FracproPT Short Course (March 2008)
March 26, 2017 | Author: Florentin Zamfirache | Category: N/A
Short Description
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Description
• • • • • • • •
Introduction Fluid Rheology, Flow Leak-off, Proppant Transport Rock mechanics & Stress, Fracture Modeling Concepts Tortuosity & Perforation Friction Net Pressure Matching Fracture Conductivity & Design Considerations Production Modeling Fracture Diagnostics & Model Calibration
Fracture Engineering & Modeling
for proppant disposal
NOT
Hydraulic fracturing is done for well stimulation
Motivation for Frac Engineering & Diagnostics
Time during fracture treatment Frac width
Frac length
Simplified cross-sectional view of the fracture
7 – Formation closes on proppant and a conductive path remains in the reservoir
6 – Pumping of the fluid/proppant mixture is stopped and fluid continues to leak away into the permeable formation
5 – Proppant advances further in the fracture and may reach the tip of the hydraulic fracture as fluid continues to leak into the permeable formation
4 - Proppant advances further into the fracture as pumping continues
3 – Proppant (usually sand) enters hydraulic fracture as it is suspended in the fracturing fluid
2 - Fracture propagation with fluid
1 - Fracture initiation as pumping of fluid is started
Hydraulic Fracture Growth
1
2
3
4
Prop conc
Flow rate
5 6
Surface pressure
7
General pressure response, flow rate, and proppant concentration during a propped fracture treatment
7 – Formation closes on proppant and a conductive path remains in the reservoir
6 – Pumping of the fluid/proppant mixture is stopped and fluid continues to leak away into the permeable formation
5 – Proppant advances further in the fracture and may reach the tip of the hydraulic fracture as fluid continues to leak into the permeable formation
4 - Proppant advances further into the fracture as pumping continues
3 – Proppant (usually sand) enters hydraulic fracture as it is suspended in the fracturing fluid
2 - Fracture propagation with fluid
1 - Fracture initiation as pumping of fluid is started
Hydraulic Fracture Growth
Rock deformation Fluid flow inside fracture Fluid leakoff Fracture propagation Proppant transport Heat transfer
• Understanding these mechanisms and their interrelationships provides a starting point for understanding hydraulic fracture growth behavior
– – – – – –
• Hydraulic fracturing is a complicated process that involves several coupled physical mechanisms
Hydraulic Fracturing
Physical Processes
0
frac
0
+ Vleakoff = 2γ 1wi Li H i + ∫
ti
Ct 2 Ai dt t − ti ( x )
Assumes spurt loss is zero
Qt = V frac + Vleakoff ≅ 2γ 1ww LH + 2 LH 2Ct t
∫ Qdt = V
ti
• At all times, the injected fluid volume is equal to the fracture volume plus the volume of fluid that has leaked off
Conservation Of Mass
Fluid Rheology & Leakoff
3 ∂p w Q = h.q ; q = v • w = µ ∂x
• Generally modeled as laminar flow between parallel plates • Flow rate is extremely sensitive to fracture width
Fluid Flow Inside A Fracture
∂ ∆ p 64 Qu = ∂x π Hw 3
• Flow down an elliptical tube
∂∆p Qu = 12 ∂x Hw 3
• Flow between 2 parallel plates
Laminar Fluid Flow
– Controls Crosslinker Reactions – Impacts Fluid Properties
• pH
– Controls Surface Treating Pressure – Impacts Injection Rate
• Friction
– Controls Hydrostatic Gradients – Impacts Proppant Convection
• Density
– Controls Amount of Fluid in Fracture – Impacts Fracture Geometry
• Fluid Loss
– Controls Fracture Width (Near Wellbore) – Impacts Proppant Transport
• Viscosity
PROPERTIES OF A FRACTURE FLUID
∆p
Q or Shear Rate (γγ)
Q
∆p µ Constant = Q for Newtonian Fluid
Newtonian Fluid
WHAT IS VISCOSITY?
Q
∆p or Shear Stress (τ)
SHEAR STRESS ( τ )
0
τy
τb
0
µ
Drilling Mud
Water
Fracturing Fluid
Dilatant (Shear Thickening)
Newtonian
PseudoPlastic (Shear Thinning)
SHEAR RATE (γ )
µp
Bingham Plastic
Example
RELATIONSHIP OF τ AND γ
LOG-SHEAR STRESS ( τ)
LOG-SHEAR RATE γ( )
k‘ = Intercept
n’= Slope 2
τ = Shear Stress, lb/ft -1 γ = Shear Rate, sec k = Consistency Index, lb-secn2 /ft n = Flow Behavior Index, dimensionless
τ = k’γγn’
FRACTURING FLUIDS ARE TYPICALLY
µ a = 47880 k’a
[γγ]
n’- 1
γ
= Shear Rate, sec-1
µa = Apparent Viscosity, cp ’ n / ft2 k’a = Consistency Index, lb-sec n’ = Flow Behavior Index, Dimensionless
Where:
• To Calculate the Apparent Viscosity of a NonNewtonian Fluid, the Following Equation is Used
VISCOSITY AT A KNOWN SHEAR RATE
• Shear Rates in Tubular: 1000 - 5000 sec-1 • Shear Rates in Fractures: 10 - 100 sec -1 • Measurements of n’ and k’ Often Made Between 170 and 600 sec -1 • May Not Be Representative of the Fluid Behavior in the Fracture (40 sec -1)
TYPICAL SHEAR RATES DURING FRACTURING
Shear Rate
{
40.46 Q w2 h
= Apparent Viscosity, cp = Consistency Index, lb-secn’/ft 2 = Flow Behavior Index, Dimensionless Q = Injection Rate, bpm w = Fracture Width, in h = Fracture Height, ft
µa k’a n’
Where
µa = 47880 ka’
n −1
• Apparent Viscosity of a Non-Newtonian Fluid in the Fracture, ’
ESTIMATING VISCOSITY IN FRACTURES
ROTATING CUP
TEST FLUID
STATIONARY BOB
Torsion Spring
VISCOSITY MEASUREMENTS
0.03 0.55
0.8
Linear Gel
Crosslinked 0.5
0.00002
1.0
Water
k’
n’
Fluid Type
2000
50
1.0
Viscosity @ 170 sec-1
TYPICAL VISCOSITY VALUES
0.1
1.0
1
D 2 3 4 5 6 TIME, hours
B
A C
0.6 .
0.8
1.0
1
2
3 4 5 TIME, hours
6
B C A
250°F 50 lb/1000 HPG w/ Titanium
0.2 0
0.4
D
EXAMPLE RHEOLOGICAL DATA
Source: Halliburton Energy Services
0.001 0
0.01
ka
n
Typical Extent
Cw
< 1/10 inch
Fracture Fracture Filtercake Filtercake
Cc
100’s of feet
FLUID LOSS
0.5 to 3 feet
Cv
Invaded Zone Invaded Zone
Reservoir
Reservoir
m A
kr Cr µr
ki ∆p φ µa 1/2
= Slope of Volume vs t Graph = Area of Core Used to Measure Cw
0 .0164m (Measured in Lab) Cw = A
= Permeability to Reservoir Fluid, md = Formation Fluid Compressibility, psi -1 = Formation Fluid Viscosity, cp
k C φ Cc = 0. 0374∆ p r r µr
= Permeability to Filtrate, darcies = (σ σx + pnet) - p, psi = Formation Porosity, fraction = Viscosity of Filtrate, cp
k ∆p φ Cv = 0.0469 i µa
1/ 2
FLUID LOSS EQUATIONS
TIME
Spurt Loss
Slope = Cw * Area / 0.0164
MEASUREMENT OF WALL BUILDING COEFFICIENT (Cw)
VOLUME
60 lb
40 lb
60 lb
250
350
With 25 lb/1000 gal Solid Particulate FLA
40 lb
Without FLA
FLUID TEMPERATURE, °F
150
Titanate Fluid
50
0.002
0.004
0.006
0.008
.
