Density (real gas): ρ (kg/m³) = P·M / (Z·R·T) — P in Pa (abs), M in kg/kmol, R = 8314.5 J/(kmol·K), T in K
Reynolds number (mass-flow form, density-independent): Re = 4·ṁ / (π·dᵢ·η)
Churchill friction factor (valid for laminar, transitional and turbulent flow):
λ = 8 × [ (8/Re)¹² + 1/(A+B)^1.5 ]^(1/12)
A = { 2.457 × ln[ 1 / ((7/Re)^0.9 + 0.27·ε/dᵢ) ] }¹⁶ B = (37530/Re)¹⁶
Friction pressure drop (mass-flow form): ΔP (Pa) = (8/π²) × λ × L × ṁ² / (ρ · dᵢ⁵) ρ per the density-basis method above
Static head (elevation, approximate): ΔP_static ≈ ρ_avg · g · H — H = elevation change (m), positive going up; gas columns are usually a minor term compared to friction, shown here only as a rough check
Velocity Head ΔP (dynamic) — applied at diameter transitions between segments, using the shared node density: ΔP_dynamic = ½ρ(v_prev² − v_this²)
Pressure profile, carried segment to segment from the starting pressure P₀: P_in(segment) = P_out(previous) + ΔP_dynamic P_out(segment) = P_in(segment) − ΔP_friction − ΔP_static
L is each segment's total equivalent length (straight + fittings) from the worksheet above.
| Pipe material | Absolute roughness ε (mm) |
Typical absolute roughness values for preliminary sizing — always confirm with your project's piping material specification.
Preliminary Velocity Guidelines — Rule of Thumb
| Service | Typical range |
| Air / other gases (non-corrosive, non-erosive) | 10 – 20 m/s (up to 60 m/s if ρv² ≤ 50,000 kg/(m·s²)) |
| Saturated steam (dry) | 15 – 30 m/s |
| Superheated steam | 30 – 60 m/s |
| Vacuum piping | 10 – 100 m/s |
Disclaimer: These are generic, rounded rule-of-thumb figures for a quick preliminary sizing pass only — not values from any specific company, licensor, or industry-code specification. Suitable ranges vary significantly with fluid, material, service, and criticality. Always confirm against your own project's design basis and piping specification before finalizing a line size, and use a rigorous compressible-flow calculation wherever this method is flagged as not applicable.