Drilling Engineering
Prepared by: Tan Nguyen
Drilling Engineering – PE 311
Turbulent Flow in Pipes and Annuli
Drilling Engineering
Prepared by: Tan Nguyen
When attempting to quantify the pressure losses in side the drillstring and in the annulus it is
worth considering the following matrix:
Frictional Pressure Drop in Pipes and Annuli
Drilling Engineering
Prepared by: Tan Nguyen
Laminar Flow: In this type of flow, layers of fluid move in streamlines. There is no microscopic
or macroscopic intermixing of the layers. Laminar flow systems are generally represented
graphically by streamlines.
Turbulent Flow: In turbulent flow, there is an irregular random movement of fluid in transverse
direction to the main flow. This irregular, fluctuating motion can be regarded as superimposed on
the mean motion of the fluid.
Turbulent Flow in Pipes – Newtonian Fluids
Introduction
Drilling Engineering
Prepared by: Tan Nguyen
Reynolds number, Re, is a dimensionless number that gives a measure of the ratio of inertial
forces to viscous forces. Reynolds number is used to characterize different flow regimes, such
as laminar or turbulent flow. Laminar occurs at low Reynolds number, where viscous forces are
dominant, and is characterized by smooth, constant fluid motion; turbulent flow occurs at high
Reynolds number and is dominated by inertial forces, which tend to produce chaotic eddies,
vortices and other flow instabilities.
For pipe
In field unit:
Definition of Reynolds Number
µ
ρ du
_
Re =
μ
duρ
_
928
Re =
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
If Re < 2,100 Laminar flow
Re = 2,100 – 4,000 Transition flow
Re > 4,000 Turbulent
Note that this critical Reynolds number is correct only for Newtonian fluids
Determination of Laminar/Turbulent Flow
cp.fluid,ofviscosity
inI.D.,pipe
ft/svelocity,fluidavg.
lbm/galdensity,fluidwhere
928
Re
=
=
=
=
μ
d
u
ρ
μ
duρ
_
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Relationship between shear stress and friction factor:
Pipe flow under laminar conditions:
Therefore,
Newtonian fluids flow in pipe under laminar flow conditions:
Hence,
This equation will be used to calculate the friction factor of Newtonian fluids flow in pipe under
laminar flow conditions.
Determination of Friction Factor - Laminar Flow
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
For turbulent flow, the friction factor can be calculated by using Colebrook correlation.
Where ε is the absolute roughness. ε/d is the relative roughness.
For smooth pipe, the relative roughness ε/d < 0.0004, the following equations can be used to
calculate the friction factor in turbulent flow
Re = 2,100 – 100,000:
Blasius approximation:
Re = 2,100 – 100,000:








+−=
fN
d
f Re
255.1
/269.0log4
1
ε
Determination of Friction Factor - Turbulent Flow
( ) 395.0log4
1
Re −−= fN
f
25.0
Re
0791.0
N
f =
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Determination of Friction Factor
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Determination of Friction Factor
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
From equation: , an equation of dp/dL can be expressed as
In field unit: . This equation can be used to calculate the frictional pressure drop
gradient for Newtonian and non-Newtonian fluids.
Combining this equation and the Blasius approximation gives
Note that the Moody friction factor is four times higher than the Fanning friction factor.
Determination of the Frictional Pressure Loss
25.0
2
928
8.25
0791.0








=
µ
ρ
ρ
dv
d
u
dL
dp
75.4
25.075.175.0
25.0
25.075.175.0
86241800 d
q
d
u
dL
dp µρµρ
==
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Example: Determine the frictional pressure drop in 10000ft of 4.5-in commercial steel drillpipe
having an internal diameter of 3.826in. If a 20 cp Newtonian fluid having a density of 9 lbm/gal is
pumped through the drillpipe at a rate of 400 gal/min
Solution:
Mean velocity:
Reynolds number:
Since Re > 2,100, the flow is under turbulent flow conditions.
Example
sft
d
q
u /16.11
826.3*488.2
400
488.2 22
===
17831
20
826.3*16.11*9*928928
Re ===
μ
duρ
_
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
From table 4.5, the absolute roughness for commercial steel pipe is ε = 0.000013 inches.
The relative roughness ε/d = 0.000013/3.826 = 0.0000034 < 0.0004 --> smooth pipe
Solve this equation for the Fanning friction factor: f = 0.00666
Thus the frictional pressure loss can be obtained by
Example