EFFECT OF FLUID LOSS ADDITIVES (FLA) ON WALL-BUILDING FLUID-LOSS COEFFICIENT, Cw ) 1/2
FLUID LOSS COEFFICIENT, C w (ft/min
Ct =
• William’s Method
• Series Average
(
2 CvCw + C2wCr2 + 4Cc2 Cv2 + Cw
[
1 1 1 1 + + Cv Cc Cw
2 CcCvCw
Ct =
)]
1/2
TOTAL FLUID LOSS C t
High Filtration
Longer Fracture
Low Filtration
HIGH SLURRY EFFICIENCY
Short Fracture
LOW SLURRY EFFICIENCY efficiency (t) =
Fluid Leakoff And Slurry Efficiency
Vpumped (t)
Vfrac (t)
• • • •
– Convection – Settling
Percentage of Fluid in the Fracture Affects Created Fracture Dimensions High Leakoff Can Lead to Screenouts Low Leakoff Will Increase Closure Time Affecting Proppant Placement
FLUID EFFICIENCY
18µ Terminal settling velocity for Newtonian fluid
Vs =
gd p2 (ρ p − ρ f )
What Is Proppant Settling? Downward Transport Of Dense Proppant Grains In Fluid
ρ3
>
ρ2 >
Convection velocity for Newtonian fluid
γ cn gw 2f (ρ max − ρ min ) Vc ≈ 12 µ
ρ1
ρ3
ρ2
ρ1
What Is Proppant Convection ? Downward Transport Of Dense Slurry
Rock Mechanics, Closure Stress, Fracture Modeling
Mini-fracs, small volume injection tests (DFIT, stress test) Drilling data Logs Estimated using net pressure matching
Need rock properties and stress for all depths where fracture propagates
– – – –
• Stress Data
– Core – Logs
• Rock mechanics
Sources for Rock Mechanics & Stress Data
σ = Stress = ε = Strain = E = Young’s modulus =
Assume linear elasticity: F/A δ/L σ/ε
L
F
A
Deformation Of A Bar Due To Uniaxial Compressive Load
δ
ν = Poisson’s ratio =
δ/L δr /R
ε r/ε (-1,1/2)
ε = Strain in axial direction = εr = Strain in radial direction =
Assume linear elasticity: L
F
R
Deformation Of A Bar Due To Uniaxial Compressive Load
δr
δ
Net Pressure is the Pressure Inside the Fracture Minus the Closure Pressure Net Pressure = 2,500 - 2,000 = 500 psi
Definition Of Net Pressure
Balloon Analogy For Opening Fracture With Constant Radius
w pnet
Generalization: w = Deflection E = Crack-opening modulus C = Compliance
R
Rock
= E/4(1-υ2) = γ R/ E
= γ pnetR/ E
Fracture cross-section
Opening Of A Fracture Due To Internal Pressure
50 psi
800 psi
Pnet =
Pnet =
Predicted net pressure
= 650 feet = 0.25 in
= 260 feet = 1.6 in
R w
R w
Predicted fracture dimensions
• Two radial fracture model solutions for the same treatment (no barriers):
Influence Of Net Pressure
Predicted frac dimensions
L = 1200 feet
R = 240 feet
Predicted net pressure
Pnet = 100 psi
Pnet = 800 psi
• Two modeling solutions for the same treatment; if 500 psi stress contrast exists around payzone
Fracture Geometry Changes With Net Pressure
• 2D models – Perkins, Kern and Nordgren (PKN) – Christianovitch, Geertsma and De Klerk (CGD) – Radial Model • 3D models – Pseudo 3D models – Lumped 3D models – Full 3D models – Non-planar 3D models
Different Models
• Solid mechanics • Fluid dynamics • Fluid Leakoff
Fluid dynamics
Fluid Leakoff
Solid Mechanics
Simplified Fracture Problem
Ww
L
h=H
Simplified Fracture Problem – Constant Height
hpnet w≈ E E L = εV 2h2pnet
• Fracture width:
• Combining these:
• Mass balance:
εV ≈ 12 2 h2 Lw
• Given: volume pumped, fluid efficiency and measured net pressure
Simple Dimensions Calculation For PKN Model
• Fluid Loss:
• Width & Fluid Flow:
• Mass balance:
LM N
2
VFL = 2 HL 2 2Ct t
π Qµ (1 − ν ) L w = ww = 4 5 5 2πE
π
Qt = 2 HLw + VFL
• Given: volume pumped, injection rate & job time, and total fluid loss coefficient
Simple Dimensions Calculation (PKN)
OP Q
1/ 4
VFL = 5.657 HLCt t Assume v=0.15
5
• Fluid Loss:
ww
QµL O L = 0.238M P E N Q
w=
π
1/ 4
5.61Qt = 01667 . HLw + VFL
• Width & Fluid Flow:
• Mass balance:
• Given: volume pumped, Fracture Height and total fluid loss coefficient
Oil Field Units
Simple Dimensions Calculation (PKN)
pnet ∝ t
• Net pressure:
1/ 5
1/ 5
w ∝t
L ∝t
• Width:
• Length:
4/5
Fracture Growth Versus Time For PKN Model
ww R
Simplified Fracture Problem – Radial Fracture
R w
Yields:
Radius Width @ wellbore
V e E ν pnet
~ ~
= = = = =
103 ft 1.51 in
1,000 bbl (~ 5,610 ft3) 0.5 1x106 psi 0.2 500 psi
Elastic opening
For: Volume pumped Efficiency (@ EOJ) Young’s modulus Poisson’s ratio Net pressure (@ EOJ)
6 eVp net w= 3 2 π E
2 pnet ⋅ R w≈ π E
Mass balance
2
3 eVE R= 4 p net
2 e • V = πR 2w 3
1 3
1 3
Estimating Frac Dimensions Radial Fracture
VFL = πR 2 2Ct t 2
• Fluid Loss:
2
• Width & Fluid Flow:
LM N
Qt = πR w + VFL 2
2 2 27Qµ (1 − ν ) R w = ww = 3 3 4π 2 E
• Mass balance:
• Given: volume pumped, injection rate & job time, and total fluid loss coefficient
OP Q
1/ 4
Simple Dimensions Calculation (radial model)
• Fluid Loss:
• Width & Fluid Flow:
• Mass balance:
Assume v=0.15
2
VFL = 8.886 R Ct t
2 QµR . w = ww = 0147 3 E
LM N
2
OP Q
1/ 4
5.61Qt = 0.262 R w + VFL
• Given: volume pumped, Fracture Height and total fluid loss coefficient
Oil Field Units
Simple Dimensions Calculation (radial model)
pnet ∝ t
• Net pressure:
−1/ 3
1/ 9
w ∝t
R∝t
• Width:
• Radius:
4/9
Fracture Growth Versus Time For Radial Model
GR
h3
PH = σ3 h3 + σ2 h2 + σ1 h1
σ3
h2
P
σ2 H
h1
σ1
Neglects fracture toughness, tip effects, composite layer
Simple Force Balance for Height Growth
Height Growth Depends on Stress Contrast, Net Pressure, and Geology
Mode I Mode II Mode III Mode IV
-
I
p' = Critical Net n Pressure
log (∆t)
II IV
III
Confined Height, Unrestricted Growth (slope = 0.20) Stable Height Growth Or Increased Fluid Loss (slope = 0) Growth Restriction, Tip Screen-out (slope=1) Rapid Height Growth
Classical Interpretation of Fracturing Pressures
log (pn )
• •
• •
•
Direct Injections Pressure decline analysis • Square-root time plot • G-function plot • Log-log plot Flow back test Step-rate test (upper bound) Logs Dipole Sonic Log (DSI) Synthetic profiles from standard logs
Different Methods To Obtain Fracture Closure Stress
• Closure stress (pressure) is identified by the transition between the two flow regimes
• reservoir diffusivity
– Radial flow regime; Pressure decline depends on:
• fluid leakoff rate • fracture compliance
– Linear flow regime; Pressure decline depends on:
• Pressure decline after a mini-frac passes through two flow regimes:
Pressure Decline Analysis
•
• • •
Tp
Tc Time
Rate
Pnet
ISIP
Efficiency ~
Closure
TcTc+ Tp
Tc Tp+Tc
Fracture closure pressure (minimum stress) Fluid efficiency Leakoff coefficient, reservoir permeability and pressure Fracture geometry estimate
What Can You Obtain From Pressure Decline Analysis?
