This innovative fracture design methodology has capability to determine appropriate fracture conductivity and an economic optimum fracture length while reconciling these with actual frac
Trang 1Copyright 2004, Society of Petroleum Engineers Inc
This paper was prepared for presentation at the SPE International Thermal Operations and
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Abstract
A new methodology to obtain the optimum fracture treatment
design for a wide range of reservoir conditions has been
developed and successfully implemented The approach
discussed here significantly reduces the time required to
evaluate an optimum design and limits the materials considered
to only those that are appropriate for the reservoir conditions
These improvements make it an ideal methodology for
real-time re-design of fracture treatments after feedback from
minifrac data has been implemented
This innovative fracture design methodology has capability
to determine appropriate fracture conductivity and an economic
optimum fracture length while reconciling these with actual
fracture growth behavior in the reservoir The technique
incorporates the following simple, automated steps:
1 Selects the most cost-effective fluid that will meet a
minimum apparent viscosity requirement at a specified shear
rate and temperature condition from a large industry fluid
library to ensure that the proppant will be placed within the
pay zone
2 Selects a proppant that will provide the required fracture
conductivity at the cheapest cost from a large industry library
3 Determines the proppant concentration that is required at
the wellbore to achieve a user-specified dimensionless
conductivity criterion for a range of fracture lengths
4 Evaluates economic criteria such as net present value
(NPV) and return on investment (ROI) for different fracture
lengths by comparing fracture treatment cost and revenues
from production response
5 Determines the optimum fracture conductivity profile that
will have a uniform pressure drop down the fracture The
conductivity is adjusted for potential losses from non-Darcy
and multi-phase flow, gel damage, embedment, and other
proppant damage effects
6 Iterates a fracture treatment schedule that will result in the best fit of the optimum conductivity profile
The methodology can help optimize fracture treatments in any type of environment The technique is simple and can be run quickly in a real-time environment after a minifrac is conducted to make changes to the propped fracture treatment The procedure has been implemented in a commercially available fracture design program
Introduction/Background
During the last two decades, the oil and gas industry has actively been seeking methods to optimize its various processes In the most recent activity, the drive for optimization has focused on operator cost reduction to improve project NPV
In the completion of a well, the fracturing process has the potential to add the most value because of the enormous effect
it can have on overall reservoir performance, and consequently,
on the economic outlook of a project Since production pays for the entire cost of the well construction and completion, fracturing efficiency is a key factor in enabling production to meet economic needs
Another need has also been evidenced in the industry; i.e., transferring the knowledge of the aging workforce in our industry to the younger generation in order to prepare for the needs of the next two decades By developing a computer model that captures the optimization processes that an experienced fracture designer would follow when designing a fracturing treatment, a vast store of knowledge can be transferred to the new workforce to provide the tools needed to design an optimized fracturing treatment
The optimization approach to fracture design given in this paper is new to our industry in that it approaches the problem from the opposite direction than other methods; i.e., it uses the conventional design method in most cases What this approach accomplishes is that it reduces the time to develop an optimized solution and constantly considers economic drivers in order to find the treatment that will provide the greatest value for the given reservoir parameters
Since fracture optimization has been considered critical to economic success for quite some time, several approaches have been devised The oldest attempt at fracture optimization was described by Prats.1 The approach that Prats took was to optimize fracture dimensions based on a pre-determined proppant volume Prats discovered that for a certain fracture volume, the fracture that gives the optimum performance should have a dimensionless conductivity of 1.6 Since then, several other authors have re-confirmed Prats’ findings
SPE 86991
Reservoir-Based Fracture Optimization Approach
M Y Soliman, SPE, Audis Byrd, SPE, Harold Walters, SPE, Halliburton Energy Services, Inc., and Leen Weijers, SPE, Pinnacle Technologies, Inc
Trang 2Theoretically speaking, this approach is probably the most
effective, but unfortunately, several factors can compromise its
general application
First, the fracture volume is not usually the controlling
parameter unless the reservoir is highly permeable Thus, high
fracture conductivity is required to achieve a dimensionless
fracture conductivity of 1.6 If the formation permeability is
low, then it would be advantageous to design the fracture with
significantly higher dimensionless conductivity than 1.6
Second, fracture conductivity always changes with time;
proppant failure, and embedment would cause conductivity to
decline with stress and time.2 It is easy to see that loss of