+−=
fN
d
f re
255.1
/269.0log4
1
ε
psiD
d
vf
D
dL
dp
pf 75610000*
826.3*8.25
16.11*9*00666.0
8.25
22
====∆
ρ
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Using Blasius approximation ,the equation becomes
Pressure drop: DP = dp/dL x D = (0.0777)(10,000) = 777 psi
Example
25.0
Re
0791.0
N
f =
25.0
2
928
8.25
0791.0








=
µ
ρ
ρ
dv
d
v
dL
dp
ftpsi
d
v
dL
dp
/0777.0
1800 25.0
25.075.175.0
==
µρ
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Using Blasius approximation ,the equation becomes
Pressure drop: DP = dp/dL x D = (0.0777)(10,000) = 777 psi
Example
25.0
Re
0791.0
N
f =
25.0
2
928
8.25
0791.0








=
µ
ρ
ρ
dv
d
v
dL
dp
ftpsi
d
v
dL
dp
/0777.0
1800 25.0
25.075.175.0
==
µρ
Turbulent Flow in Pipes – Newtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Hydraulic diameter is defined as:
Equivalent diameter by using hydraulic diameter method:
Equivalent Diameter for Annular Geometry – Hydraulic Diameter Method
Turbulent Flow in Pipes/Annuli – NonNewtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
From the momentum equation, frictional pressure drop for Newtonian fluid in the annulus is
For pipe flow, d1 --> 0 then
Comparing these two equations, the equivalent diameter an annulus can be obtained
Equivalent Diameter for Annular Geometry – From Momentum Equation
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids










−
−+
=
1
2
2
1
2
22
1
2
2
ln
500,1
d
d
dd
dd
u
dL
dpf µ
2
500,1 d
u
dL
dpf µ
=
( )1
2
ln
2
1
2
22
1
2
2
d
de
dd
ddd
−
−+=
Drilling Engineering
Prepared by: Tan Nguyen
From the narrow slot approximation, frictional pressure drop for Newtonian fluid in the annulus is
For pipe flow
Comparing these two equations, the equivalent diameter an annulus can be obtained
Equivalent Diameter for Annular Geometry – Narrow Slot Approximation
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
2
500,1 d
u
dL
dpf µ
=
( )12816.0 ddde −=
Drilling Engineering
Prepared by: Tan Nguyen
A fourth expression for the equivalent diameter of an annulus was developed by Crittendon.
When using Crittendon correlation, a fictitious average velocity also must be used in describing
the flow system.
Equivalent Diameter for Annular Geometry – Crittendon Correlation
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
1. Obtain apparent viscosity by combining the frictional pressure loss in
pipe (or annulus) for both Newtonian and Bingham Plastic models
2. Use apparent viscosity to determine Reynolds Number
Bingham Plastic Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
dd
v
d
v ypa
22515001500 22
τµµ
+=
)(
66.6
Pipe
v
dy
pa
τ
µµ +=
)(
)(5 12
Annulus
v
ddy
pa
−
+=
τ
µµ
or
Drilling Engineering
Prepared by: Tan Nguyen
Another way to determine the flow regime (critical Reynolds number) is to use the Hedstrom number
In field unit
Bingham Plastic Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
2
2
p
y
HE
d
N
µ
ρτ
=
2
2
37100
p
y
HE
d
N
µ
ρτ
=
Drilling Engineering
Prepared by: Tan Nguyen
Bingham Plastic Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
Turbulent
Drilling Engineering
Prepared by: Tan Nguyen
Apparent Viscosity for use in the Reynolds Number is obtained by comparing the laminar flow
equations for Newtonian and Power Law fluids
Pipe flow:
Annular flow:
Power Law Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
n
n
n
a n
d
vK
d
v





 +
= +
0416.0
/13
1440001500 )1(2
µ
)(
0416.0
/13
96
)1(
)1(
Pipe
n
v
Kd
n
n
n
a 




 +
= −
−
µ
n
n
n
a n
dd
vK
dd
v





 +
−
=
− +
0208.0
/12
)(144000)(1000 )1(
12
2
12
µ
)(
0208.0
/12
144
)(
)1(
)1(
12
Annulus
n
v
ddK
n
n
n
a 