Bottomhole pressure
dP/dt
BHP
Reference line
Square-root-of-shutdown time
Fracture closure
Mini-Frac Analysis: Square-root-of-time graph
Pressure, dP/dt
Log Scale (∆P, t*d∆P,d∆t)
∆ t*d∆P/d∆t
Radial flow
½-slope
Log Scale (∆t = t-t shut-down)
linear flow
∆P = BHP-ISIP
Fracture closure
Mini-Frac Analysis: Log-Log graph
Pressure, dP/dG, G*dP/dG
BHP
G-function
Fracture closure
dP/dG
G*dP/dG
Reference line
Mini-Frac Analysis: G-Function graph
BHP
G-function
Fracture closure
Height recession
dP/dG
G*dP/dG
Reference line
Mini-Frac Analysis: G-Function graph
Deviation below reference line could indicate height recession
Pressure, dP/dG, G*dP/dG
G-function
Fracture closure
Deviation above reference line could indicate pressure dependent leakoff/fissure opening
BHP
dP/dG
G*dP/dG
Reference line
Pressure Dependent Leakoff/Fissure Opening
Mini-Frac Analysis: G-Function graph
Pressure, dP/dG, G*dP/dG
BHP
G-function
Fracture closure
dP/dG
G*dP/dG
Reference line
Fracture Growth After Pump Shut-down
Mini-Frac Analysis: G-Function graph
Linear behavior, but intersection above the origin could indicate fracture growth after shut-down
Pressure, dP/dG, G*dP/dG
Pressure Decline Analysis – Square-root Time Plot
Pressure Decline Analysis – G-function Plot
Pressure Decline Analysis – Log-log Delta Pressure Plot
•
•
Step Rate Test – Start at matrix rate – Increase in steps until fracture extended (≈ 1 to 10 BPM) – Provides upper bound for closure – Can determine if you are fracturing at all Flowback at Constant Rate
Steprate/Flowback test
•
•
" near-well pinch "
~ 15 min
~ 30 psi SI-Rebound < p c independent of " tortuosity" SPE PF Feb '97
FB induced " wellbore pinch”
Here ‘frac WB pinch’ is identified at closure: very small
– otherwise volume of fracture is to small due to high leakoff
High perm well where the FB-SI is run after the gel calibration test
Pump-In/Flowback/Shut-in Test (SPE 24844)
Onion-Skin
Cement
Unfractured Halo
Blue-Dyed Fracture
Perforation Tunnel
Pipe
Perforation Damage - Crushed, Compacted, “Onion-Skin” Zone
Tortuosity & Perforation Friction
• Instantaneous rate changes, e.g. 30, 20, 10 and 0 BPM exact rates are unimportant, but changes should be abrupt • Implemented easiest by taking pumps off line • Each rate step takes about 20 seconds -- just enough to equilibrate the pressure • Fracture geometry should not change during stepdown total stepdown test volume small compared to test injection volume (note: pfrac not proportional to Q1/4 during stepdown test) • Use differences in behavior of the different friction components with flow rate
Tortuosity Can Be Measured: Stepdown Test
What Is Tortuosity? Width Restriction Close To Wellbore
Width Restriction Increases Necessary Wellbore Pressure
Wellbore
Net fracturing pressure Near-wellbore friction
Distance into fracture
Pressure after shut-in
Low
High
Fracture tip
Tortuosity Leads To Large Pressure Drop In Fracture Close To Well
Fractures Grow Perpendicular To The Least Principle Stress -- But What Happens At The Wellbore ?
Near-wellbore Friction Vs. Perforation Friction
Time (min)
20.20
21.00
5500 19.40
0.00
18.60
6100
10.00
17.80
6700
20.00
17.00
7300
8500
30.00
Meas'd Btmh (psi)
7900
Btm Slry Rate (bpm)
40.00
50.00
Near-wellbore Friction Vs. Perforation Friction
Source: “SPE paper 29989 by C.A. Wright et al.
• Perforation friction dominated regime
Tortuosity Can Be Measured: Stepdown Test
• Near-wellbore friction dominated regime
Tortuosity Can Be Measured: Stepdown Test
Use proppant slugs Initiate with high viscosity fluid Increase gel loading
Re-perforate
Ball-out treatment
Spot acid
Future wells may have altered completion strategy such as FEWER perfs
Increase rate
Severe fracture tortuosity
High perf friction
High entry friction
Maximum Treating Pressure Limitation Is Reached -- Can’t Pump Into Zone
• Situation: • Diagnosis: • Solution:
• Formation: • Completion:
Naturally fractured dolomite @ 8200’ (gas) 5-1/2” casing frac string, max. surface pressure 6000 psi; 70’ perf interval shot at 4 SPF, 90°°, 0.45” diameter hole; Previously acidized with 70 gallons/ft 20% HCl Declining injectivity leading to “pressure-out” on pad Severe near-wellbore fracture tortuosity 1 and 2 PPG proppant slugs very early in the pad to screen out fracture multiples
Example Application – “Pressure Out” on Pad
28.0
56.0
84.0
Time (min)
112.0
0.00 0.0 140.0
8.00 40.0
12.00 60.0
16.00 80.0
0.00 0
Increased max prop conc
no tortuosity at end of pumping
4.00 20.0
0.0
S/D#1: 1700 psi tortuosity; small perf fric.
S/D#2: 300 psi tortuosity
20.00 Max surface pressure 6000 psi 100.0
Btm Prop Conc (ppg) Slurry Flow Rate (bpm)
4.00 1200
8.00 2400
12.00 3600
16.00 4800
20.00 6000
Proppant Conc (ppg) Surf Press [Csg] (psi)
1400 psi friction reduction (1st slug)
Example Application – “Pressure Out” on Pad
Encyclopedia Britannica
Petroleum Engineers
Net Pressure History Matching
• Surface pressure OK for decline match • Deadstring or bottomhole gauge required for matching while pumping
– With “anchor points” from diagnostic injections – Recorded pressure, slurry rate and proppant concentration
• Well completion and perforations • Treatment schedule, proppant and fluid characteristics • Treatment data
– Young’s modulus (from core or sonic log) – closure stress profile (injection/decline data or sonic log) – Permeability (from PTA)
• Mechanical rock properties
Minimum Model Input Requirements
Earth Model
Earth Model
• Allows on-site design refinement based on observed fracture behavior
• Provides a powerful tool for on-site diagnosis of fracture entry problems
• Relatively inexpensive and quick diagnostic technique to apply
• Basic analysis data collected (in some sense) during every frac treatment
Fracture Pressure Analysis - Advantages
Net pressure
Pump time
Pump rate Predicted net pressure
Use predicted net pressure
Wellbore
Pay
• Early designs (pre-1980) did not incorporate feedback from real data • Fractures at that time were still smart enough to stay in zone
Modeling without Real-Data Feedback
Fracture Design and Analysis Evolution
Pay
Net pressure
Pump time
Pump rate Predicted net pressure
Measured net pressure
Use predicted net pressure
Wellbore
?
Pay
• Early designs (pre-1980) did not incorporate feedback from real data • Fractures at that time were still smart enough to stay in zone • But measured net pressure was generally MUCH higher than model net pressure
Modeling without Real-Data Feedback
Fracture Design and Analysis Evolution
Pay
Net pressure
Pump time
Matching measured net pressure with model net pressure
Use measured net pressure
Wellbore
• Net pressure history match can be obtained by adding new physics to fracture models • With the right assumptions and physics, inferred geometry has a better chance to be correct
Modeling with Net Pressure Feedback
Fracture Design and Analysis Evolution
Pay
Net pressure
Pump time
Matching measured net pressure with model net pressure
Use measured net pressure
Wellbore
• Net pressure history matching can be implemented by adding new physics to fracture models • With the RIGHT assumptions and physics, inferred geometry has a better chance to be correct • BUT pressure matching inferred geometry does not always fit directly measured geometry
Modeling with Net Pressure Feedback
Fracture Design and Analysis Evolution
Pay
2
Pre-frac com pletion and fracture design
4
3
pressure
E xplo re / bo und altern ative explanations for observed net
M atch m odel net pressure to observed net pressure
Determ ine observed net pressure
Characterize friction param eters using rate stepdow n tests
Determ ine f racture closure stress and m atch perm eability
1
Interpret m odel results, m ake engineering decisions
Perform treatm ent
Post-frac m odeling review and incorporate other fracture diagnostics
Repeat process in succeeding stages or w ells
Basic Fracture P ressure A nalysis Steps
• Obtain surface pressure from service companies recorded data • Obtain hydrostatic head from staging and fluid/proppant densities • Obtain frictional components from S/D tests • Obtain fracture closure stress from pressure decline
pnet ,obs = psurface + ∆phydrostatic − ∆p friction − σ closure
Required to Obtain Observed Net Pressure
Net Pressure Matching
Net Pressure Vs. Friction Pressure
• Model net pressure can be changed to match observed net pressures using several “knobs”
– Correct for fracture closure, frictional effects and hydrostatic
• Match “observed” net pressure with calculated “model” net pressure • Observed net pressure obtained from surface or downhole treatment pressure
Net Pressure Matching
• Provide “anchor points” for real-data (net pressure) analysis • Obtain accurate measurement of the true net pressure in the fracture • On site diagnosis and remediation of proppant placement – Near-wellbore tortuosity – Perforation friction – fluid leakoff • Bottom line: provide accurate estimates of the fracture geometry
Purpose Of Diagnostic Injections
0.00 0
4.00 600
8.00 1200
50.00
58.00
Time (mins)
66.00
74.00
Closure ?
