The entrance length for pipe flow is a function of Reynolds number for both turbulent flow and laminar flow. You probably recall that turbulent flow will occur for flow in a pipe or duct if the Reynolds Number (Re) is greater than 4000. Most pipe flow of gases and liquids with a viscosity similar to water is turbulent flow.
For turbulent flow the entrance length, Le, can be estimated from the equation: Le/D = 4.4Re1/6.
where Re = DVρ/μ for flow in circular pipes and Re = 4RHVρ/μ for flow in non-circular ducts, and
D = pipe diameter, ft
V = average flow velocity in pipe (= Q/A), ft/sec
ρ = fluid density, slugs/ft3
μ = fluid viscosity, lb-sec/ft2
RH = hydraulic radius, ft, where RH = A/P, and
A = cross-sectional area normal to flow, ft2
P = wetted perimeter of pipe or duct cross-section, ft
Laminar flow in pipes and ducts takes place for Reynolds Number less than 2100, with Reynolds Number as defined just above. Laminar flow in pipes will occur only for very viscous fluids and/or very slow flows.
For Laminar Flow, the entrance length, Le, can be estimated from the equation: Le/D = 0.06 Re.