 +−
= −
−
µ
Drilling Engineering
Prepared by: Tan Nguyen
Reynolds number for power law fluids in pipe:
Reynolds number for power law fluids In annulus:
Friction factor for power law fluids under turbulent flow conditions
Power Law Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
nn
n
d
K
v
N 





+
=
−
/13
0416.089100
)2(
Re
ρ
nn
n
dd
K
v
N 





+
−
=
−
/12
)(0208.0109000 12
)2(
Re
ρ
2.1
2/1
Re75.0
395.0
)log(
0.4
/1
n
fN
n
f n
−= −
Drilling Engineering
Prepared by: Tan Nguyen
Power Law Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Summary
Drilling Engineering
Prepared by: Tan Nguyen
Summary
Newtonian Model Bingham Plastic Model Power Law Model
Drilling Engineering
Prepared by: Tan Nguyen
Summary
Newtonian Model Bingham Plastic Model Power Law Model
Drilling Engineering
Prepared by: Tan Nguyen
Summary
Newtonian Model Bingham Plastic Model Power Law Model
Drilling Engineering
Prepared by: Tan Nguyen
Example – Newtonian Fluid in Annulus
Example 1: A 9.0 lbm/gal brine having a viscosity of 1.0 cp is being circulated in a well at a rate
of 200 gal/min. Apply the all the criteria for computing equivalent diameter. Determine the flow
pattern and frictional pressure gradient. The drillpipe has an external diameter of 5.0 in. and the
hole has a diameter of 10 in.
Solution:
Drilling Engineering
Prepared by: Tan Nguyen
Example – Newtonian Fluid in Annulus
Drilling Engineering
Prepared by: Tan Nguyen
Example – Newtonian Fluid in Annulus
Drilling Engineering
Prepared by: Tan Nguyen
Example – Newtonian Fluid in Annulus
Note that the Crittendon correlation is applied for the fourth method. In this
method, we need to calculate the equivalent diameter based on Crittendon
correlation and the fictitious average velocity.
Hydraulic Method
Momentum Mothod
Narrow Slot Method
Crittendon Method
Drilling Engineering
Prepared by: Tan Nguyen
Example – BHF - Annulus
Example 2: A 10 lbm/gal mud having a plastic viscosity of 40 cp and a yield point of 15 lbf/100ft2
is circulated at a rate of 600 gal/min. Estimate the frictional pressure loss in the annulus opposite
the drill collars if the drill collars are in a 6.5-in hole, have a length of 1,000 ft, and a 4.5 in. OD.
Check for turbulence using both the apparent viscosity concept and the Hedstrom number
approach. Use an narrow slot equivalent diameter to represent the annular geometry.
Drilling Engineering
Prepared by: Tan Nguyen
Example – BHF - Annulus
Equivalent diameter using narrow slot approximation
Reynolds number based on apparent viscosity
Drilling Engineering
Prepared by: Tan Nguyen
Example – BHF - Annulus
Reynolds number for a plastic viscosity of 40 cp
Using the graph for Hedstrom number, the critical Reynolds number is 3,300. The flow is turbulent
Drilling Engineering
Prepared by: Tan Nguyen
Example – BHF - Annulus
Using Blasius approximation with Re = 3,154, the friction factor is f = 0.0098
Frictional pressure loss is given:
Drilling Engineering
Prepared by: Tan Nguyen
Example – BHF - Annulus
Drilling Engineering
Prepared by: Tan Nguyen
Example – PL - Annulus
Example 3: A 15.6 lbm/gal cement slurry having a consistency index of 335 eq cp and a flow
behavior index of 0.67 is being pumped at a rate of 672 gal/min between a 9.625-in. hole and a
7.0-in.casing. Determine the frictional pressure loss per 100 ft of slurry. Use the equivalent
diameter based on the narrow slot approximation.
Solution:
The mean velocity:
Reynolds number:
Drilling Engineering
Prepared by: Tan Nguyen
Power Law Model
Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
Drilling Engineering
Prepared by: Tan Nguyen
Example– PL - Annulus

More Related Content

PDF
Turbulent flows and equations
PPTX
Compressible Fluid
PPTX
Turbulent flow
PPTX
Navier-Stokes Equation of Motion
PDF
120218 chapter 8 momentum analysis of flow
PPTX
PRESSURE & HEAD (PART-1)
PDF
Fluid mechanics question bank
PPTX
Francis turbine
Turbulent flows and equations
Compressible Fluid
Turbulent flow
Navier-Stokes Equation of Motion
120218 chapter 8 momentum analysis of flow
PRESSURE & HEAD (PART-1)
Fluid mechanics question bank
Francis turbine

