Flow in Pipes: Fundamentals & Losses

Laminar and turbulent flow, Reynolds number, friction factor, and calculation of head loss in pipes.

Overview

Pipe flow refers to the flow of a liquid in a closed conduit that completely fills the cross-section. The driving force is typically a pressure difference or gravity.

Reynolds Number

The nature of flow (laminar or turbulent) is determined by the dimensionless Reynolds Number (ReRe).

Reynolds Number

A dimensionless quantity used to predict transition from laminar to turbulent flow in pipe systems.

Re=ρVDμ=VDνRe = \frac{\rho V D}{\mu} = \frac{V D}{\nu}

Variables

SymbolDescriptionUnit
ReReReynolds numberdimensionless
Fluid densitykg/m3kg/m^3
VVMean flow velocitym/s
DDInternal pipe diameterm
Dynamic viscosity of fluidPa·s
m2/sm^2/s

Pipe Flow Regimes

Based on the Reynolds Number, pipe flow is classified into three distinct regimes:

  • Laminar Flow (Re<2000Re < 2000): Viscous forces dominate. Fluid moves in smooth, parallel layers. The velocity profile is parabolic.
  • Transitional Flow (2000<Re<40002000 < Re < 4000): Unstable flow, alternating between laminar and turbulent.
  • Turbulent Flow (Re>4000Re > 4000): Inertial forces dominate. Chaotic mixing and eddies. The velocity profile is flatter.

Reynolds Number Simulation

Use the interactive Reynolds Number Simulation below to experiment with fluid velocity, pipe diameter, and viscosity to see the flow regime change in real time.

Reynolds Number Visualizer

Calculated Reynolds Number (ReRe)
50,000
Flow Regime: Turbulent

Particle visualization of flow lines. Note: visual speed is scaled.

Friction Loss

As fluid flows, energy is lost due to friction between fluid layers and against the pipe wall. This energy loss is expressed as head loss (hfh_f).

Darcy-Weisbach Equation Overview

The Darcy-Weisbach equation is the most accurate and universally applicable formula for calculating major head loss due to friction in pipe flow.

Darcy-Weisbach Equation

Calculates the friction head loss in a pipe of circular cross-section.

hf=fLDV22gh_f = f \frac{L}{D} \frac{V^2}{2g}

Variables

SymbolDescriptionUnit
hfh_fHead loss due to frictionm
ffDarcy friction factordimensionless
LLLength of the pipem
DDDiameter of the pipem
VVAverage flow velocitym/s
ggAcceleration due to gravitym/s2m/s^2

Determining the Friction Factor (ff)

The value of the friction factor ff depends on the flow regime and the relative pipe roughness (ϵ/D\epsilon/D).

Procedure

To determine the friction factor ff, follow these steps:

  1. Calculate the Reynolds Number (ReRe) to identify the flow regime.
  2. For laminar flow (Re<2000Re < 2000), calculate ff directly.
  3. For turbulent flow (Re>4000Re > 4000), determine ff using the implicit Colebrook-White equation, the explicit Haaland approximation, or the Moody Chart.

Friction Factor for Laminar Flow

Calculates the friction factor for laminar pipe flow directly from the Reynolds number.

f=64Ref = \frac{64}{Re}

Variables

SymbolDescriptionUnit
ffDarcy friction factordimensionless
ReReReynolds numberdimensionless

Colebrook-White Equation

The fundamental implicit equation to determine the friction factor in turbulent flow.

1f=2log(ϵ/D3.7+2.51Ref)\frac{1}{\sqrt{f}} = -2 \log \left( \frac{\epsilon/D}{3.7} + \frac{2.51}{Re \sqrt{f}} \right)

Variables

SymbolDescriptionUnit
ffDarcy friction factordimensionless
Absolute pipe wall roughnessm
DDInternal pipe diameterm
ReReReynolds numberdimensionless

Haaland Equation

An explicit approximation of the Colebrook-White equation that avoids iterative calculations.

