Drawing No. EH–FM–007 // Fluid Mechanics & Piping
Fluid Mechanics Formula Sheet
Part 1 of the EngineerHub fluid-mechanics reference series: internal flow and pump systems. It connects flow rate, velocity, pressure, friction, pump head and cavitation. Each section includes variable definitions, SI and US customary units, a worked example and a direct link to the corresponding EngineerHub calculator.
From continuity to NPSH
Use the sheet as a quick reference or follow it in sequence. The equations assume conventional engineering sign conventions; always use a consistent unit system inside a calculation.
Reference conventions
Energy grade line along a pipe run
01 // Continuity
Conservation of mass links flow area and velocity. For an incompressible fluid of constant density, volumetric flow rate is conserved through a single streamtube.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| Q | Volumetric flow rate | m³/s, L/s | ft³/s, gpm |
| A | Flow area normal to velocity | m² | ft², in² |
| v | Mean cross-sectional velocity | m/s | ft/s |
| ṁ | Mass flow rate | kg/s | lbm/s |
| ρ | Fluid density | kg/m³ | lbm/ft³ |
For compressible flow, conserve mass rather than volume: ρ₁A₁v₁ = ρ₂A₂v₂. For a circular pipe, A = πD²/4. For non-circular internal flow, use hydraulic diameter Dh = 4A/Pw, where Pw is wetted perimeter.
Worked example — flow from pipe diameter and velocity
Given: water flows through a 100 mm internal-diameter pipe at an average velocity of 2.0 m/s.
US check: US equivalent: Q ≈ 249 US gpm.
Area–velocity relationship
02 // Bernoulli equation
Bernoulli expresses mechanical energy per unit weight along a streamline. The extended form includes pump head, turbine extraction and irreversible head losses.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| p | Static pressure | Pa, kPa | psf or psi (convert psi × 144 before p/γ) |
| γ | Specific weight = ρg | N/m³ | lbf/ft³ |
| ρ | Mass density | kg/m³ | lbm/ft³ |
| α | Kinetic-energy correction coefficient | dimensionless | dimensionless |
| v | Mean fluid velocity | m/s | ft/s |
| z | Elevation datum | m | ft |
| Hₚ | Head added by pump | m fluid | ft fluid |
| Hₜ | Head removed by turbine | m fluid | ft fluid |
| hL | Total irreversible head loss | m fluid | ft fluid |
The ideal form assumes steady, incompressible flow along a streamline. For ordinary turbulent pipe-flow screening, α ≈ 1 is commonly used; for fully developed laminar circular-pipe flow, α = 2. The extended form adds shaft work and irreversible head loss.
Worked example — reservoir to atmospheric discharge
Given: water is pumped from a large open reservoir to an atmospheric pipe discharge 10 m higher. The discharge velocity is 2.0 m/s, total head loss is 3.0 m, and the source-reservoir free-surface velocity is negligible.
US check: US equivalent: required pump head ≈ 43.32 ft.
Head terms are all lengths
Bernoulli is especially convenient because pressure head, velocity head and elevation head are expressed in the same unit: metres or feet of the flowing fluid. Using specific weight γ keeps the head equation dimensionally clean in both SI and US customary systems.
US: h(ft) = 144·Δp(psi)/γ(lbf/ft³). For water-like liquids, h(ft) ≈ 2.31·Δp(psi)/SG.
03 // Reynolds number
Reynolds number compares inertial and viscous effects and is the primary regime indicator for internal flow.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| Re | Reynolds number | dimensionless | dimensionless |
| ρ | Density | kg/m³ | lbm/ft³ |
| v | Mean velocity | m/s | ft/s |
| D | Pipe internal diameter / hydraulic diameter | m | ft |
| μ | Dynamic viscosity | Pa·s | lbm/(ft·s) |
| ν | Kinematic viscosity = μ/ρ | m²/s | ft²/s |
For circular pipe flow, a common engineering classification is laminar Re ≲ 2300, transition ≈ 2300–4000, and turbulent Re ≳ 4000. For non-circular ducts use Dh = 4A/Pw. Transition depends on inlet disturbances, roughness and geometry.
Worked example — water in a 50 mm pipe
Given: 20°C water, ρ = 998 kg/m³, μ = 1.002×10⁻³ Pa·s, v = 2.0 m/s, D = 0.050 m.
US check: Using ρ ≈ 62.30 lbm/ft³, μ ≈ 6.733×10⁻⁴ lbm/(ft·s), v ≈ 6.562 ft/s and D ≈ 0.1640 ft gives the same Re ≈ 99,600.
Why Reynolds matters downstream
- It determines whether laminar friction factor f = 64/Re applies.
- It affects turbulent friction-factor correlations such as Colebrook or Swamee–Jain.
- It influences heat-transfer and mass-transfer correlations.
- It helps interpret whether a scale model is dynamically similar.