What's hot (20)

PPTX
Stream lines and streak lines
PPTX
Types of fluid flow best ppt
PPTX
Design Of Flow Meters
PPT
Ideal flow
PPTX
orifice meter and its application_ppt
PPTX
Turbulent Flow 130120119126
PPT
Laminar Flow in pipes and Anuli Newtonian Fluids
PDF
Fluid Mechanics Chapter 2. Fluid Statics
PPTX
Losses in Pumps
PDF
Chapter four fluid mechanics
PPTX
navier stokes equation
PPTX
Bernoulli's Principle
PDF
Darcy weisbach formula
PPTX
Fm final ppt
PDF
Fluid MechanicsLosses in pipes dynamics of viscous flows
PDF
Bernoulli's Theorem, Limitations & its Practical Application
PDF
Buoyancy and floatation
PPTX
fluid mechanics- pressure measurement
PPTX
Fluid Mechanics - Fluid Pressure and its measurement
PDF
Fluid tutorial 3
Stream lines and streak lines
Types of fluid flow best ppt
Design Of Flow Meters
Ideal flow
orifice meter and its application_ppt
Turbulent Flow 130120119126
Laminar Flow in pipes and Anuli Newtonian Fluids
Fluid Mechanics Chapter 2. Fluid Statics
Losses in Pumps
Chapter four fluid mechanics
navier stokes equation
Bernoulli's Principle
Darcy weisbach formula
Fm final ppt
Fluid MechanicsLosses in pipes dynamics of viscous flows
Bernoulli's Theorem, Limitations & its Practical Application
Buoyancy and floatation
fluid mechanics- pressure measurement
Fluid Mechanics - Fluid Pressure and its measurement
Fluid tutorial 3
Ad

Viewers also liked (20)

PDF
TDF Sturgeon Passage Ladder
PPTX
Spillway and Fish Ladder
PPTX
Young’s modulus 2
PPT
Effect of-flexural-rigidity-in-textile-97
PPTX
What is laminar flow updated for slideshare
PDF
Laminar turbulent
PPTX
5 refraction, snells law (8.2)
PPTX
Modulus of rigidity
PDF
Tarbulent flow
PDF
11th Physics Notes - Magnetism
PPT
Physics 504 Chapter 12 & 13 Different Types of Forces
DOCX
Torsion of circular shafts
PPTX
Viscometers
PPTX
Study of fluids
PPT
Thermal Expansion.
PPT
Laminar Flow
PPTX
Flow through pipes
PPT
Flow in pipes
PDF
Thermal properties of matter
TDF Sturgeon Passage Ladder
Spillway and Fish Ladder
Young’s modulus 2
Effect of-flexural-rigidity-in-textile-97
What is laminar flow updated for slideshare
Laminar turbulent
5 refraction, snells law (8.2)
Modulus of rigidity
Tarbulent flow
11th Physics Notes - Magnetism
Physics 504 Chapter 12 & 13 Different Types of Forces
Torsion of circular shafts
Viscometers
Study of fluids
Thermal Expansion.
Laminar Flow
Flow through pipes
Flow in pipes
Thermal properties of matter
Ad

Similar to 4 turbulent flow (20)

