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Drilling Fluids – Frictional Pressure Loss

Formulas

Flow rate, flow regime, rheological properties, and conduit geometry are among the key parameters that impact frictional pressure losses in the drill string and annulus. The process to model these pressures, complex in its own right for Herschel-Bulkley fluids, is further complicated in HTHP and deepwater wells by the sensitivity of drilling fluid density and rheological properties to downhole temperatures and pressures

Yield Stress:

Ty= 2 \times R3 – R6

Ty= 2 \times R3 - R6

R3 – R3 Viscometer Reading (RPM)
R6 – R6 Viscometer Reading (RPM)

Plastic Viscosity:

PV = R600 – R300

PV = R600 - R300

R600 – R300 Viscometer Reading (RPM)
R300 – R600 Viscometer Reading (RPM)

Yield Point of Drilling Fluid:

YP = R300 – PV

YP = R300 - PV
Flow Behavior Index (Herschel-Bulkley Fluids)

N = 3.32 \cdot \log{10}\left({(2 \cdot PV + YP – Ty)}/{(PV + YP – Ty)}\right)

N = 3.32 \cdot \log{10}\left({(2 \cdot PV + YP - Ty)}/{(PV + YP - Ty)}\right)

Consistency Factor (Herschel-Bulkley Fluids)

K = {(PV + YP – Ty)}/{(511^N)}

K = {(PV + YP - Ty)}/{(511^N)}
Flow Behavior Index (Power Low Fluids)

n_p = 3.32 \cdot \log{10}\left({(2 \cdot PV + YP)}/{(PV + YP)}\right)

n_p = 3.32 \cdot \log{10}\left({(2 \cdot PV + YP)}/{(PV + YP)}\right)

Consistency Factor (Power Low Fluids)

kp = {(PV + YP)}/{(511^{np})}

kp = {(PV + YP)}/{(511^{np})}
Frictional Pressure Loss in Drill Pipe:

Drilling Fluid Velocity Inside Pipe

V_p = \frac{24.51 \cdot Q}{D_i^2}

V_p = \frac{24.51 \cdot Q}{D_i^2}

Q = Flow Rate (gal/min)

Di = Internal Diameter of Drill Pipe (inch)

Shear Rate Correction

B_a = \frac{3(N + 1)}{4N}\~\ G = B_a \~\ \gamma_w = \frac{1.6GV_p}{D_i} \~\\tau_f = \left(\frac{4}{3}\right)^N \tau_y + K(\gamma_w)^N \~\\tau_w = 1.066\tau_f

B_a = \frac{3(N + 1)}{4N}\\~\\ G = B_a \\~\\ \gamma_w = \frac{1.6GV_p}{D_i} \\~\\\tau_f = \left(\frac{4}{3}\right)^N \tau_y + K(\gamma_w)^N \\~\\\tau_w = 1.066\tau_f
Reynolds Number

N_{Re}{pipe} = \frac{\rho V_p^2}{19.36 \tau_w}

N_{Re}{pipe} = \frac{\rho V_p^2}{19.36 \tau_w}

ρ = Drilling Fluid Density (gal/min)

Critical Reynolds Number

N_{CRe}{{pipe}} = 3470 – 1370N

N_{CRe}{{pipe}} = 3470 - 1370N
Fanning Friction Factor

f_{\text{lam}} = \frac{16}{N_{Re}{\text{annulus}}}\~\ f_{\text{trans}} = \frac{16 \cdot N_{Re}{\text{annulus}}}{N_{CRe}{\text{annulus}}^2}\~\ a = \frac{\log n_p + 3.93}{50} \~\ b = \frac{1.75 – \log n_p}{7} \~\ f_{\text{tur}} = \frac{a}{N_{Re}{\text{annulus}}^b}\~\ f_{\text{int}} = \left(f_{\text{trans}}^{-8} + f_{\text{turb}}^{-8}\right)^{-1/8} \~\f = \left(f_{\text{int}}^{12} + f_{\text{lam}}^{12}\right)^{1/2}