1f1.8log[(ϵ/D3.7)1.11+6.9Re]\frac{1}{\sqrt{f}} \approx -1.8 \log \left[ \left( \frac{\epsilon/D}{3.7} \right)^{1.11} + \frac{6.9}{Re} \right]

Variables

SymbolDescriptionUnit
ffDarcy friction factor approximationdimensionless
Absolute pipe wall roughnessm
DDInternal pipe diameterm
ReReReynolds numberdimensionless

Moody Chart

The Moody Chart is a graphical plot of the friction factor ff versus the Reynolds number ReRe for various relative roughness values (ϵ/D\epsilon/D). Use the interactive Moody Chart simulation below to explore these relationships visually.

Empirical Pipe Flow Formulas

These are commonly used explicit formulas specifically tailored for water distribution systems.

Hazen-Williams Equation Overview

The Hazen-Williams equation is widely used in waterworks design because it is explicit and does not require calculating the friction factor (ff) iteratively. It is valid only for water at ordinary temperatures (5°C to 25°C) and for pipe diameters larger than 50 mm.

Hazen-Williams Equation

Calculates flow velocity for water in pipes under steady state conditions.

V=0.849ChwR0.63S0.54(SI Units)V = 0.849 C_{hw} R^{0.63} S^{0.54} \quad (\text{SI Units})

Variables

SymbolDescriptionUnit
VVMean velocitym/s
ChwC_{hw}Hazen-Williams roughness coefficientdimensionless
RRHydraulic radius (D/4 for full circular pipes)m
SSSlope of the energy grade line (h_f/L)m/m

Manning Equation Overview

While more common in open channels, the Manning equation is also frequently used for full pipe flow, especially in sewer and gravity storm drain design.

Manning Equation for Pipes

Calculates flow velocity under gravity flow or full pipe conditions.

V=1nR2/3S1/2(SI Units)V = \frac{1}{n} R^{2/3} S^{1/2} \quad (\text{SI Units})

Variables

SymbolDescriptionUnit
VVMean velocitym/s
nnManning's roughness coefficients/m1/3s/m^{1/3}
RRHydraulic radius (D/4 for full circular pipes)m
SSSlope of the energy grade line (h_f/L)m/m

Minor Losses Overview

Minor losses represent energy losses that occur due to localized flow disturbances at pipe components such as valves, bends, elbows, expansions, contractions, entrances, and exits.

Minor Head Loss Equation

Calculates the localized energy loss across a pipe component or fitting.

hm=KV22gh_m = K \frac{V^2}{2g}

Variables

SymbolDescriptionUnit
hmh_mMinor head lossm
KKMinor loss coefficientdimensionless
VVMean velocity in the pipem/s
ggAcceleration due to gravitym/s2m/s^2

Common Minor Loss Coefficients

The loss coefficient KK is determined empirically and varies based on the geometry of the fitting:

  • Entrance: K0.5K \approx 0.5 (sharp-edged), K0.04K \approx 0.04 (well-rounded).
  • Exit: K=1.0K = 1.0 (sudden expansion).
  • 90° Elbow: K0.9K \approx 0.9.
  • Globe Valve (Fully Open): K10K \approx 10.
Key Takeaways
  • The Reynolds Number (ReRe) is a dimensionless parameter that dictates the flow regime by comparing inertial forces to viscous forces.
  • The Hazen-Williams Equation is an explicit, empirical formula often preferred in water distribution systems over the iterative Darcy-Weisbach equation.
  • Flow transitions from laminar (smooth, predictable) to turbulent (chaotic, highly mixed) as velocity or pipe diameter increases, or as fluid viscosity decreases.
  • The critical threshold for pipe flow is generally Re2000Re \approx 2000.
  • Major losses are due to friction over the length of the pipe and are best calculated using the Darcy-Weisbach Equation.
  • For laminar flow, the friction factor ff depends solely on the Reynolds number (f=64/Ref = 64/Re).
  • For turbulent flow, ff depends on both ReRe and the relative roughness of the pipe wall (ϵ/D\epsilon/D), often requiring the Colebrook-White equation or the Moody Chart.
  • Minor losses occur at localized points in a pipe system due to changes in geometry (valves, bends, expansions, entrances).
  • They are calculated as a fraction of the velocity head (KV22gK \frac{V^2}{2g}).
  • Despite the name "minor", in short, highly convoluted pipe systems, these losses can exceed the "major" friction losses.