PPT
silo.tips_pete-203-drilling-engineering.ppt
PDF
Computational Analysis of Turbulent flow heat transfer and pressure loss in D...
PPT
viscous laminar fluid flow through pipes
PDF
009a (PPT) Viscous Flow-1 New.pdf .
PPTX
Module 4 - flow through a pipe - Fluid Dynamics
DOC
sheet of pipe flow
PPTX
Mini Project Final (1) (1) (1).pptx
PPT
Flowinpipe.ppt
PPTX
Flow of incompressible fluids through pipes
PPT
Closed conduct flow
PPT
Closed conduct flow
PPTX
Calculation of Flowrate and Pressure Drop Relationship for Laminar Flow using...
PDF
Enhancement of Heat Transfer Rate using Helix Tube and Friction Factor
PPTX
Single phase flow line sizing
PDF
PDF
Comparison of flow analysis of a sudden and gradual change
PDF
Comparison of flow analysis of a sudden and gradual change of pipe diameter u...
PPTX
7-gassteam-medium.pptx
PDF
Volume flow rate_measurement
PDF
Lecture 6
silo.tips_pete-203-drilling-engineering.ppt
Computational Analysis of Turbulent flow heat transfer and pressure loss in D...
viscous laminar fluid flow through pipes
009a (PPT) Viscous Flow-1 New.pdf .
Module 4 - flow through a pipe - Fluid Dynamics
sheet of pipe flow
Mini Project Final (1) (1) (1).pptx
Flowinpipe.ppt
Flow of incompressible fluids through pipes
Closed conduct flow
Closed conduct flow
Calculation of Flowrate and Pressure Drop Relationship for Laminar Flow using...
Enhancement of Heat Transfer Rate using Helix Tube and Friction Factor
Single phase flow line sizing
Comparison of flow analysis of a sudden and gradual change
Comparison of flow analysis of a sudden and gradual change of pipe diameter u...
7-gassteam-medium.pptx
Volume flow rate_measurement
Lecture 6

Recently uploaded (20)

PDF
ENT215_Completing-a-large-scale-migration-and-modernization-with-AWS.pdf
PDF
Microsoft Solutions Partner Drive Digital Transformation with D365.pdf
PDF
Hybrid horned lizard optimization algorithm-aquila optimizer for DC motor
PDF
Five Habits of High-Impact Board Members
PDF
DASA ADMISSION 2024_FirstRound_FirstRank_LastRank.pdf
PPTX
Tartificialntelligence_presentation.pptx
PDF
STKI Israel Market Study 2025 version august
PPT
What is a Computer? Input Devices /output devices
PDF
Hybrid model detection and classification of lung cancer
PDF
A review of recent deep learning applications in wood surface defect identifi...
PDF
TrustArc Webinar - Click, Consent, Trust: Winning the Privacy Game
PPTX
MicrosoftCybserSecurityReferenceArchitecture-April-2025.pptx
PPTX
Modernising the Digital Integration Hub
PPTX
The various Industrial Revolutions .pptx
PDF
Transform Your ITIL® 4 & ITSM Strategy with AI in 2025.pdf
PPTX
O2C Customer Invoices to Receipt V15A.pptx
PDF
Univ-Connecticut-ChatGPT-Presentaion.pdf
PDF
Taming the Chaos: How to Turn Unstructured Data into Decisions
PDF
Architecture types and enterprise applications.pdf
PDF
From MVP to Full-Scale Product A Startup’s Software Journey.pdf
ENT215_Completing-a-large-scale-migration-and-modernization-with-AWS.pdf
Microsoft Solutions Partner Drive Digital Transformation with D365.pdf
Hybrid horned lizard optimization algorithm-aquila optimizer for DC motor
Five Habits of High-Impact Board Members
DASA ADMISSION 2024_FirstRound_FirstRank_LastRank.pdf
Tartificialntelligence_presentation.pptx
STKI Israel Market Study 2025 version august
What is a Computer? Input Devices /output devices
Hybrid model detection and classification of lung cancer
A review of recent deep learning applications in wood surface defect identifi...
TrustArc Webinar - Click, Consent, Trust: Winning the Privacy Game
MicrosoftCybserSecurityReferenceArchitecture-April-2025.pptx
Modernising the Digital Integration Hub
The various Industrial Revolutions .pptx
Transform Your ITIL® 4 & ITSM Strategy with AI in 2025.pdf
O2C Customer Invoices to Receipt V15A.pptx
Univ-Connecticut-ChatGPT-Presentaion.pdf
Taming the Chaos: How to Turn Unstructured Data into Decisions
Architecture types and enterprise applications.pdf
From MVP to Full-Scale Product A Startup’s Software Journey.pdf