conductivity when starting with relatively low conductivity
could seriously compromise the fracture performance
Third, it has been found that the clean up of fracturing fluid
and the associated multi-phase flow in the fracture would
require higher conductivity to be effective.3 This is especially
true for tighter gas-bearing formations
Fourth, the presence of several fluids inside the fracture, as
could be expected in all but dry gas reservoirs, would require
higher fracture conductivity than 1.6 to efficiently produce the
reservoir The potential presence of turbulence would also
dictate the creation of highly conductive fractures
As an example, if the formation permeability is 0.1 md, and
we design a 500-ft fracture with a dimensionless conductivity
of 1.6, the required fracture conductivity is only 80 md-ft This
low conductivity would impair the cleanup of the fracture, and
consequently, would negatively affect the productivity of the
well On the other hand, increasing the conductivity to the level
advocated in reference 3 would be fairly inexpensive
Another optimization technique was presented by Poulsen
and Soliman.4 In their approach, Poulsen and Soliman
optimized the proppant distribution inside a fracture in order to
achieve an equivalent fracture with uniform conductivity.5
Although the approach did consider some of the reservoir
properties, it did not optimize the total process In other words,
the designed fracture was not necessarily the optimum fracture
that had the best economical return In addition, the process
used a two-dimensional reservoir simulator approach
The technique considered state-of-the-art in today’s oilfield
is to run a simulator and develop a matrix of possible solutions
for the design parameters Then, the NPV is evaluated for each
design This process is very tedious because of the many
variables that come into play There are different fluids, fluid
concentrations, chemical additives, proppants, proppant
concentrations, and pump rates that can make this a tedious
task The most significant problem with this approach is that
the designer has to select the materials for the design matrix,
and because of the numerous possibilities available, the
designer may not select the best combination of fluids, fluid
concentrations, proppant type, proppant size, etc to produce
the optimum solution for reservoir This approach only picks
the best option in the matrix and is not a true optimization
process For this reason, many people give up on the
optimization process
This process may be also considered a simulation process,
and therefore, needs to be differentiated from the design
process A design process consists of assembling the building
blocks one after another to eventually build the best
fracture design
After the optimization has been done, it is common to perform a pump-in shut-in test to verify the reservoir inputs prior to the treatment on the day of the treatment At this point, there is not enough time on location to re-do the design matrix for the optimization process prior to pumping the treatment It
is for this reason that most of the changes on the day of the treatment are limited to adjusting the PAD volume only and not the proppant pumping schedule
Some of the new 3-D geometry models have a design tool
to speed the process The software integrates the desired proppant concentration into a pumping schedule to provide the desired proppant concentration in the fracture from the tip to the wellbore This approach provides the speed to do the computation on location but only provides a change in the PAD volume and the pumping schedule
A true design model would use the rock mechanics and stress layers to evaluate the fracture-growth profile predicted
by the model, and then, would create an optimized conductivity profile for the permeability of the reservoir It would also create the needed geometry to develop a treatment that may deliver the selected conductivity profile using the best combinations of all the design-material options based on a cost-versus-results basis In this way, the design model can iterate all the variables available to the fracture designer This process can be accomplished successfully if the material criteria limits are defined in a database that the design program can use In cases where no real data base exists, a rule-based system is developed by experts and used to fill in the gaps The criteria can be established by testing, or in other cases, by expert opinion on the appropriate application ranges This allows the developed technique to iterate or make selections on the rule-based system during the process to prioritize the materials appropriate for the design criteria These criteria would include temperature, closure stress, conductivity, two-phase flow, and any other parameters that an expert would deem appropriate
By developing a design process as described above, a consistent design philosophy can be deployed to transfer best practices and enable the novice to design fracture treatments based on the latest technology Using a consistent approach will help prove new technology and any new design philosophies developed as result of applying the new concept
This approach will ensure that the new philosophies will be transferred to everyone using this optimization approach, and thus, reduce the learning curve and training requirements
In this paper, the authors will present a methodology for designing a fracture that results in optimum return from the reservoir This approach relies not only on theoretical considerations, but also on practical experience and considerations Field examples illustrating the application of this methodology will be presented and discussed later in this paper