04 // Darcy–Weisbach major loss
The Darcy–Weisbach equation gives frictional loss along a straight pipe. It is dimensionally consistent and widely applicable when the Darcy friction factor is known.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| hƒ | Major head loss | m fluid | ft fluid |
| Δpƒ | Major pressure loss | Pa | psf; divide by 144 for psi |
| f | Darcy friction factor | dimensionless | dimensionless |
| L | Straight pipe length | m | ft |
| D | Internal / hydraulic diameter | m | ft |
| v | Mean velocity | m/s | ft/s |
| g | Gravitational acceleration | m/s² | ft/s² |
| γ | Specific weight | N/m³ | lbf/ft³ |
Important: this page uses the Darcy friction factor. The Fanning factor is one quarter of the Darcy value: fF = fD/4.
Worked example — straight-pipe loss
Given: f = 0.020, L = 50 m, D = 0.100 m, v = 2.0 m/s, water density ≈ 998 kg/m³.
US check: US equivalent: hƒ ≈ 6.691 ft and Δpƒ ≈ 2.895 psi.
Choosing the Darcy friction factor
Laminar circular pipe:
Turbulent pipe — Colebrook–White:
Here ε is absolute roughness and ε/D is relative roughness. Colebrook is implicit in f; a Moody chart or validated explicit approximation is often more convenient.
Transition region: friction is less predictable; do not treat Re = 2300 or 4000 as a perfectly sharp physical switch.
05 // Minor / local losses
Fittings, entrances, exits, valves and local geometry changes are commonly represented by dimensionless loss coefficients.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| hₘ | Minor / local head loss | m fluid | ft fluid |
| K | Loss coefficient for fitting / component | dimensionless | dimensionless |
| v | Reference velocity associated with K | m/s | ft/s |
| Leq | Equivalent straight-pipe length | m | ft |
| f | Darcy friction factor | dimensionless | dimensionless |
Use the velocity specified for the coefficient source. For area changes, a coefficient may be based on upstream, downstream or throat velocity; mixing definitions can produce large errors.
Worked example — fittings represented by ΣK
Given: combined fitting coefficient ΣK = 4.5 and pipe velocity v = 2.0 m/s.
US check: US equivalent: local head loss ≈ 3.011 ft.
“Minor” does not mean negligible
In short piping systems, suction lines, valve stations or heavily fitted process systems, local losses can equal or exceed straight-pipe friction.
06 // Pump hydraulic and shaft power
Pump head becomes hydraulic power through flow rate and fluid specific weight. Pump and motor efficiencies determine the shaft and electrical input required.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| Pₕ | Hydraulic power delivered to fluid | W, kW | hp |
| γ | Specific weight | N/m³ | lbf/ft³ |
| ρ | Mass density | kg/m³ | lbm/ft³ |
| Q | Volumetric flow rate | m³/s | ft³/s, US gpm |
| H | Total pump head | m fluid | ft fluid |
| ηₚ | Pump efficiency | fraction or % | fraction or % |
| ηₘ | Motor efficiency | fraction or % | fraction or % |
| SG | Specific gravity for practical US pump-power form | dimensionless | dimensionless |
Use total dynamic head at the actual operating point, not only static elevation. Total head can include static head, pressure difference, velocity-head change and pipe/fitting losses. The 3960 constant is the conventional US gpm–ft–horsepower conversion used with specific gravity.
Worked example — shaft power
Given: water, ρ = 998 kg/m³, Q = 0.020 m³/s, pump head H = 25 m, pump efficiency ηₚ = 0.75.
US check: US equivalent: hydraulic power ≈ 6.56 hp and pump shaft/input power ≈ 8.75 hp. The conventional 3960 form gives essentially the same result, subject to its rounded conversion constant.
Energy chain
07 // Net positive suction head (NPSH)
NPSH measures how far the pump suction condition lies above the liquid vapor-pressure head. Use absolute pressures.
| Symbol | Meaning | SI units | US customary |
|---|---|---|---|
| NPSHₐ | Net positive suction head available | m liquid | ft liquid |
| γ | Liquid specific weight | N/m³ | lbf/ft³ |
| pₛ,abs | Absolute static suction pressure | Pa absolute | psia (×144 for psf in p/γ) |
| vₛ | Suction-pipe mean velocity | m/s | ft/s |
| pᵥ | Liquid vapor pressure at temperature | Pa absolute | psia |
| pₐtm | Atmospheric pressure | Pa absolute | psia |
| zstatic | Liquid-surface elevation above pump datum; negative for lift | m | ft |
| hL,suction | Suction-line losses | m liquid | ft liquid |
NPSH required is a pump characteristic supplied by the manufacturer for a defined test criterion. Published rotodynamic-pump curves commonly use NPSH3: the NPSH available at which total head has fallen by 3% at the specified condition. NPSHA equal to NPSH3 therefore does not mean zero cavitation or full non-cavitating performance. Establish margin from applicable pump/vendor/project guidance rather than assuming one universal margin.
US customary: convert pressure to head as h(ft) = 144·p(psia)/γ(lbf/ft³). Use absolute pressure for atmospheric, suction and vapor-pressure terms.