82.00
Leak-off ? 90.00
0.0
40.0
80.0
120.0
200.0
12.00 1800
Friction ?
Slurry Rate (bpm)
160.0
Net pressure ?
Proppant Concentration (ppg) Surface Pressure (psi)
16.00 2400
20.00 3000
“Typical” Fracture Treatment Data
End Frac Rate Stepdown / Pressure Decline Monitoring
Diagnostic Step Breakdown Injection / rate stepdown / pressure decline Crosslinked Gel Minifrac with proppant slug / rate stepdown / pressure decline ~100-500 Bbl fracture fluid including 25-50 Bbl proppant slug (possible range 0.5-5 PPG) Minimum of 10 minute decline data
New areas Real-time pad resizing TSO treatments
Always
Fluid & Volume ~50-100 Bbl KCl
When Always
Purpose / Results Establish injectivity; obtain small volume ISIP; estimate closure pressure and formation permeability. Leakoff calibration; Net pressure sensitivity to volume and crosslink gel; Characterize fracture entry friction; Evaluate near-wellbore reaction to proppant; Screen out or erode near-wellbore multiple fractures. Characterize fracture entry friction; Post-frac leakoff calibration.
Recommended Diagnostic Injection Procedures
0 0.0
2000 20.0
4000 40.0
6000 60.0
8000 80.0
10000 100.0
0.0
Rate
70.0
Time (mins)
140.0
Pulses ?
Step-down Test
Surf Pressure (psi) Slurry Rate (bpm) Breakdown Mini-Frac Injection
210.0
Proppant
Proppant Slug ?
280.0
Surface Treating Pressure
Step-down Test
350.0
Step-down Test
Prop Conc (ppg)
0.00
4.00
8.00
12.00
16.00
20.00
History Matching “Anchor Points”: Shut-in Pressure Decline Slope and Net Pressure Level
Time (min)
120.0
150.0
0.00 0 90.0
0.00 0.0 0
60.0
5.00 500
5.00 25.0 500
30.0
10.00 1000
10.00 50.0 1000
0.0
15.00 1500
15.00 75.0 1500
25.00 2500
20.00 2000
Prop Conc (ppg) Net Pressure (psi)
20.00 100.0 2000
25.00 125.0 2500
Btm Prop Conc (ppg) Slurry Rate (bpm) Observed Net (psi)
History Matching “Anchor Points”: Shut-in Pressure Decline Slope and Net Pressure Level
• “Decline Slope” parameters – Permeability – Wallbuilding coefficient (Cw) – Pressure-dependent leakoff (Multiple fracture leakoff factor) • “Level” parameters – (Sand-shale) Closure stress contrast – Fracture complexity (Multiple fracture opening/volume factor) – Tip effects coefficient – Proppant drag exponent – Tip screen-out backfill coefficient – (Young’s modulus) • “Geometry” parameters – Composite layering effect – Crack opening / width coupling coefficient
FracproPT Net Pressure Matching Parameters
– Level (low perm): stress contrast, proppant drag – Level (high perm): TSO backfill, Young’s modulus, stress contrast, proppant drag – Decline slope: Pressure-dependent leakoff – Geometry: composite layering effect, width decoupling
• Prop frac:
– Level: Tip effects, Fracture complexity – Decline slope: Wallbuilding coefficient Cw
• Minifrac
– Level: Tip effects, Fracture complexity – Decline slope: permeability
• B/D Injection
Net Pressure Matching Strategy
5-1/2” casing frac string; 40’ perf interval shot with 4 SPF, 90°° phasing, 0.31” diameter holes Disappointing production performance for expected 600 ft fracture half-length (based on fracture growth design without real-data feedback) Sand/shale stress contrast much lower than estimated, resulting in significant fracture height growth and a much shorter fracture half-length (250’) Utilize fracture pressure analysis to optimize fracture treatment design
• Completion:
• Situation:
• Diagnosis:
• Solution:
Hard sandstone @ 7600’ (gas) in West Texas
• Formation:
Example Application – Estimation of Realistic Fracture Length
Geometry inferred design without real-data feedback
Time (min)
80.0
100.0
0 0.00 60.0
0.00 0.0
40.0
400 10.00
10.00 20.0
20.0
800 20.00
20.00 40.0
0.0
1200 30.00
30.00 60.0
2000 50.00 1600 40.00
Net Pressure (A) (psi) Prop Conc (ppg)
40.00 80.0
50.00 100.0
Btm Prop Conc (ppg) Slurry Rate (bpm)
High stress contrast 0.3 psi/ft (based on Dipole Sonic log interpretation)
Example Application: Estimation of Realistic Fracture Length
Geometry inferred design without real-data feedback
Time (min)
80.0
100.0
0.00 0.0 60.0
0 0.00 0
40.0
10.00 20.0
400 10.00 400
20.0
20.00 40.0
800 20.00 800
0.0
30.00 60.0
1200 30.00 1200
50.00 100.0 40.00 80.0
Btm Prop Conc (ppg) Slurry Rate (bpm)
1600 40.00 1600
2000 50.00 2000
Net Pressure (A) (psi) Prop Conc (ppg) Observed Net (psi)
Observed net pressure does not match design net pressure response
Example Application – Estimation of Realistic Fracture Half-Length
Geometry inferred from net pressure matching
Geometry inferred design without real-data feedback
0.0
40.0
60.0
80.0
0 0.00 100.0 0
0.00 0.0 0
Lower stress contrast (0.1 psi/ft) required to match observed net pressure Confirmed with shale stress test in subsequent wells
Time (min)
400 10.00 400
10.00 20.0 400
20.0
800 20.00 800
20.00 40.0 800
1200 30.00 1200
30.00 60.0 1200
2000 50.00 2000 1600 40.00 1600
Net Pressure (A) (psi) Prop Conc (ppg) Net Pressure (psi)
40.00 80.0 1600
50.00 100.0 2000
Btm Prop Conc (ppg) Slurry Rate (bpm) Observed Net (psi)
Example Application – Estimation of Realistic Fracture Half-Length
• Closure stress σmin determines minimum pressure to open a fracture • Usually closure increases with depth • Closure stress is lithology dependent (shales usually higher than sands) • Represents only the minimum principal stress component in the vicinity of the well
Closure Stress Profile
• Closure stress profile determines fracture shape – Radial if stress profile is uniform (theoretical decrease in net pressure with pump time) – Confined height growth if closure stress “barriers” are present (theoretical increase in net pressure with pump time) • Effectiveness of “barrier” determined by – Closure stress contrast – Level of net pressure • “Typical” sand-shale closure stress contrast 0.05 - 0.1 psi/ft – Higher if there has been significant depletion (~2/3 of pore pressure change) – Lower if sands and shales are not clean • When do you change it? – Increase contrast when net observed pressures are higher – Increase contrast when fracture is more confined (up to 1.0 psi/ft)
Matching Parameter -Closure Stress Profile
• Modulus should be obtained from static tests (preferably similar to fracturing conditions) – Dynamic modulus two times or more larger than static modulus (use with caution !) • Once modulus is determined, this should be a FIXED parameter in a net pressure matching procedures • An increase in Young’s modulus results in less fracture width (for the same net pressure) • For simple radial model: Lfrac ∝ E1/3 (for the same net pressure) • Modeling results not extremely sensitive to modulus. • When do you change it? – With low moduli in GOM environment when modulus uncertainty is high – Character of TSO net pressure slope depends on modulus
Main Input Parameter - Young’s Modulus
GR.......................Vshale ........................Φ , E ,ν , σ , CLE , K Ic
• Calculation logic for GR-only log data (for sand-shale reservoirs):
Φ N ......................Φ, E...................... Sw , k Rt ..................................................... GR.......................Vshale ........................ν , σ , CLE , K Ic
• Calculation logic for triple-combo log data:
GR.......................Vshale ........................K Ic
Φ D or ρ b ..............M........... Φ.......... Φ N .................................. Sw , k Rt ....................................................
Tcomp ................................................ ν , σ , CLE Tshear ..................... E........................
• Calculation logic for quad-combo log data:
Developing an Earth Model from Log Data
2
2
( VP - VS )
=
2
2
2 ( VP - VS )
2
VP - 3 VS
2
Poisson’s Ratio
E=
2
2
VS ( 3 VP - 4 VS )
2
Young’s Modulus
VP -- Compressional Wave Velocity VS -- Shear Wave Velocity -- Density
Obtained From Logs or Tomograms
Calculating Dynamic Modulus
= 1-
(
Elastic Behavior No History Effects No Thermal Stresses No Strain B.C.