f_{\text{lam}} = \frac{16}{N_{Re}{\text{annulus}}}\\~\\ f_{\text{trans}} = \frac{16 \cdot N_{Re}{\text{annulus}}}{N_{CRe}{\text{annulus}}^2}\\~\\ a = \frac{\log n_p + 3.93}{50} \\~\\ b = \frac{1.75 - \log n_p}{7} \\~\\ f_{\text{tur}} = \frac{a}{N_{Re}{\text{annulus}}^b}\\~\\ f_{\text{int}} = \left(f_{\text{trans}}^{-8} + f_{\text{turb}}^{-8}\right)^{-1/8} \\~\\f = \left(f_{\text{int}}^{12} + f_{\text{lam}}^{12}\right)^{1/2}
Pressure Loss in Drill Pipe

P_{DS} = \frac{1.076\rho V_p^2 f L}{10^5(D_i)}

P_{DS} = \frac{1.076\rho V_p^2 f L}{10^5(D_i)}

L = Length of the Pipe or Annulus (ft)

Frictional Pressure Loss in Annulus:

Drilling Fluid Velocity Inside Annulus

V_{a} = \frac{24.51 \cdot Q}{D_h^2-D_p^2}

V_{a} = \frac{24.51 \cdot Q}{D_h^2-D_p^2}

Dh = Borehole Diameter (inch)
Dp = Outside Diameter of Drill Pipe (inch)

Shear Rate Correction

B_a = \frac{2(N + 1) }{3N} \cdot \frac{3}{2}\~\G = B_a \~\ \gamma_w = \frac{1.6GV_a}{D_h – D_p}\~\\tau_f = \left(\frac{3}{2}\right)^N \tau_y + K(\gamma_w)^N \~\\tau_w = 1.066\tau_f

B_a = \frac{2(N + 1) }{3N} \cdot \frac{3}{2}\\~\\G = B_a \\~\\ \gamma_w = \frac{1.6GV_a}{D_h - D_p}\\~\\\tau_f = \left(\frac{3}{2}\right)^N \tau_y + K(\gamma_w)^N \\~\\\tau_w = 1.066\tau_f
Reynolds Number

{N_{Re}{\text{annulus}}}= \frac{\rho V_a^2}{19.36\tau_w}

{N_{Re}{\text{annulus}}}= \frac{\rho V_a^2}{19.36\tau_w}
Critical Reynolds Number

N_{CRe}{{pipe}} = 3470 – 1370N

N_{CRe}{{pipe}} = 3470 - 1370N
Fanning Friction Factor

f_{\text{lam}} = \frac{16}{N_{Re}{\text{annulus}}}\~\ f_{\text{trans}} = \frac{16 \cdot N_{Re}{\text{annulus}}}{N_{CRe}{\text{annulus}}^2}\~\ a = \frac{\log n_p + 3.93}{50} \~\ b = \frac{1.75 – \log n_p}{7} \~\ f_{\text{tur}} = \frac{a}{N_{Re}{\text{annulus}}^b}\~\ f_{\text{int}} = \left(f_{\text{trans}}^{-8} + f_{\text{turb}}^{-8}\right)^{-1/8} \~\f = \left(f_{\text{int}}^{12} + f_{\text{lam}}^{12}\right)^{1/2}

f_{\text{lam}} = \frac{16}{N_{Re}{\text{annulus}}}\\~\\ f_{\text{trans}} = \frac{16 \cdot N_{Re}{\text{annulus}}}{N_{CRe}{\text{annulus}}^2}\\~\\ a = \frac{\log n_p + 3.93}{50} \\~\\ b = \frac{1.75 - \log n_p}{7} \\~\\ f_{\text{tur}} = \frac{a}{N_{Re}{\text{annulus}}^b}\\~\\ f_{\text{int}} = \left(f_{\text{trans}}^{-8} + f_{\text{turb}}^{-8}\right)^{-1/8} \\~\\f = \left(f_{\text{int}}^{12} + f_{\text{lam}}^{12}\right)^{1/2}
Pressure Loss in Drill Pipe