4 turbulent flow

  • 1. Drilling Engineering Prepared by: Tan Nguyen Drilling Engineering – PE 311 Turbulent Flow in Pipes and Annuli
  • 2. Drilling Engineering Prepared by: Tan Nguyen When attempting to quantify the pressure losses in side the drillstring and in the annulus it is worth considering the following matrix: Frictional Pressure Drop in Pipes and Annuli
  • 3. Drilling Engineering Prepared by: Tan Nguyen Laminar Flow: In this type of flow, layers of fluid move in streamlines. There is no microscopic or macroscopic intermixing of the layers. Laminar flow systems are generally represented graphically by streamlines. Turbulent Flow: In turbulent flow, there is an irregular random movement of fluid in transverse direction to the main flow. This irregular, fluctuating motion can be regarded as superimposed on the mean motion of the fluid. Turbulent Flow in Pipes – Newtonian Fluids Introduction
  • 4. Drilling Engineering Prepared by: Tan Nguyen Reynolds number, Re, is a dimensionless number that gives a measure of the ratio of inertial forces to viscous forces. Reynolds number is used to characterize different flow regimes, such as laminar or turbulent flow. Laminar occurs at low Reynolds number, where viscous forces are dominant, and is characterized by smooth, constant fluid motion; turbulent flow occurs at high Reynolds number and is dominated by inertial forces, which tend to produce chaotic eddies, vortices and other flow instabilities. For pipe In field unit: Definition of Reynolds Number µ ρ du _ Re = μ duρ _ 928 Re = Turbulent Flow in Pipes – Newtonian Fluids
  • 5. Drilling Engineering Prepared by: Tan Nguyen If Re < 2,100 Laminar flow Re = 2,100 – 4,000 Transition flow Re > 4,000 Turbulent Note that this critical Reynolds number is correct only for Newtonian fluids Determination of Laminar/Turbulent Flow cp.fluid,ofviscosity inI.D.,pipe ft/svelocity,fluidavg. lbm/galdensity,fluidwhere 928 Re = = = = μ d u ρ μ duρ _ Turbulent Flow in Pipes – Newtonian Fluids
  • 6. Drilling Engineering Prepared by: Tan Nguyen Relationship between shear stress and friction factor: Pipe flow under laminar conditions: Therefore, Newtonian fluids flow in pipe under laminar flow conditions: Hence, This equation will be used to calculate the friction factor of Newtonian fluids flow in pipe under laminar flow conditions. Determination of Friction Factor - Laminar Flow Turbulent Flow in Pipes – Newtonian Fluids
  • 7. Drilling Engineering Prepared by: Tan Nguyen For turbulent flow, the friction factor can be calculated by using Colebrook correlation. Where ε is the absolute roughness. ε/d is the relative roughness. For smooth pipe, the relative roughness ε/d < 0.0004, the following equations can be used to calculate the friction factor in turbulent flow Re = 2,100 – 100,000: Blasius approximation: Re = 2,100 – 100,000:         +−= fN d f Re 255.1 /269.0log4 1 ε Determination of Friction Factor - Turbulent Flow ( ) 395.0log4 1 Re −−= fN f 25.0 Re 0791.0 N f = Turbulent Flow in Pipes – Newtonian Fluids
  • 8. Drilling Engineering Prepared by: Tan Nguyen Determination of Friction Factor Turbulent Flow in Pipes – Newtonian Fluids
  • 9. Drilling Engineering Prepared by: Tan Nguyen Determination of Friction Factor Turbulent Flow in Pipes – Newtonian Fluids
  • 10. Drilling Engineering Prepared by: Tan Nguyen From equation: , an equation of dp/dL can be expressed as In field unit: . This equation can be used to calculate the frictional pressure drop gradient for Newtonian and non-Newtonian fluids. Combining this equation and the Blasius approximation gives Note that the Moody friction factor is four times higher than the Fanning friction factor. Determination of the Frictional Pressure Loss 25.0 2 928 8.25 0791.0         = µ ρ ρ dv d u dL dp 75.4 25.075.175.0 25.0 25.075.175.0 86241800 d q d u dL dp µρµρ == Turbulent Flow in Pipes – Newtonian Fluids
