
interval
Fracture
identification is easiest when several detection methods are combined.
This is illustrated in Figures 28.31 and 28.32, where sonic variable
intensity and televiewer images are used. If density of the rock
is also measured, numerous elastic properties of the rock can
be derived, which are useful in hydraulic fracture design and
sanding studies. The mathematics for this work is covered in Chapter
Twenty.
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