Fractured Well Productivity Ratio
Fractured-well productivity has been extensively studied, and several production-increase curves have been developed and presented in literature.6-8 These production-increase curves varied in complexity, but all predicted increase in well productivity as a result of fracturing treatments The curves presented by Tinsley, et al6 and Soliman7 are probably the most comprehensive They consider not only the effect of fracture
Trang 3conductivity and length relative to the reservoir radius, they
consider the effect of fracture height to the total formation
height However, most of the production increase curves and
ratios are given in terms of dimensionless parameters Using
this type of presentation, it is often difficult to translate to
practical values This is the motivation for determining a new
dimensional approach to presenting production increase
concepts to average users
A transient pressure analysis of a vertical fractured well in
pseudo-radial flow, as described by Cinco-Ley and
Samaniego-V.9, forms the basis for the new technique Pseudo-radial flow
is appropriate for evaluating long-term production trends,
which is our area of interest The basic idea was to present the
production increase contours as a function of fracture half
length and fracture conductivity, both of which are widely
understood variables The process is as follows:
For a given reservoir, wellbore conditions and production
increase ratio contours are used to calculate the infinitely
conductive fracture half length
⎜⎜
⎛
−
=
PI
r r r
L f exp ln2d ln d / w (1)
Then, for the finite conductivity fracture half
lengths, calculate
⎜⎜
⎛
−
=
PI
r r r
r w' exp ln d ln d / w (2)
Using the dimensionless curves in Cinco-Ley and
Samaniego-V,9 calculate the dimensionless fracture
conductivity, and finally, the fracture conductivity
f fD
fw C kL
k = (3)
An example of this new type of production increase ratio
curve presentation is given in Figure 1 The figure is for a well
spacing of 320 acres and a wellbore diameter of 7.875 in
Reproducing the figure with a formation permeability of 0.1
md yields Figure 2 Assuming that for an efficient fracture
cleanup a CfDof approximately 30 is required, if a production
increase ratio of 4 is desired, then a fracture conductivity of
about 1300 md-ft would be required
The relationship between the parameters that can be
changed by fracture design, which include fracture half length
and conductivity, are now easily related in a dimensional
fashion to production increase ratios and dimensionless fracture
conductivity The average user is now able to easily examine
the tradeoffs between these variables and make informed
decisionsconcerning their use
Other production increase curves could be plotted easily in
the fashion that would make them more valuable to the
practicing engineer
Outline of the Optimization Process
The integrated computer-aided design and completion approach
presented in this paper includes at least three steps, and
possibly, a fourth step as well The goal of the first step is to
calculate the parameters of an approximately optimized fracture using a simple graphical approach This step includes selecting initial fracture parameters This step also provides an initial completion design to be further optimized in the next steps The second step involves a comprehensive approach to optimizing fracture design based on economics The initial design of step one is the starting point of the optimization process of step two Step three includes adjusting the model parameters on location using real data from the subject well to create an optimized treatment schedule for the fluid and proppant available on location at the time of treatment The fourth step is the inclusion of risk analysis in this optimization process The fourth step is optional, but it will provide another quantitative measure to the optimized design, and while not required for generating the optimum fracture design, does add
an important analysis to the process
The four steps may be based on computational algorithms
or may be based on neural network algorithms The neural network algorithm accurately mimics the behavior of various computational algorithms such as fracture geometry calculation Each of these steps will be described in more detail in the following sections
Initial Design
1 Run logs to determine physical and mechanical properties
of the formation The physical properties may include, for example, permeability, porosity, type of the fluid and fluid saturation The physical properties are usually obtained from a combination of logs such as gamma ray, density, sonic, electric, and pulse neutron logs The mechanical properties include Young’s Modulus and Poisson’s Ratio The stress field, including in-situ stresses at different height locations, can also be determined Logs such as long-spaced sonic and dipole sonic may be used for this task If a magnetic resonance imaging (MRI) tool is used, the list of parameters may also include irreducible fluid saturation, hydrocarbon, and water permeability The MRI log gives a strong indication of the grain size and distribution, and in some cases, clay content Whatever parameters are selected should be digitally encoded
2 Divide the measured and calculated formation parameters into zones from a fracturing point of view Usually, this is done based on the calculated or measured in-situ stress