Assumptions
Hmin
OV
OV
P) +
2
P+
T
= 1.05 x Depth (ft)
1
= 0.2 P = 0.45 x Depth (ft) 1 = 2 = 0.9 T = Derived Value
-
STANDARD UNIAXIAL STRAIN
Estimating In Situ Stress from Logs
• If permeability profile is “known”, use Kp/Kl ratio for matching instead • Fix by matching decline slope of B/D KCl injection • Adjust Cw to match decline for gelled fluids
– only change permeability in pay interval.
• Keep it simple:
– Relative permeability issues – Opening of natural fractures – Relies on many other assumptions
• Matching perm is “permeability under fracturing conditions” – not necessarily under production conditions
Main Input Parameter – Permeability, Cw
High Leakoff, 25% Fluid Efficiency
Moderate Leakoff, 50% Fluid Efficiency
Low Leakoff, 65% Fluid Efficiency
Effect of Leakoff
• When do you change it? – Increase from default 0.0001 up to 0.4 when observed net pressure is lower than model (w/o multiples) – When fluid viscosity change has significant effect on observed net pressure behavior
• Tip process zone (with opening fractures) slows down fracture growth • Non-linear rock behavior at large differential compressional stress
• How does it work? – This parameter controls the near-tip pressure drop and thus the net pressure level in the fracture. – Mimics increased fracture growth resistance at the tip
Main Matching Parameters – Tip Effects Coefficient (Gamma 2)
pfrac
σH,min
Fluid Lag
Cohesive Zone
σH,max
Shielding of process zone, crack bridging and offsets
High Shear Stress: Plastic Zone
Tip Effects
wfrac
pnet
Linear elastic model
Lf
Lf Non-linear elastic model
Linear elastic model (Gamma 2 = 0.4)
Non-linear elastic model (Gamma 2 = 0.0001)
Net pressure decline slope w/ distance represents Gamma 2)
Tip Effects Coefficient
Tip Effects - Increased Fracture Growth Resistance
• Experiments by Shlyapobersky reveal fracture process zone • Process zone is scale dependent, and results in multiple fractures ahead of hydraulic fracture tip • Can result in higher net pressures to propagate fracture
Process Zone Around Fracture Tip
• Only change during injections • Tie opening and volume factors for “point source” perfs • Tie leakoff and volume factors for “distributed limited entry” perfs
• How does it work? – Opening and volume factor control the degree of fracture complexity using the amount of overlapping “equivalent” (equal sized) fractures – Leakoff factor can mimic increase leakoff or pressure-dependent leakoff • When do you change it? – When observed net pressure with default Gamma 2 (0.0001) is significantly higher than model net pressure – Use specific starting points for distributed limited entry and point source perforation strategies – Use strict rules
Main Matching Parameter – Multiple Fractures
Multiple Hydraulic Fractures In FracproPT
200 psi
1000
4 ft
400
Failure Zone Around Tip
Offsets at Natural Fractures
Regeneration Due to Plugging
Speculation On Genesis Of Multiple Fractures
1
2
3
3
3
3
Equivalent number of spaced identical fractures without interference
Equivalent number of fractures competing For width
Equivalent number of fractures with leakoff (ML)
Equivalent number of growing multiple fracs (MV)
Situation
3
2
1
Equivalent number of fracs competing for width (MO)
Modeling Approach for Multiple Hydraulic Fractures
1-Fracture
3-Fractures 2-Fractures
4-Fractures
Measured Net Pressure
Effect of Multiple Fractures
• • • • •
Conclusion: multiple fractures may be the rule rather than the exception
Core through and mineback experiments Direct observations of multi-planar fracture propagation Fracture growth outside plane of wellbore Observation of high net fracturing pressures Continuous increases in ISIPs for subsequent injections
Evidence for the Simultaneous Propagation of Multiple Hydraulic Fractures
NEVADA TEST SITE HYDRAULIC FRACTURE MINEBACK
Physical evidence of fractures nearly always complex
Observations of Fracture Complexity
NEVADA TEST SITE HYDRAULIC FRACTURE MINEBACK
Physical evidence of fractures nearly always complex
Multiple Strands in a Propped Fracture (Vertical Well)
Courtesy: N.R. Warpinski, Sandia Labs
NEVADA TEST SITE MINEBACK
Multiple Hydraulic Fracture Strands in a Horizontal Well
M-Site Experiment
Physical evidence of fractures nearly always complex
Multiple Strands in a Propped Fracture (Vertical Well)
– Confined fracture height growth – Increased fracture closure stress due to pore pressure increase – Higher Young’s modulus than anticipated – Fracture tip effects – Tip screen-out initiation – Simultaneously propagating multiple hydraulic fractures
• Potential causes for high net pressures:
Use Multiple Hydraulic Fractures Prudently for Modeling Purposes
• How does it work? – Mimics the increase in frictional pressure drop along the fracture as proppant is introduced – Controls how much the proppant in the fracture slows the fracture length and height growth. – Separate terms for Upper and Lower height growth calculated. Length effect is based on average of upper and lower terms. – Once a stage has become packed with sand (“immobile proppant bank”), there is no more growth in that direction – If both an upper and lower stage are dehydrated, quadratic backfill model takes over (if enabled) • When do you change it? – Significant proppant induced observed net pressure increase during proppant stages (that is not due to TSO)
Main Matching Parameters – Proppant Drag Exponent
Effect of Proppant Drag
Drag = 2
Drag = 6
Drag = 10
Drag = 14
Effect of Leakoff
Low Leakoff
High Leakoff
– Increase it when the TSO-induced observed net pressure rise is steeper than model predicts
• When do you change it?
– When fracture height and length growth are stopped due to dehydration of an upper and lower stage, quadratic backfill model starts working (if enabled) – Quadratic backfill is based on the idea the the fracture dimension controlling fracture stiffness will decrease as the fracture fills with immobile packed proppant from the tip back to the wellbore.
• How does it work
Main Matching Parameter – Quadratic Backfill Exponent
DBF=0
DBF=0.5
Effect of Quadratic Backfill
Linear TSO response
Height Growth due to Leverage
Fracture closure stress/ permeability barrier Interface slippage
Composite layering / width decoupling
Fracture Height Confinement Mechanisms
Poorly Understood Critical Model Input Parameters
Occurs with Height Growth
– Increase in layer adjacent to pay zone if no other confining mechanism can explain actual level of fracture confinement Composite Mechanisms: – Keep unity in pay zone
• When do you change it ?
– This parameter controls the near-tip pressure drop in each individual layer
• How does it work ?
Main Matching Parameters – Composite Layering Effect
NEVADA TEST SITE HYDRAULIC FRACTURE MINEBACK
Fracture Complexity Due To Joints
δ
pnet R
δ = Wcγ1 pnetR/ E
– Decrease it to trade fracture width for half-length – Decrease it to mimic reduced coupling “shear-decoupling” over fracture height (also associated with use of composite layering effect)
• When do you change it ?
– Multiplier for Gamma 1 representing how fracture width is decoupled along fracture height – We will provide automatic correlation as a function of composite layering effect
• How does it work ?
New Matching Parameter – Width Coupling Coefficient
• “We analyzed the treatment and determined optimum frac design” – Optimization is an evolutionary process, completed over the course of a series of fracture treatments
– Results usefulness determined 90% by engineer, 10% by model
The analysis is credible because I used the ‘FracRocket’ model”
Or
• “You used the wrong frac model !”
• “You can get any answer you want” – Not if you are constrained by real-data feedback, engineering judgment, and the results of other fracture diagnostics !