P_{a} = \frac{1.076\rho V_a^2 f L}{10^5(D_h-D_p)}

P_{a} = \frac{1.076\rho V_a^2 f L}{10^5(D_h-D_p)}

L = Length of the Pipe or Annulus (ft)

Bit Pressure Loss:

T_{fa} = 0.00076699 \cdot ((Ndn1 \cdot dn1^2) + (Ndn2 \cdot dn2^2) + (Ndn3 \cdot dn3^2))\~\\Delta P_{\text{Nozzle}} = \frac{\rho \cdot Q^2}{12042 \cdot (Cv)^2 \cdot T_{fa}^2}

T_{fa} = 0.00076699 \cdot ((Ndn1 \cdot dn1^2) + (Ndn2 \cdot dn2^2) + (Ndn3 \cdot dn3^2))\\~\\\Delta P_{\text{Nozzle}} = \frac{\rho \cdot Q^2}{12042 \cdot (Cv)^2 \cdot T_{fa}^2}

Ndn1 = Number of Nozzle 1
Ndn2 = Number of Nozzle 2
Ndn3 = Number of Nozzle 3
dn1 = Nozzle 1 Size (1/32 inch)
dn2 = Nozzle 2 Size (1/32 inch)
dn3 = Nozzle 3 Size (1/32 inch)
Cv = Nozzle Discharge Coefficient

Total Frictional Pressure Losses:

P_{\text{tot}} = P_{DS} + P_a + \Delta P_{\text{NOZZLE}}

P_{\text{tot}} = P_{DS} + P_a + \Delta P_{\text{NOZZLE}}

Input Parameters

  • R3 Viscometer Reading [RPM]
  • R6 Viscometer Reading [RPM]
  • R300 Viscometer Reading [RPM]
  • R600 Viscometer Reading [RPM]
  • Flow Rate [gal/min]
  • Drilling Fluid Density [lb/gal]
  • Internal Diameter of Drill Pipe [inch]
  • Outside Diameter of Drill Pipe [inch]
  • Bore Hole Diameter [inch]
  • Length of Pipe Annulus [ft]

Bit Nozzle Input Parameters:

  • Nozzle 1 Size [1/32 inch]
  • Nozzle 2 Size [1/32 inch]
  • Nozzle 3 Size [1/32 inch]
  • Number of Nozzle 1
  • Number of Nozzle 2
  • Number of Nozzle 3
  • Nozzle Discharge Coefficient

Outputs/Reports

  • Yield Stress [lb/100ft2]
  • Plastic Viscosity [cP]
  • Yield Point of Drilling Fluid [lb/100ft2]
  • Flow Behavior Index (Herschel-Bulkley Fluids)
  • Consistency Factor (Herschel-Bulkley Fluids)
  • Flow Behavior Index (Power Low Fluids)
  • Consistency Factor (Power Low Fluids)
Frictional Pressure Loss in Drill Pipe:
  • Drilling Fluid Velocity Inside Pipe [ft/min]
  • Reynolds Number
  • Fanning Friction Factor
  • Pipe Pressure Loss [psi]
Frictional Pressure Loss in Annulus:
  • Drilling Fluid Velocity Inside Annulus [ft/min]
  • Reynolds Number
  • Fanning Friction Factor
  • Pressure Loss in Annulus [psi]
  • Bit Pressure Loss [psi]
  • Total Frictional Pressure Losses [psi]

References

  • Willoughby, David (2005). Horizontal Directional Drilling, McGraw-Hill, New York, ISBN 0-87814-395-5. v.
  • Willoughby, David, Training – Horizontal Directional Drilling, TTI, November 2016
  • HDD Consortium. (2001). Horizontal directional drilling, good practices guidelines, HDD Consortium.
  • Horizontal Directional Drilling Training Manual, Horizontal Drilling International, February 1999
  • Skonberg, Eric R. II. Muindi, Tennyson M. (2014). Pipeline Design for Installation by Horizontal Directional Drilling, American Society of Civil Engineers. Horizontal Directional Drilling Design Guideline Task Committee.
  • “Installation of Pipelines by Horizontal Directional Drilling”, PRCI Report PR-227-9424
  • Nayyar, Mohinder L. (1992). Piping Handbook, 6th Edition, McGraw-Hill, New York, NY.
  • AWWA (2006), PE Pipe Design and Installation, M55, American Water Works Association, Denver, CO
  • ASTM (1962), PPI Handbook