  • 11. Drilling Engineering Prepared by: Tan Nguyen Example: Determine the frictional pressure drop in 10000ft of 4.5-in commercial steel drillpipe having an internal diameter of 3.826in. If a 20 cp Newtonian fluid having a density of 9 lbm/gal is pumped through the drillpipe at a rate of 400 gal/min Solution: Mean velocity: Reynolds number: Since Re > 2,100, the flow is under turbulent flow conditions. Example sft d q u /16.11 826.3*488.2 400 488.2 22 === 17831 20 826.3*16.11*9*928928 Re === μ duρ _ Turbulent Flow in Pipes – Newtonian Fluids
  • 12. Drilling Engineering Prepared by: Tan Nguyen From table 4.5, the absolute roughness for commercial steel pipe is ε = 0.000013 inches. The relative roughness ε/d = 0.000013/3.826 = 0.0000034 < 0.0004 --> smooth pipe Solve this equation for the Fanning friction factor: f = 0.00666 Thus the frictional pressure loss can be obtained by Example         +−= fN d f re 255.1 /269.0log4 1 ε psiD d vf D dL dp pf 75610000* 826.3*8.25 16.11*9*00666.0 8.25 22 ====∆ ρ Turbulent Flow in Pipes – Newtonian Fluids
  • 13. Drilling Engineering Prepared by: Tan Nguyen Using Blasius approximation ,the equation becomes Pressure drop: DP = dp/dL x D = (0.0777)(10,000) = 777 psi Example 25.0 Re 0791.0 N f = 25.0 2 928 8.25 0791.0         = µ ρ ρ dv d v dL dp ftpsi d v dL dp /0777.0 1800 25.0 25.075.175.0 == µρ Turbulent Flow in Pipes – Newtonian Fluids
  • 14. Drilling Engineering Prepared by: Tan Nguyen Using Blasius approximation ,the equation becomes Pressure drop: DP = dp/dL x D = (0.0777)(10,000) = 777 psi Example 25.0 Re 0791.0 N f = 25.0 2 928 8.25 0791.0         = µ ρ ρ dv d v dL dp ftpsi d v dL dp /0777.0 1800 25.0 25.075.175.0 == µρ Turbulent Flow in Pipes – Newtonian Fluids
  • 15. Drilling Engineering Prepared by: Tan Nguyen Hydraulic diameter is defined as: Equivalent diameter by using hydraulic diameter method: Equivalent Diameter for Annular Geometry – Hydraulic Diameter Method Turbulent Flow in Pipes/Annuli – NonNewtonian Fluids
  • 16. Drilling Engineering Prepared by: Tan Nguyen From the momentum equation, frictional pressure drop for Newtonian fluid in the annulus is For pipe flow, d1 --> 0 then Comparing these two equations, the equivalent diameter an annulus can be obtained Equivalent Diameter for Annular Geometry – From Momentum Equation Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids           − −+ = 1 2 2 1 2 22 1 2 2 ln 500,1 d d dd dd u dL dpf µ 2 500,1 d u dL dpf µ = ( )1 2 ln 2 1 2 22 1 2 2 d de dd ddd − −+=
  • 17. Drilling Engineering Prepared by: Tan Nguyen From the narrow slot approximation, frictional pressure drop for Newtonian fluid in the annulus is For pipe flow Comparing these two equations, the equivalent diameter an annulus can be obtained Equivalent Diameter for Annular Geometry – Narrow Slot Approximation Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids 2 500,1 d u dL dpf µ = ( )12816.0 ddde −=
  • 18. Drilling Engineering Prepared by: Tan Nguyen A fourth expression for the equivalent diameter of an annulus was developed by Crittendon. When using Crittendon correlation, a fictitious average velocity also must be used in describing the flow system. Equivalent Diameter for Annular Geometry – Crittendon Correlation Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
  • 19. Drilling Engineering Prepared by: Tan Nguyen 1. Obtain apparent viscosity by combining the frictional pressure loss in pipe (or annulus) for both Newtonian and Bingham Plastic models 2. Use apparent viscosity to determine Reynolds Number Bingham Plastic Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids dd v d v ypa 22515001500 22 τµµ += )( 66.6 Pipe v dy pa τ µµ += )( )(5 12 Annulus v ddy pa − += τ µµ or
  • 20. Drilling Engineering Prepared by: Tan Nguyen Another way to determine the flow regime (critical Reynolds number) is to use the Hedstrom number In field unit Bingham Plastic Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids 2 2 p y HE d N µ ρτ = 2 2 37100 p y HE d N µ ρτ =
  • 21. Drilling Engineering Prepared by: Tan Nguyen Bingham Plastic Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids Turbulent