3 Develop a limit on fracture-design parameters using the physical properties of the formation and a production increase curve such as the one discussed in the previous section It is possible to use other production increase curves described in literature.6-8 Unsteady-state production increase calculations may be also used
For illustration of this concept using steady-state conditions, the production increase curves discussed in the previous section and Figure 1 are used The production-increase curves are dependent on formation permeability, fracture length, fracture conductivity, drainage area, and wellbore diameter For example, if one is to stimulate a formation with a permeability of only 0.1 millidarcy (md), the
graph of Figure 2 reveals that a fairly long fracture with
conductivity in excess of 1,000 md-ft would be beneficial This is shown more clearly in the expanded section shown in
Figure 3 The graph of Figure 3 indicates that a production
increase (PI) ratio of 7.5 is attainable with a fracture
Trang 4conductivity of 2,000 md-ft and a fracture length of 667 feet
shown as intersection point A
To allow for an efficient fracture clean up in a fairly tight
formation, a dimensionless fracture conductivity approaching
30 is usually recommended.3 The line for a dimensionless
fracture conductivity of 30 is shown in Figure 3
If the formation permeability is 100 md and the curve for
dimensionless conductivity of 30 is again considered, creating
a fracture length of 33 feet requires a fracture conductivity of
100,000 md-ft as shown in Figure 4 at point A Such
conductivity would be difficult to attain if not impossible In
addition, this high dimensionless conductivity is no longer
required for clean up Thus, the design should be only
considering the well productivity In this case, the program
then may opt to use a dimensionless conductivity of 3, yielding
a required fracture conductivity of 10,000 md-ft (see point B in
Figure 4) Such fracture conductivity may be attainable using
special fracture design procedures (tip screen out) In a
high-conductivity fracture such as this, the use of an optimum
dimensionless conductivity of 1.6 (discussed earlier in the
paper) may be acceptable provided degradation of conductivity
is taken into consideration
If turbulent flow is expected to take place inside the fracture
(from calculated flow rate), adjustment of designed
conductivity should be considered as the effective fracture
conductivity is lower than the actual fracture conductivity
First, the potential for turbulence using established techniques
should be calculated A factor based on degree of turbulence
and the effective fracture conductivity should be determined
The actual flow rate is then calculated In case of steady state,
the calculation can be done once; however, in the case of
unsteady state, the calculation of the turbulent factor is done in
steps at different times
4 Calculate an approximate fracture width using the
mechanical properties of rock (Young’s Modulus and Poisson’s
Ratio) For example, a two-dimensional model equation such
as those developed by Perkins and Kern can be used
5 Calculate the required proppant deposition (such as in
pounds per square feet) given the conductivity that has been
determined using published tables or equations Such
determination should account for stress carried by the proppant
type(s) and size of the proppant(s) Allow for possible
proppant embedment, especially in soft formations, and any
effect of proppant embedment in filtercake
Referring to Figure 5, the graphs show that different
proppants have different disposition requirements at a
conductivity of 10,000 md-ft, for example The one requiring
the least amount per square foot for this condition is a
resin-coated proppant indicated at point A of Figure 5 (slightly less
than four lbm per square foot) This material is suitable for a
stress characteristic of approximately 3,000 psi at a
conductivity of 10,000 md-ft shown as point A in Figure 6
Thus, given a calculated desired conductivity, a desired
concentration, and a stress parameter, the list of available
proppants may be quickly narrowed
6 Calculate the required sand concentration in pounds per
gallon (lbm/gal or ppg) for a given width and desired
conductivity using digitally encoded published equations or
graphs such as those illustrated in Figure 7 For the above
example of a proppant deposition of about four pounds per
square foot and a calculated width of 0.875 inch Figure 7 shows that the proppant concentration in the fracturing fluid should be 10 lbm/gal; point A
7 Calculate downhole temperature at each fluid stage using a temperature calculation model/correlation
8 Define the best fluid to carry the proppant and keep the majority of the proppants in suspension (70%) using the calculated temperature Factors that may be considered include leak-off coefficient, closure time, and degradation of fluid viscosity with time
9 If it is found that the designed proppant concentration is higher than could be normally achieved, a tip-screen-out (TSO) design should be considered In tip screen out, the fracture is designed so that the proppant reaches the tip of the fracture at the time the fracture reaches the desired length When the proppant reaches the tip of the fracture, the fracture will stop growing in length Then, by continuing to inject sand-laden fluid, the fracture will grow in width (balloon) After the fracture is allowed to close, the sand concentration will be significantly higher than would otherwise be achieved
Steps 6 through 9 may be reiterated to conclude the best proppant, average proppant concentration, and fluid system for the treatment Preferably, the foregoing will be performed using a suitable software that includes digital implementations