Appendix of Definitions

AUGER BORING – Casing is jacked into the ground as a rotating auger works simultaneously to remove the excavated soil. It is commonly used in applications where settlement is a concern: under highways, railways and levies. Also known as a dry bore.

BENTONITE – A natural clay material used as a basic ingredient for drilling muds and lubricants to facilitate ease of installation.

BORE OR BOREHOLE – drilling term – The elongated cavity created by the drilling process. Often the borehole is not a void, but rather a hole filled with drilling mud and cuttings. Well casing is pulled or pushed into the borehole to complete a well.

CASING – drilling term – The non-perforated or non-slotted pipe that comprises the entry and exit sections of a horizontal well, as opposed to the well screen. Surface casing is a pipe that is set through loose surficial deposits to stabilize the bore, so the deeper sections can be drilled without difficulty from caving or collapse in the upper section of the borehole.

CROSSING – A pipeline installation designed to pass beneath a surface obstruction. Examples of crossings include roads, railway tracks, water bodies, pipeline corridors, and utilities.

DRILLING MUD – drilling material – aqueous slurry that is used during drilling to transport drill cuttings from the borehole, prevent borehole collapse and provide lubrication for the drill string. Most horizontal drilling uses drilling mud of some sort, although in some conditions it is possible or preferable to drill using air or water. Drilling mud made be made using the mineral bentonite, synthetic or natural polymers, or some combination of the two.

DRILL RIG – A trenchless machine that installs pipes and cables by drilling a pilot hole that can be enlarged (if necessary), and then pulling the product line.

ENTRY POINT – The starting location of the crossing where the drill enters the ground.

EXIT POINT – The end location of the crossing.

FORWARD REAMER – drilling tool – A type of reamer used to enlarge the diameter of the borehole in a blind or single-entry well.

HORIZONTAL DIRECTIONAL DRILLING (HDD) – A surface-based trenchless technology that involves a horizontal bore under the surface along a planned pathway. Once the HDD creates a bore of a suitable size – which may require one or multiple passes by the drilling apparatus – the conduit or pipe is pulled into the bore and connections are made to the appropriate utilities.

OPEN CUT – Underground construction method involving excavation from ground level to the level required for the installation, maintenance, or inspection of a pipe, conduit, or cable. Upon completion of the work, the trench is backfilled, and the surface restored. Backhoe excavation is an example of open-cut construction.

PILOT BORE – drilling term – The initial boring made in a horizontal well installation. The pilot bore is steered, using any of several technologies, from a designated entry point, along a predetermined bore path, to a designated endpoint, either at the ground surface or at depth. The pilot bore subsequently may be reamed to a larger diameter to accommodate the desired size well screen and casing.

PIPE PULLING – Method used to replace small diameter pipes by attaching new product pipe to the existing pipe, which is then pulled out of the ground.

POTHOLE – drilling term – a small hole excavated from the surface to a buried utility in order to provide positive verification of its location.

REAMER – drilling tool – a cutting tool used to enlarge the diameter of a borehole after the pilot bore has been drilled.

FAQ

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  • Combined Stresses and Limitations for Both Liquid & Gas HDD?

    HDD combined stresses can be analyzed by calculating the maximum shear stress on a small element in the pipeline.  Maximum shear stress should be limited to 45% of the SMYS of the pipe (ASME/ANSI B31.4). This is in accordance to PRCI report PR-227-9424 from the findings and conclusions of those companies who performed and approved the research work, However, the question comes up from time to time that the B31.4 code can be converted to B31.8’s code application. Check Out

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Updated on January 9, 2024

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