Worked example — open tank suction
Given: water at about 20°C, ρ = 998 kg/m³, atmospheric pressure 101.325 kPa absolute, vapor pressure 2.34 kPa absolute, liquid surface 2.0 m above the pump, and suction-line loss 1.0 m.
US check: US equivalent: NPSHA ≈ 36.46 ft of water.
What lowers NPSHa?
- Higher liquid temperature → higher vapor pressure.
- Higher elevation above sea level → lower atmospheric pressure.
- Longer / smaller suction piping → greater suction friction loss.
- Higher flow → greater velocity and usually greater suction losses.
- Liquid level below the pump centerline → negative static contribution.
08 // How the equations fit together
A pipe-and-pump calculation usually moves through these relationships in sequence rather than treating them as isolated equations.
The pump operating point is the intersection of the pump curve and the system curve. Friction-factor variation means the exact system curve is not always a perfect Q² parabola.
09 // Quick formula summary
Use this table as the compact print reference. The detailed sections above contain definitions and assumptions.
| Topic | Equation | Main purpose | EngineerHub tool |
|---|---|---|---|
| Continuity | Q = Av | Relate area, velocity and volumetric flow | Pipe Velocity |
| Hydraulic diameter | Dh = 4A/Pw | Characteristic diameter for non-circular internal flow | Reynolds Number |
| Bernoulli | p/γ + αv²/2g + z = H | Mechanical energy / head balance | Bernoulli |
| Reynolds | Re = ρvD/μ | Classify internal-flow regime | Reynolds Number |
| Friction factor | f = 64/Re (laminar); Colebrook for turbulent | Determine Darcy friction factor | Moody Chart |
| Major loss | hƒ = f(L/D)v²/(2g) | Straight-pipe friction loss | Darcy–Weisbach |
| Minor loss | hₘ = ΣK v²/(2g) | Fittings / valves / local geometry | Pipe Flow & Head Loss |
| Pressure ↔ head | Δp = γh | Convert pressure loss and head loss | Pipe Flow & Head Loss |
| Pump power | Pₕ = γQH = ρgQH | Convert hydraulic duty to power | Pump System |
| NPSH available | pₛ,abs/γ + vₛ²/2g − pᵥ/γ | Assess suction condition above vapor pressure | Pump NPSH |
10 // Assumptions, units & reference notes
The formulas are simple; choosing the correct inputs and conventions is the real engineering work.
In SI, a clean base set is metres, seconds, kilograms, pascals and watts. In US customary calculations, distinguish mass density (lbm/ft³) from specific weight (lbf/ft³). If lbm is inserted directly into force equations, the gravitational conversion constant gc ≈ 32.174 lbm·ft/(lbf·s²) is required. This sheet avoids that common trap in head/pressure equations by using specific weight γ. For pump horsepower, use the explicit US gpm–ft–SG–3960 form. Avoid mixing psi with psf or inches with feet without conversion.
- Pressure head: h(ft) = 144·Δp(psi)/γ(lbf/ft³). For water-like liquids, h(ft) ≈ 2.31·Δp(psi)/SG.
- Pressure from head: Δp(psi) = γ(lbf/ft³)·h(ft)/144.
- Darcy and minor-loss head: use D, L and h consistently in ft, velocity in ft/s and g ≈ 32.174 ft/s².
- Reynolds number: ρ in lbm/ft³ and μ in lbm/(ft·s) cancel consistently; no gc is needed in Re.
- Pump power: use Q in US gpm, H in ft, SG dimensionless and η as a fraction with the 3960 horsepower form.
- NPSH: use absolute pressure; convert psia to psf before dividing by γ, or use the explicit 144 multiplier.
- The page is aimed at steady, single-phase engineering flow problems unless stated otherwise.
- Compressible gas flow, choking, water hammer, two-phase flow and non-Newtonian fluids require additional models.
- Fitting K values, roughness values, viscosity, vapor pressure and pump NPSHr should come from appropriate project/vendor/reference data.
- Bernoulli / energy equations do not replace a momentum balance where forces and reactions are the primary unknowns.
- NPSH available is a system calculation; NPSH required is pump-specific test/catalog data.
The equations shown are standard fluid-mechanics relations. EngineerHub calculators may implement additional correlations and assumptions beyond the compact forms shown here; review each calculator's Background and limitations before design use.
- NASA Glenn — Bernoulli's Equation: assumptions and mechanical-energy interpretation.
- Hydraulic Institute Data Tool — Pump Curves: pump power, efficiency and the US 3960 conversion.
- Hydraulic Institute — Pump FAQs: NPSH3 definition and pump-performance interpretation.
- NIST TN 2294 — Pressure Losses in Pipes and Fittings: friction-factor and fitting-loss measurement basis.
11 // Related fluid mechanics tools
Use the formula sheet as the entry point, then move to the full calculators for input handling, unit conversion and expanded assumptions.