  • 22. Drilling Engineering Prepared by: Tan Nguyen Apparent Viscosity for use in the Reynolds Number is obtained by comparing the laminar flow equations for Newtonian and Power Law fluids Pipe flow: Annular flow: Power Law Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids n n n a n d vK d v       + = + 0416.0 /13 1440001500 )1(2 µ )( 0416.0 /13 96 )1( )1( Pipe n v Kd n n n a       + = − − µ n n n a n dd vK dd v       + − = − + 0208.0 /12 )(144000)(1000 )1( 12 2 12 µ )( 0208.0 /12 144 )( )1( )1( 12 Annulus n v ddK n n n a       +− = − − µ
  • 23. Drilling Engineering Prepared by: Tan Nguyen Reynolds number for power law fluids in pipe: Reynolds number for power law fluids In annulus: Friction factor for power law fluids under turbulent flow conditions Power Law Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids nn n d K v N       + = − /13 0416.089100 )2( Re ρ nn n dd K v N       + − = − /12 )(0208.0109000 12 )2( Re ρ 2.1 2/1 Re75.0 395.0 )log( 0.4 /1 n fN n f n −= −
  • 24. Drilling Engineering Prepared by: Tan Nguyen Power Law Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
  • 25. Drilling Engineering Prepared by: Tan Nguyen Summary
  • 26. Drilling Engineering Prepared by: Tan Nguyen Summary Newtonian Model Bingham Plastic Model Power Law Model
  • 27. Drilling Engineering Prepared by: Tan Nguyen Summary Newtonian Model Bingham Plastic Model Power Law Model
  • 28. Drilling Engineering Prepared by: Tan Nguyen Summary Newtonian Model Bingham Plastic Model Power Law Model
  • 29. Drilling Engineering Prepared by: Tan Nguyen Example – Newtonian Fluid in Annulus Example 1: A 9.0 lbm/gal brine having a viscosity of 1.0 cp is being circulated in a well at a rate of 200 gal/min. Apply the all the criteria for computing equivalent diameter. Determine the flow pattern and frictional pressure gradient. The drillpipe has an external diameter of 5.0 in. and the hole has a diameter of 10 in. Solution:
  • 30. Drilling Engineering Prepared by: Tan Nguyen Example – Newtonian Fluid in Annulus
  • 31. Drilling Engineering Prepared by: Tan Nguyen Example – Newtonian Fluid in Annulus
  • 32. Drilling Engineering Prepared by: Tan Nguyen Example – Newtonian Fluid in Annulus Note that the Crittendon correlation is applied for the fourth method. In this method, we need to calculate the equivalent diameter based on Crittendon correlation and the fictitious average velocity. Hydraulic Method Momentum Mothod Narrow Slot Method Crittendon Method
  • 33. Drilling Engineering Prepared by: Tan Nguyen Example – BHF - Annulus Example 2: A 10 lbm/gal mud having a plastic viscosity of 40 cp and a yield point of 15 lbf/100ft2 is circulated at a rate of 600 gal/min. Estimate the frictional pressure loss in the annulus opposite the drill collars if the drill collars are in a 6.5-in hole, have a length of 1,000 ft, and a 4.5 in. OD. Check for turbulence using both the apparent viscosity concept and the Hedstrom number approach. Use an narrow slot equivalent diameter to represent the annular geometry.
  • 34. Drilling Engineering Prepared by: Tan Nguyen Example – BHF - Annulus Equivalent diameter using narrow slot approximation Reynolds number based on apparent viscosity
  • 35. Drilling Engineering Prepared by: Tan Nguyen Example – BHF - Annulus Reynolds number for a plastic viscosity of 40 cp Using the graph for Hedstrom number, the critical Reynolds number is 3,300. The flow is turbulent
  • 36. Drilling Engineering Prepared by: Tan Nguyen Example – BHF - Annulus Using Blasius approximation with Re = 3,154, the friction factor is f = 0.0098 Frictional pressure loss is given:
  • 37. Drilling Engineering Prepared by: Tan Nguyen Example – BHF - Annulus
  • 38. Drilling Engineering Prepared by: Tan Nguyen Example – PL - Annulus Example 3: A 15.6 lbm/gal cement slurry having a consistency index of 335 eq cp and a flow behavior index of 0.67 is being pumped at a rate of 672 gal/min between a 9.625-in. hole and a 7.0-in.casing. Determine the frictional pressure loss per 100 ft of slurry. Use the equivalent diameter based on the narrow slot approximation. Solution: The mean velocity: Reynolds number:
  • 39. Drilling Engineering Prepared by: Tan Nguyen Power Law Model Turbulent Flow in Pipes/Annuli – nonNewtonian Fluids
  • 40. Drilling Engineering Prepared by: Tan Nguyen Example– PL - Annulus