Net Pressure Analysis Untruths
• Production data & welltest analysis • Direct fracture diagnostics
– Indirect Diagnostic Technique - frac geometry inferred from net pressure and leakoff behavior – Solution non-unique – careful & consistent application required for useful results – Technique most useful when results are integrated or calibrated with results of other diagnostics
• Net Pressure History Matching
– Using surface pressure increases results uncertainty – Problematic near-wellbore friction level variable
• Fracture Entry Friction Evaluation
Fracture Pressure Analysis - Limitations
– ? Modulus, stress, leakoff, and multiple fractures – ? Layer interface mechanisms
• Appropriate Mechanisms for Net Pressure History Matching
– Pipe friction vs. perforation friction – Identifying marginally unfavorable entry friction
• Minimizing diagnostic injection time & cost without compromising effectiveness • Differentiating between “engineering” and “science” • Unclear fracture closure pressure • Practical bottom hole pressure measurement • Surface pressure rate stepdown complications
Fracture Pressure Analysis Problems / Opportunities
• Measurement of real-data is relatively simple and cheap • The right analysis assumptions and a consistent approach can get you “on the right page”, but geometry require calibration with direct measurements
– Reducing screen-out problems – Improving production economics – Achieving appropriate fracture conductivity
• Benefits of real-data fracture treatment analysis can be enormous
Fracture Analysis - Conclusions
Fracture Conductivity – the key to frac design
• Propped Fracture Width is Primarily a Function of Proppant Concentration
wkf = fracture width x fracture permeability
• Fracture Conductivity, wkf
Important Parameter Is Relative Fracture Conductivity At Reservoir Conditions
Conductivity (Cf) is a measure of the fracture’s ability to transmit fluids
cf = kf * wf wf
Fracture Conductivity
kf
FCD =
kf
k f * wf kform * xf
wf
Dimensionless Fracture Conductivity (FCD) is a measure of the contrast between the flow capacity of the fracture and the formation
xf
kform
Why is Conductivity Important?
or
wkf Cr = πkL
For FCD > 30 or Cr > 10, Lf is infinite conductive - No Significant Pressure Drop in Fracture - Value of 1.6 or larger generally sufficient
Lf = Fracture Half-Length, ft
k = Formation Permeability, md
wkf = Fracture Conductivity, md-ft
wkf FCD = kLf
Dimensionless Fracture Conductivity (FCD) Is Used To Design Fracture Treatments
0.01 0.1 0.2
0.03 0.02
0.05
0.1
0.3 0.2
0.5
1
0.5 1 2 5 10 20 (Kp)(Wf) / (Xf)(Kf) Fcd Fcd = (K=f)(W f) / (Xf)(Kform)
50 100
Increasing Effectiveness of the Fracture
Prats Correlation
Prats, M.: "Effect of Vertical Fractures on Reservoir Behavior-Incompressible Fluid Case," paper SPE 1575-G
rw' / Xf
Frac design change with same amount of proppant
Increase in frac length
Increase in conductivity
Need Length Or Conductivity? (After McGuire&Sikora)
Productivity increase
Need long fractures
Dimensionless conductivity “easily” greater than 10 – Fracture conductivity generally not an issue – “Self propping” (water) fractures may already provide sufficient conductivity
Treatment design – Moderate pad size (avoid long closure times on proppant) – Relatively low maximum proppant concentrations – Poor quality proppant can be OK (if closure stress is relatively low) – Pump rate not very critical
•
•
•
Design In Low-permeability Formation
• •
Sufficient fracture conductivity is critical Treatment design – Minimum pad size to create TSO (Tip Screen-Out) based on crosslink gel minifrac – Use best possible (and economic) proppant for expected closure stress – Larger diameter proppant provides more conductivity and reduces proppant flowback problems – Use high maximum proppant concentrations – Use of large casing frac string makes achieving TSO difficult for small treatments – Pump rates generally high, but can be decreased to initiate TSO
Design In High-permeability Formation
– – – – – – – – –
Closure Stress Embedment Crushing (generates fines and damages proppant) Corrosion Gel Residue Plugging Convection Proppant Settling Multiphase flow effects Turbulent flow
• Conductivity is reduced by
Fracture Conductivity In The Reservoir
• • • • •
Reference: API RP-61
Steel pistons 2 lb/ft2 proppant loading Stress maintained for 15 minutes Ambient temperature Extremely low water velocity (2 ml/min)
API 15-Minute Conductivity Test
1. 2. 3. 4. 5. 6. 7. • •
Ambient temperature Extremely low water velocity (2 ml/min)
Embedment, Duration, Temperature Non-Darcy Flow Reduced Proppant Concentration Multiphase Flow Gel Damage • Steel pistons Fines Migration • Stress maintained for only 15 minutes Cyclic Stress
To obtain a realistic proppant conductivity for design, the API test results must be modified to account for:
Problem
– – – – • • •
Embedment Duration Temperature.
Stim-Lab Consortium 40+ members from industry companies Developed and published a modified procedure in SPE 16415 Modified API test to address:
Deficiencies of the API conductivity testing recognized
1. Embedment, Duration, Temperature
Modified API RP61 Conductivity Test
References: Stim-Lab Consortia Feb 2002 1.6-46, SPE 16415
With proppant concentrations of 1 lb/ft2 (5 kg/m2) and soft core, 90% loss of conductivity has been observed.
Spalling
a) From Steel Plate to Sandstone core; allows modest embedment and spalling
Test Improvements:
Embedment/Spalling
References: SPE 16415, 14133
Longer test captures a portion of the time-dependent decline
b) Test duration increased to 50 hours (from 15 minutes)
Test Improvements:
Duration
Conductivity (md-ft)
0
25
50
75
20/40 Jordan sand, 8000 psi
100 Hours at Constant Stress
100
1000
Fig 4, SPE 16415
•
•
Reference: Stim-Lab Consortia Feb 2002 Fig 1.7-8
Uncoated and resin-coated sand show degradation at high temperatures. Ceramic proppants are manufactured at ~2700°F (1500°C) and are unaffected by reservoir temperature.
c) Realistic temperatures 150° F Sands 150-250° F Resin Coat 250° F Ceramics
(was ambient):
Test Improvements
0
0.2
0.4
0.6
0.8
1
0
2
4 6 8 10 Stress (x1000 psi)
250F (121C) 300F (149C) 350F (177C)
12
14
Temperature Degradation of Premium Precured Resin Coated Sand
Temperature
P e rm e a b ility Im p a c t
1500
7000
Jordan Sand
1137
5715
CarboLITE
API Test 50 Hour Test 6 Conditions: YM=5e psi, zero gel damage, 250°F, 2 lb/ft 2, 6000 psi YM=34e3 MPa, zero gel damage, 121°C, 10 kg/m 2, 41 MPa
0
1000
2000
3000
4000
5000
6000
7000
1) API Test versus Modified 50-hour Test
~20 to 30% reduction against hard core and modest conditions
References: ST Sand: SPE 14133, 16415, CL: Carbo typical, LT: Stim-Lab PredK 2002
Effective Conductivity (md-ft)
1. 2. 3. 4. 5. 6. 7.
Embedment, Duration, Temperature Non-Darcy Flow Reduced Proppant Concentration Multiphase Flow Gel Damage Fines Migration Cyclic Stress
To obtain a realistic proppant conductivity for design, the API test results must be modified to account for:
Problem
∆ P/L = µ v / k + β ρ v2
In realistic tests, the fluid velocity is high. Pressure losses are dominated by acceleration (inertial effects), and are described by Forchheimer’s Equation. This departure from Darcy’s Law can be considered a loss of effective conductivity.
∆ P/L = µ v / k
In the API test, the fluid velocity is extremely low. Pressure losses are dominated by friction, and can be described by Darcy’s Law.
2) Non-Darcy Flow (Inertial Effects)
1137
0
1000
50 Hour Test
672
3481
CarboLITE
Jordan Sand
Inertial Flow with Non-Darcy Effects
Realistic flowrates also consider fluid acceleration.
2000
3000
Low velocity testing measures only friction.
5715
4000
5000
6000
7000
2) Non-Darcy Flow (Inertial Effects)
~40% reduction for low productivity dry gas well
References: Stim-Lab PredK 2002, Forchheimer effect, SPE 54630, 77675
Conditions: YM=5e6 psi, zero gel damage, 250°F, 2 lb/ft 2, 6000 psi, 250 mcfd, 1000 psi bhfp, 20 ft pay YM=34e3 MPa, zero gel damage, 121°C, 10 kg/m 2, 41 MPa, 7000 m3/d, 7 MPa bhfp, 6 m pay
Effective Conductivity (md-ft)
• It is likely that there are some unpropped regions, which increases the stress, crush, and embedment of the surrounding grains. • The following plot shows the effect of reducing the concentration but maintaining a uniformly packed fracture.
• In the API test, proppant is uniformly distributed with a concentration of 2 lb/ft2, or 10 kg/m2. • In actual fractures, the achieved proppant concentration may be much lower.
3) Effect of Lower Proppant Concentration
Effective Conductivity (md-ft)
2 lb/sq ft (10 kg/sq m)
672
3481
225
1243
CarboLITE
1 lb/sq ft (5 kg/sq m)
Jordan Sand
References: Stim-Lab PredK 2002, Forchheimer effect, SPE 54630, 77675
0
1000
2000
3000
4000
5000
6000
7000
3) Effect of Lower Proppant Concentration
Non-linear, as pressure drop function of velocitysquared, and embedment more significant
~65% damage for cutting concentration by 50%.