or representations of computational and materials information (for example, suitable programming to permit use of the information and relationships as represented in Figures 5-10)
Refined Design
The above is done more for materials selection, whereas the following fine tunes the design using the lowest cost materials
The initial run uses more generic information to limit the materials list, and in this stage of selection, the various chosen materials are run in one or more models provided in commercially available simulators
One may have noted from the above discussion that a specialized approach is needed to obtain the desired conductivity and that this phase is where that process will be optimized The following steps should be followed:
1 Generate a desired fracture conductivity using the initial design given above and the determined desired fracture conductivity This fracture conductivity is the fracture
conductivity at the wellbore; therefore, a conductivity profile that creates a fracture with constant pressure drop down the fracture is generated.10
2 Run a fracture simulation using the mechanical properties
of rock (Young’s Modulus and Poisson’s Ratio), physical properties, zoning of the formation, and calculated in-situ stresses The simulator uses the fluid and proppant type or
types that were determined in the initial design
3 Calculate downhole temperature using a temperature calculation model/correlation This temperature profile is used
to determine the fluid degradation, and thus, proppant transport and settling to develop the in-situ proppant conductivity
4 Define the best fluid needed to carry the proppant and keep the majority (for example, 70%) of the proppants in suspension using the calculated temperature Factors that should be
considered include leak-off coefficient, closure time, and degradation of fluid viscosity with time and temperature If the original fluid mixture is insufficient, then more polymer or less
Trang 5breaker will be adjusted to achieve the desired proppant
suspension Determine the feasibility of propped fracture
length and width by running a fracturing model using selected
fluid/fluids to determine the effect on the fracture geometry
This process examines whether the fracture geometry (length,
height, and width profile) would significantly change from the
original design
6 Calculate the proppant profile inside the fracture, both
settled or in suspension These calculations take into
consideration fluid rheology, proppant size, density and
concentration This is needed in the event that all the proppant
is not perfectly transported to the designed location within the
fracture (which it will not be but it should be close if the fluids
are adjusted correctly), the ideal conductivity will be affected
7 Determine proppant concentration needed at each location
to produce the non-uniform fracture conductivity This could
be based on the theoretical curve developed by Soliman,5 who
developed a set of curves describing the change in conductivity
with distance inside the fracture As described by Soliman, if
the conductivity inside the fracture changes, then the fracture
will behave as if it has a uniform conductivity
8 Determine initial proppant in slurry and fluid for each
location This is done by dividing the fracture into segments
and adding the fluid that was lost during its transport down the
fracture to give the needed concentration at the surface This
calculation considers the physical properties of the rock, the
rheological properties of the fluid, and the concentration of the
proppant in the fluid
9 Adjust for settled proppant and determine proppant
schedule The fluid degradation may cause some settling, and
this is where the final fluid mixture is adjusted to achieve the
proppant transport needed for the conductivity profile Steps 4
through 9 may be reiterated to conclude the best proppant,
average proppant concentration, and fluid system for
the treatment
10 Run a reservoir simulation to predict well performance
using the optimum fracture designs with and without fracturing
and for the different designs that will result from the material
selections The reservoir simulator produces a profile of well
productivity for each local optimum fracture design Based on
the chosen economic drivers (see next item) a global optimum
is determined
11 Run an economics model and plot a selected economic
parameter such as NPV, Benefit/Cost Ratio, ROI, etc., versus
fracture length
If working with a 3-D design, only concentration against
the pay zone is considered The above design was essentially
for a two-dimensional model It may be expanded to a
three-dimensional situation by considering that the formation
consists of a contributing formation and non contributing
formation The proppant concentration against the contributing
formation is the critical factor
Real Time Modification to Design
After the desired fluid and proppant have been determined
using the above steps, those materials in suitable quantities are
delivered to the actual well site (if they are not already there)
Before the fracturing job is performed, however, a pumping or
treatment schedule must be determined This is accomplished
by conducting the following steps:
1 Pump mini-frac job with step-down test to perform a fluid efficiency test
2 Determine if and how much near-wellbore friction exists
3 Determine closure, net pressure, and fluid efficiency for formation
4 Adjust fracture-design program-model parameters to match net-pressure and leak-off rate from mini-frac
5 Use fracture-design program model design mode to optimize fluid and proppant on location for new model parameters matched