0
1000
2000
3000
4000
5000
6000
7000
Dry Gas
225
1243
liquid
gas
Multiphase Flow
49
479
CarboLITE
Jordan Sand
4) Effect of Multiphase Flow
~60 to 80% reduction for modest liquid rates
References: Stim-Lab PredK 2002, Forchheimer effect, SPE 54630, 77675
Conditions: YM=5e6 psi, zero gel damage, 250°F, 1 lb/ft 2, 6000 psi, 250 mcfd, 1000 psi bhfp, 20 ft pay, 10 blpd YM=34e3 MPa, zero gel damage, 121°C, 5 kg/m 2, 41 MPa, 7000 m3/d, 7 MPa bhfp, 6 m pay, 1.6 m3l/d
Effective Conductivity (md-ft)
0
1000
2000
3000
4000
5000
6000
7000
Clean Pack
49
479 14
144
CarboLITE
Jordan Sand
50% Gel Damage
5) Effect of Gel Damage
~70% damage for 50% loss in laminar flow. (Gel damage affects beta more than perm)
References: Stim-Lab PredK 2002, Stim-Lab SEM photos
Conditions: YM=5e6 psi, 50% gel damage, 250°F, 1 lb/ft 2, 6000 psi, 250 mcfd, 1000 psi bhfp, 20 ft pay, 10 blpd YM=34e3 MPa, 50% gel damage, 121°C, 5 kg/m 2, 41 MPa, 7000 m3/d, 7 MPa bhfp, 6 m pay, 1.6 m3l/d
Effective Conductivity (md-ft)
0
1000
2000
3000
4000
5000
6000
7000
No Fines
14
144
Modest Fines
7
RC Sand
130
Ceramic
CarboLITE
Jordan Sand
6) Effect of Fines Migration/Plugging
Uniformly sized, spherical proppants less susceptible to plugging. Larger pore throats reduce bridging.
References: Stim-Lab thin section photos, SPE 24008, 3298, 7573, 11634
Conditions: YM=5e6 psi, 50% gel damage, 250°F, 1 lb/ft 2, 6000 psi, 250 mcfd, 1000 psi bhfp, 20 ft pay, 10 blpd YM=34e3 MPa, 50% gel damage, 121°C, 5 kg/m 2, 41 MPa, 7000 m3/d, 7 MPa bhfp, 6 m pay, 1.6 m3l/d
Effective Conductivity (md-ft)
0
1000
2000
3000
4000
5000
6000
7000
130
Single Stress Cycle
7
25 Cycles
4
CarboLITE
96
Jordan Sand
7) Effect of Cyclic Stress
Stronger proppants are less damaged by repeated stress cycles.
References: CARBO Tech Rpt 99-062, StimLab July 2000, SPE 16912, 19091, 22850
Conditions: YM=5e6 psi, 50% gel damage, 250°F, 1 lb/ft 2, 6000 psi, 250 mcfd, 1000 psi bhfp, 20 ft pay, 10 blpd YM=34e3 MPa, 50% gel damage, 121°C, 5 kg/m 2, 41 MPa, 7000 m3/d, 7 MPa bhfp, 6 m pay, 1.6 m3l/d
Effective Conductivity (md-ft)
Effective Conductivity (md-ft)
API Test
1500
7000
Modified 50-Hour Test
1137
5715
"Inertial Flow" with Non-Darcy Effects
672
3481
Lower Achieved Width (1 lb/sq ft)
225
Multiphase Flow
49
479
50% Gel Damage
14
7
130
Fines Migration / Plugging
144
99.73%
Cyclic Stress
4
0.001 D-m reduction
96
98.63%
0.029 D-m reduction
Effective conductivities can be less than 1% of API test values
Conditions: YM=5e6 psi, 50% gel damage, 250°F, 1 lb/ft 2, 6000 psi, 250 mcfd, 1000 psi bhfp, 20 ft pay, 10 blpd YM=34e3 MPa, 50% gel damage, 121°C, 5 kg/m 2, 41 MPa, 7000 m3/d, 7 MPa bhfp, 6 m pay, 1.6 m3l/d
1243
CarboLITE
Jordan Sand
References: ST Sand: SPE 14133, 16415, CL: Carbo typical, LT: Stim-Lab PredK 2002, SPE 24008, 3298, 7573, 11634, CARBO Tech Rpt 99-062, Run #6542, StimLab July 2000, SPE 16912, 19091, 22850
0
1000
2000
3000
4000
5000
6000
7000
Cumulative Conductivity Reductions
•
Gel-plugged tip
“Equivalent” infiniteconductivity frac
“Apparent” frac matched to production data, assuming apparent conductivity of 10 md-ft
Cleaned up / Flowing length is likely lower
Slurry / Propped Length may be lower
Mapped half-length
Caveat: Assumes single, planar frac, homogeneous reservoir
Effective Fracture Length
0.720
Time (days)
1.080
1.440
1.800
2000 8000
0 0 0.360
Test
Model
3000 12000
4000 16000
5000 20000
0 0
Test
Model
Production Surf Pres (psi) Production Gas Rate (Mscf/d)
1000 4000
0.000
(scale = 0-20,000 M CFD)
Gas Rates
(scale = 0-5000 psi)
Tubing P ressures
Calc'd Toph Press (psi) HC Rate (Mscf/d)
1000 4000
2000 8000
3000 12000
4000 16000
5000 20000
Production Modeling
• Finite-Difference • Numerical Solution to Diffusivity Equation • Reservoir As Grid System • Single Well Within Rectangular Grid System • Single Flowing Phase • 2-D • Unfractured and Hydraulically Fractured Wells • Fracture Input From FracproPT • Proppant Crushing • Non-Darcy and Multi-Phase Flow Effects in Fracture • Fracture Face Clean-up
Production Modeling - ReservoirPT
Oil Rate (bbl/day)
1
10
100
1000
10
Transient Flow
100 Time (days)
Boundary Influenced Flow
High Conductivity Fracture
1000
100 ac
Log-Log Rate versus Time Plot Transient & Boundary Influenced Flow
200 ac
10000
360 ac
2300 ac
Oil Rate (bpd)
1
10
100
1000
0
1000
2000
3000
4000
100 ac
Time (days)
5000
6000
High Conductivity Fracture
7000
200 ac
9000
360 ac
2300 ac
8000
Semi-Log Rate versus Time Plot Transient & Boundary Influenced Flow
10000
Oil Rate (bbl/day)
1
10
100
1000
10
No Fracture
100
Low Conductivity Fracture
High Conductivity Fracture
Time (days)
1000
360 acres
10000
Beginning of Boundary Influenced Flow
High & Low Conductivity Fracture & Un-fractured Case
Log-Log Rate versus Time Plot Transient & Boundary Influenced Flow
Rate (bbl/day)
1
10
100
1000
0
360 acres
1000
2000
3000
Low Conductivity Fracture
4000
High Conductivity Fracture
Time (days)
5000
No Fracture
6000
7000
8000
High & Low Conductivity Fracture & Un-fractured Case
Semi-Log Rate versus Time Plot Transient & Boundary Influenced Flow
9000
10000
Fracture Mapping & Model Calibration
H?
W? L? pnet
Pay
Pay
Analogies Between Hydraulic Frac and Balloon
H?
W?
pnet
L? pnet
R?
Pay
Pay
Analogies Between Hydraulic Frac and Balloon
Some balloons have a tendency to move up
Mother Nature’s Birthday Party
Some show a huge length-height aspect ratio …
Mother Nature’s Birthday Party
… while others show high levels of complexity
Mother Nature’s Birthday Party
Some grow in a specific way in the US …
Mother Nature’s Birthday Party
… and quite differently in the rest of the world
Mother Nature’s Birthday Party
Incomplete coverage
T-shaped fractures
Horizontal fractures
Perfectly confined frac
Poor fluid diversion
Multiple fractures dipping from vertical
Twisting fractures
Out-of-zone growth
Why Map Fracs? Why Model Fracs?
FRACTURE DIAGNOSTICS
conductive liquidexcitation electrode
gas bubble
Pick-up electrodes
Induced tilt reflects the geometry and orientation of created hydraulic fracture
Hydraulic fracture induces a characteristic deformation pattern
Fracture
Downhole tiltmeters In offset well
Fracture-induced surface trough
Principle of Tilt Fracture Mapping Direct Fracture Diagnostic Technique
• Measure frac height, length and azimuth in real-time
FracSeis Microseismic Fracmapping
SOLUTION: Calibrate model
PROBLEM: Physics of model not consistent with reservoir
SOLUTION: Spend time and money to obtain better inputs
PROBLEM: Poorly defined input parameters
Why Bad Models Happen to Good Engineers
Captain, my frac modeling builds a mountain of results on a molehill of inputs
Use some fudge factors and let’s frac this well
Fracture Models Sometimes Need Calibration
• • • • • • • • • • • •
Fluid rheology Wallbuilding coefficient Pressure-dependent leakoff Closure stress in pay Young’s modulus Permeability and pore pressure Closure stress in neighboring layers Fracture complexity Tip effects Proppant drag Composite layering Fracture width decoupling
Critical Model Input Parameters
Improve Measurements
Impossible to measure directly and physics not well understood
Harder to measure directly and less reliable
Relatively easy & reliable measurement
Color Key:
Too many knobs to turn
Why Bad Models Happen to Good Engineers
Grasshopper, Now You Must Choose!
• • • • • • • • • • • •
Fluid rheology Wallbuilding coefficient Pressure-dependent leakoff Closure stress in pay Young’s modulus Permeability and pore pressure Closure stress in neighboring layers Fracture complexity Tip effects Model Calibration Proppant drag Composite layering Fracture width decoupling
Impossible to measure directly and physics not well understood
Harder to measure directly and less reliable
Relatively easy & reliable measurement
Color Key:
• • • •
Net pressure Fracture length Fracture height Fracture width and conductivity
Directly Measured Model Outputs
Improve Measurements
Critical Model Input Parameters
Knobs “locked in” by improved measurements
Why Bad Models Happen to Good Engineers
• • • • • • • • • • • •
Fluid rheology Wallbuilding coefficient Pressure-dependent leakoff Closure stress in pay Young’s modulus Permeability and pore pressure Closure stress in neighboring layers Fracture complexity Tip effects Model Calibration Proppant drag Composite layering Fracture width decoupling
Impossible to measure directly and physics not well understood
Harder to measure directly and less reliable
Relatively easy & reliable measurement
Color Key:
• • • •
Net pressure Fracture length Fracture height Fracture width and conductivity
Directly Measured Model Outputs
Improve Measurements
Critical Model Input Parameters
Knobs “locked in” by model calibration
Why Bad Models Happen to Good Engineers
D e pth (ft)
stress contrast
Stress Profile
Low
3400 1600
3380
3360
3340
3320
3300
3280
2300
Closure Stress (psi)
1950
High
Permeability
Perfs Perfs
2650
Large stress contrast Large sand-shale 3260
3240
3220
3200
3000
0
50
Downhole tilt
Downhole tilt analysis results
Length (ft)
100
150
0.00 0.10 0.20 0.30 0.40 0.50 0.60 0.70 0.80 0.90 1.0
Proppant Concentration (lb/ft²)
Pressure analysis
Pressure analysis results
Concentration of Proppant in each Fracture (lb/ft²)
Depleted Portion of Field
200
Perfs
Stress Profile
Low
3550 2000
3520
3490
3460
3430
3400
2250 2500 2750 Closure Stress (psi)
High
Permeability
stress contrast 3370SmallSmall sand-shale
3340
3310
3280
3250
3000
0
75
150 Length (f
1.2
225
0.00 0.20 0.40 0.60 0.80 1.0
1.4
1.6
Proppant Concentration (lb/ft²)
1.8
Fracture Half-length 95 ft Pressure analysis 6 “equivalent” fracture multiples
Pressure analysis results:
Downhole tilt
Concentration of Proppant in each Fracture (lb/ft²)
l
Un-depleted Portion of Field
–Confined fracture growth in significantly depleted sand
–Unconfined height growth in undepleted sand
•Different fracture height growth behavior in two wells is explained by pore pressure depletion
Sometimes the Models Work Without Calibration
2.0
300
Uncalibrated match
But Many Times Models Need Calibration DJ Basin
But Many Times Models Need Calibration DJ Basin
Calibrated match
But Many Times Models Need Calibration DJ Basin
But Many Times Models Need Calibration DJ Basin
Cotton Valley Taylor
Time (min)
160.0
12000
Tools
11800
11600
11400
11200
8/26/03
11000
240.0
320.0
400.0
Calibrated Model
Distance Along Wellbore (ft)
Wright #1-3 GR
frac is assumed to be symmetric
One On frac wing was not fully seen by MS mapping-
-1600
80.0
-1400
0.0
0
-1200
0
400
-1000
10800
-800
400
800
-600
10600
-400
800
1200
-200
10400
0
1200
-2000
Depth (ft)
Wright #1-3 1600
200
1600
400
10200
600
Woolf #1-9
-1800
2000
800
Net Pressure (psi)
1000
Observed Net (psi)
1200
2000
1400
10000
1600
Wright 1-3 Net Pressure Match
1800
11450
11400
11350
11300
11250
11200
Taylor Sands
Taylor Sands
Taylor Sands
GR_STGC (GAPI) 5
But Many Times Models Need Calibration Cotton Valley Taylor Sand
2000
Calibrated Model
But Many Times Models Need Calibration Cotton Valley Taylor Sand
Un-Calibrated Model
But Many Times Models Need Calibration Cotton Valley Taylor Sand
not predictive
Direct diagnostics
Calibrated models more realistically predict how fractures will physically grow for alternative designs
incomplete physical understanding
Fracture growth models
Calibrated Model Approach: Modeling and Measuring
• Model calibration can provide “Good Models to Good Engineers”
– Hopefully leading to improved physics in models
• Model calibration is currently only done empirically, by matching geometries
– Poor characterization of rock / reservoir / geology – Incomplete understanding of relevant physics, especially with respect to height growth
• Models of today are more sophisticated than 20 years ago, but often still do NOT accurately predict fracture growth
Conclusions
Questions ?
0.0 0
20.0 400
14.00
42.00
Net Pressure Match
Time (min)
28.00
Bottom hole proppant concentration
Rate
56.00
70.00
200
8500
8550
8600
8500
8550
8600
0
150
200
250
1.2
1.5
1.8
2.1
Proppant Concentration (lb/ft²)
100
0.30 0.60 0.90
50
2.4
300
Concentration of Proppant in Fracture (lb/ft²)
2.7
350
3.0
1
0
1
Width Profile (in)
Predicted Fracture Geometry
8450
8350
8300
8250
8200
8150
8100
8450
350
350
350
350
350
8400
Gamma Ray (API) 0 Temp 1 150 Temp 2 150 Temp 3 150 Temp 4 150 Temp 5 150
8400
8350
8300
0.00 8250 0
8200
4.00 400
8.00 800
16.00 1600
20.00 2000
40.0 800
Model Net Pressure
Actual Net Pressure
Btm Prop Conc (ppg) Observed Net (psi)
12.00 1200
0.00
Slurry Flow Rate (bpm) Net Pressure (psi)
60.0 1200
80.0 1600
100.0 2000
FracproPT Overview
Depth, TVD (ft)
Depth TVD (ft-TVD) Depth, (ft)
• Contains preloaded libraries of stimulation fluids, proppants, and rock properties for many lithologies
• Supports remote access via modem or internet
• Optimizes fracture treatment economics
• Integrated reservoir simulator for production forecasting and matching
• Performs near-wellbore tortuosity / perf friction analysis – allows identification and remediation of potential premature screenout problems
• Provides unique tool to capture what is learned from direct fracture diagnostics through calibrated model settings
• Estimates fracture geometry and proppant placement in real-time by net pressure history matching
FracproPT System - Highlights
Production Forecast or Match
Estimated Fracture Geometry
Treatment Schedule
FracproPT Economic Optimization
FracproPT Production Analysis
FracproPT Fracture Analysis
FracproPT Fracture Design
Production Data
Treatment Data
Wellbore Information Log/layer Information
Calibrated Model Settings
DataAcqPT Real-Time Data Acquisition
FracproPT Module Interaction
– Capturing the physics of details is not as important as honoring large-scale elasticity and mass balance – Calibrated simplified approximation with full 3D growth model, lab tests and field observations – Model calibration is now a continuous effort
• After development of pseudo-3D models (early 1980’s) the industry was jubilant as it was now known how fractures really behaved -- or not ? • Observed net pressures were consistently far higher than net pressures predicted by these models (discovered in early 1980’s) -- parameter sensitivity also inconsistent • Development of Fracpro started in 1980’s with the aim to honor the “message” contained in real-data
FracproPT Development Philosophy
• Fracture Temperature Model
• Fracture Leakoff Model(s)
• Fracture Growth Model(s)
• Perforation and NearWellbore Model
• Wellbore Model
• Multiple Fracture Model
• Backstress (poro-elastic) Model
• Acid Fracturing Model(s)
• Proppant Transport Model(s)
Fracture Modeling in FracproPT
– Making the right engineering assumptions is key – Garbage in = garbage out – The KEY is to honor the observed data with the most reasonable assumptions possible
• The FracproPT system contains several 2D models, a conventional 3D model, an adjustable 3D model incorporating “tip effects”, and a growing number of calibrated model settings • There is NO “FracproPT answer” • Designed for on-site engineering flexibility • Quality of results are more user-dependent than model dependent
FracproPT is Just a Tool
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