in step 4 of this section
6 Pump treatments as per new optimized design in step 5 of this section
7 Monitor treatment with fracture-design program in real time model to predict fracture growth during treatment
8 Make adjustments to treatment based on model prediction
as required
Real-Time Application
Implementation of this design methodology in a commercial simulator allows the design strategy to be revisited many different times as the amount of knowledge about a reservoir increases during the development cycle of a well or a field
An initial design based on log-based reservoir information can be created using this methodology and can be redone in real time once additional data from breakdown injections and/or minifracs (fluid efficiency test) becomes available These injection tests provide necessary information about fracture-closure stress, level of net pressure, and fracture-fluid efficiency (or leakoff behavior) These simple and direct measurements can have a big impact on fracture designs and should be incorporated in the final treatment design For example, leakoff behavior observed during a minifrac has a big impact on sizing the pad to obtain a TSO in a high-permeability reservoir
In a field development situation, once a single fracture treatment is conducted, fracture design work is not finished Instead, fracture design is a continuous task that slowly evolves
as more data become available, for example, from net pressure matching of the propped fracture treatment data, from direct measurements of fracture growth using direct fracture diagnostics (such as tiltmeter or microseismic fracture mapping), or from longer-term production data
Implementation into Fracturing Simulator
This methodology was recently implemented into a commercial hydraulic-fracture-growth system to 1) make the methodology widely available, and 2), to come to a more uniform design approach throughout the company This method is illustrated
in the chart in Figure 8
Once the most applicable and cheapest proppant and fluids are selected, the simulator will approximate how much proppant and fluid will be required to obtain a certain fracture length, given a user-defined dimensionless conductivity criterion
As shown in Figure 9, the simulator will determine the
fracture height, conductivity, net pressure, etc for every length
the user wants, Figure 10 shows a fracture profile as a function
of all the fracture lengths for which the model has been run
Once the fracture dimensions are known as well as how the actual reservoir impacts fracture growth, it also becomes
Trang 6possible to estimate a theoretical production response using the
PI-conductivity plot in Figure 11 The black dots in this figure
provide the solution from the simulator that is closest to a
desired dimensionless conductivity criterion that is specified by
the user
If the required fracture width at closure time is smaller than
the width during the fracture opening in the baseline design, we
do not have to go into a TSO The required width at the
wellbore at closure on proppant is a function of the width at the
end of pumping and the actual proppant concentration in the
fracture (close to the wellbore) at that time:
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛ +
−
=
max
max
1
) 1 /(
C X
C X w
w
propvol
prop propvol
pumping end proppant
on
closed
φ
(4)
where Cmax is the maximum proppant concentration, φprop
is the proppant porosity and Xpropvol is the proppant volume
factor in gal/lbs (which equals 1/ (SG*8.345404)) with SG
being the proppant’s Specific Gravity in kg/l
The desired width to obtain a certain CfD goal is
calculated by
embedment f
f fD goal
k
kL C
w
where kis the average height-weighted permeability for all
pay zones combined, Lf is the fracture half-length, and kf is the
permeability (after damage) of the proppant pack M is the
number of conductive multiples and dembedment is the embedment
thickness of one fracture wall
Now, we can determine the maximum proppant
concentration that needs to be pumped to obtain the required
propped width by setting
proppant on closed goal
C w
w
If wC goal wclosed on proppant
fD > with 15 ppg is being set at
the default proppant concentration, then the simulator will
automatically consider a TSO design To do this, we will keep
the maximum proppant concentration at 15 ppg (or anything
else the user has defined in the screen above) and keep the tip
screen-out net pressure increase within user-defined limits
The net pressure increase to reach the CfDgoal can be
estimated as follows:
( max) ,
,
C w
w p
p
proppant on closure
goal C pumping
of end net goal
C
net
fD
The net pressure at the end of pumping would be the net
pressure taken at the required fracture half-length in the
baseline calculation
When conducting a design, it could very well be possible (as shown in Figure 11) that the CfD
goal cannot be achieved,
in which case the only other available alternative is to pump better proppant or a higher proppant concentration
Economic Analysis
The simulator contains a large library with fluid and proppant properties as well as pricing Up to date pricing information is obtained from the service company’s price book The simulator has calculated how much fluid and proppant is required for every fracture half-length, how long it will take to pump the job, and what the required horsepower will be With this information, it is possible to calculate the approximate cost
of each job as a function of the obtained propped fracture
half-length as shown in Figure 12
Figure 13 shows results when a single-layer single-phase
finite difference simulator is used to forecast production response of the stimulated fracture
To do a proper economic analysis, both treatment cost and expected revenues from production should be evaluated The simulator can then be used to select the treatment with the best NPV or ROI for a user-specified time period as shown in
Figure 14
Determine Treatment Schedule
The proppant distribution is provided by the following equations4:
8 8 2 2 1
⎠
⎞
⎜
⎜
⎝
⎛ + +
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛ +
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛ +
=
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛
f f
f f
fD
L
x a L
x a L
x a a L
x
with
( ) ( ( ) )2
2 , 1
, 0
,
0
j fD
j j
j
C
A C
A A
f L
x being the distance in the fracture away from the
wellbore divided by the fracture half-length, and CfD (0) is the CfD goal at the wellbore
The simulator will iterate on the proppant profile within the fracture and minimize a weighted, least-squares error of the difference between the ideal proppant profile and the actual proppant profile
The error is weighted by distance away from the wellbore
to allow the profile at the wellbore to be more important than if matching it far away into the fracture The following error is minimized while using a constant of approximately 1:
) 9 ( ) )
/ 1
((
) )
/ 1
((
)
constant fraclength
distance ideal
constant fraclength
distance ideal
model error i i
+
−
+
−
−
Trang 7Example Application 1 - Moderate permeability oil
well in Venezuela
Figures 9-14 show fracture design and optimization results for
an oil reservoir at a depth of 6100 ft in the Lagunillas field in
Venezuela The horizontal section has moderate permeability
of about 60 md and requires a TSO design strategy in order to
obtain CfD’s within a reasonable range
Fracture growth is believed to be somewhat confined based
on anecdotal evidence that certain fracture treatment sizes do
not penetrate specific layers The stress profile is not well
known – the stress in the producing sand comes from
pressure-decline analysis of breakdown injections, while the sand-shale
stress contrast is “guesstimated,” based on pore-pressure
differences To mimic the slight fracture confinement, a
composite layering effect was used The permeability, the
driving parameter for the type of design, was determined from
pressure buildup tests in nearby wells, and therefore, is
relatively well known
Two selection criteria dominated the analysis:
1 What treatment can maximize economic benefits? The
economic analysis resulted in a maximum NPV for a fracture
half-length of about 240 ft
2 What treatment can avoid growth in a water-bearing zone
approximately 100 ft above the top perforation? Since the
fracture profile for a fracture with a 240-ft half length is clearly
penetrating the water-bearing zone above, a smaller half length
of 150 ft was selected to avoid growth into this unfavorable
zone
Example Application 2 - Low permeability Gas well in
the Rockies
This application is in a sandstone reservoir bounded by
shale layers, all with moderate to high Young's modulus of
about 3,500,000 psi which is typical for the US Rockies The
closure stress gradients are modest at about 0.55 - 0.60 psi/ft,
and reservoir permeability is of order 0.1 md A Borate Guar
fluid with relative low gel loading was used to stimulate
these wells
Many times, when people design a fracture, they usually do
not incorporate any feedback from real data Engineers could
use what they have learned from indirect measurements such as
net-pressure history matching and production data analysis to
estimate what they are achieving with their propped fracture
treatments Although this type of analysis can be very
beneficial to obtain a basic understanding of what is achieved,
a problem with these types of analyses is that solutions can be
non-unique As a result, economic optimization may not
provide a true design optimum
To address this shortcoming, the capability to calibrate
fracture models with directly measured fracture dimensions, for
example, using tiltmeter fracture mapping or microseismic
fracture mapping is now possible
Figure 15 shows the net pressure history match The
uncalibrated net pressure inferred geometry in Figure 16 (top)
shows significant out-of-zone growth This match was
conducted using the “classical” assumption that confinement
was only caused by fracture closure stress contrast
However, microseismic mapping showed an actual fracture
height of only 130 ft and a fracture half-length of 700 ft – very
different from the uncalibrated pressure-matching result Net pressure history matching was redone to match the actual geometry First, we determined that a closure stress gradient in excess of 1 psi/ft was required in the shale to obtain the observed confinement, and this was considered unrealistic Therefore, a composite layering effect was introduced Most fracture-growth models in the industry assume that there is perfect coupling of the fracture walls along its height As a fracture tip grows through layer interfaces, some of these interfaces may become partially de-bonded, and the fracture may start growing again at a local weakness offset from the
original path, slowing vertical fracture growth Figure 16 (bottom) shows the final fracture geometry from the
calibrated model
Now that a calibrated model has been obtained by matching net pressure response AND directly measured fracture dimensions, the fracture model can be run in predictive mode
to evaluate alternative designs In this particular example, production data showed that effective propped half-length was far shorter than the 700-ft hydraulic fracture half-length, most likely due to insufficient cleanup farther away in the fracture Significant cost savings have been achieved by pumping smaller treatments on subsequent jobs, reducing hydraulic fracture half-length while maintaining effective propped fracture half-length and production response
Figure 17 shows the fracture treatment cost for typical
fracture treatments in this area These treatment costs incorporate variable costs dictated by horsepower, level of surface pressure and rate, job duration, quantity of fluid and proppant used, and fixed costs such as mobilization The dashed curve shows the dramatic increase in costs for the near-radial fracture growth anticipated in the initial design, which was not calibrated using direct fracture growth measurements The solid curve shows the modest increase in costs for the confined fracture growth that was measured using direct fracture growth measurements
Figure 18 shows the differences in NPV for a 1-year period
following the propped fracture treatments, assuming the following facts:
1) monthly production maintenance cost of about $500 2) average cost for fracture job with 500,000 lbs Ottawa and about 5000 bbl fluid of approximately $100,000
3) expected IP at 500 to 700 Mscfd, 35 ft pay, 0.1 mD permeability and 200 ft half-length
4) approximately 75% decline
Due to the differences in height/length growth, NPV estimates for both designs are very different Due to dramatically increasing cost when assuming near-radial fracture growth, the NPV maximizes for a much shorter propped half-length of about 280 ft This requires a treatment volume of about 800 bbl The calibrated design, which incorporates the measurement of significant fracture confinement, provides a maximum NPV at a fracture half-length of more than 600 ft, and will require a fracture treatment volume of about 1500 bbl This calibrated design and larger optimum length also requires the use of a larger amount
of proppant
Trang 8Conclusions
A comprehensive methodology that equally considers both
theoretical and practical aspects has been developed to
optimize fracture design
1 The procedure can help to effectively optimize fracture
treatments in any type of environment and can be done quickly
in real-time after a minifrac is conducted to make changes to
the propped fracture treatment
2 The methodology has been successfully implemented in
fracture design software
3 The presented field examples illustrate the validity of the
presented methodology
Acknowledgments
The authors of this paper would like to express their thanks to
Halliburton Energy Services, Inc and Pinnacle Technology for
allowing this work to be published They would also like to
thank Nancy Woods, Carolyn Williams, and Sam Moore for
their efforts in preparing the manuscript
Nomenclature
,
0
a
= constants
,
, j
i
A
= constants
fD
C
= dimensionless fracture conductivity
max
C
= the maximum proppant concentration
embedment
d
= the embedment thickness of fracture wall
w
kf
= fracture conductivity, md-ft
k= reservoir permeability, md
f
k
= fracture permeability, md
f
L
= fracture half length, ft
M = the number of conductive multiples
p= pressure
net
p
= pressure above closure pressure (net pressure)
PI = production increase ratio
d
r
= drainage radius, ft
w
r
= wellbore radius, ft
'
w
r
= effective wellbore radius, ft
w= fracture width
proppvol
X
= the proppant volume factor, gal/lbs
propp
φ
= the proppant porosity
References
1 Prats, M.: “Effect of Vertical Fracture on Reservoir Behavior – Incompressible Fluid Case,” JPT (June, 1961) 105-118
2 McDaniel, B W.: “Conductivity Testing of Proppants at High Temperature and Stress,” SPE 15067 presented at the 56th California Regional Meeting, held in Oakland, California, April 2-4, 1986
3 Soliman, M.Y and Hunt, J.: “Effect of Fracturing Fluid and Its Clean-up on Well Performance,” SPE 14514, presented at the Eastern Regional Meeting held in Morgantown, West Virginia, Nov 6-8, 1985
4 Poulsen, D., and Soliman, M Y.: "A Procedure for Optimal Fracturing Treatment Design," SPE 15940, presented at the Eastern Regional Meeting held in Columbus, Ohio, November 12-14, 1986
5 Soliman, M Y.: "Fracture Conductivity Distribution Studied,” Oil
& Gas Journal, February 10, 1986
6 Tinsley, J M., Tiner, R., Williams, J and Malone, W T.: “Vertical Fracture Height — Its effect on Steady State Production Increase,” JPT, May 1969, 633-638
7 Soliman,M.Y.:“Modifications to Production Increase Calculations for a Hydraulically Fractured Well,” JPT, Jan 1983
8 McGuire, W.J, and Sikora, V J.: “The Effect of Vertical Fracture
on Well Productivity,” Trans AIME, (1960) 219, 401-405
9 Cinco-Ley, H and Samaniego-V., F.:“Transient Pressure Analysis for Fractured Wells,” JPT, Sept 1981, 1749-1758
10 Perkins, T K and Kern, L R.: “Width of Hydraulic Fractures,”
JPT (Sept 1961) 937-49
SI Metric Conversion Factors
bbl x 1.589 873 E - 01 = m3 gal x 3.785 412 E - 03 = m3 bbl/min x 2.649 788 E - 02 = m3/h
ft x 2.831 685 E - 02 = m3
in x 2.54* E + 01 = mm
md x 9.869 233 E - 04 = m3 psi x 6.894 757 E + 00 = kPa
*Conversion factor is exact
Trang 9Figure 1 - Fractured Well
Production Increase Curves
1E3 1E4 1E5 1E6 1E7
Fracture Half Length
Well Diameter 7.875 (in) Spacing 80 (acre)
8 7 6 5 4 3 2
1 10 100 1E3 1E4
0.1 1 10 100 1E3
10 100 1E3 1E4 1E5
100 1E3 1E4 1E5
1E6
Permeability 0.1
Production Increase
Trang 10Figure 2 Fractured Well Production Increase Example
Figure 3 - Expanded view of
Production Increase Curve
Figure 4 Production Increase curves
1
Permeability 0.1 md Well Spacing 320 acre Hole Diameter 7.875 in
Fracture Half Length (ft)
2
3
4
6
8
2
3
4
6
8
2
3
4
6
8
10
100
1000
10000
C fD 10
5
PI6
Fracture Half Length (ft)
2000
1000
30
A
B
PI
C fd
7 7.5