๐ŸŒŠ Reynolds Number & Entry Length

Compute Reynolds number, classify flow regimes, find hydraulic diameter, and estimate entry lengths for pipes, flat plates, annuli, and rectangular ducts.

โšก Fortran 90 Engine Double Precision (IEEE 754) โœ“ ISO / ASME Validated
Reynolds Number & Entry Length Fluid Mechanics
๐Ÿ“Š Solver Telemetry โ— ACTIVE
๐Ÿ‘๏ธ Views 3,850
โšก Solves 3,046
๐Ÿ’พ Downloads 599 ๐Ÿ“ฆ Fortran Code 4.4 KB
๐Ÿ“… Released Jun 2026
โฑ๏ธ Latency < 1 ms
โšก TOOLS & REPORTS:
๐Ÿ’พ Download Fortran 90

๐Ÿ“ Configuration

๐Ÿ“ Geometry
๐ŸŒŠ Flow Conditions
Key Equations:

Re = ฯยทVยทD_h / ฮผ
D_h = D (pipe), L (plate)
D_h = D_oโˆ’D_i (annulus)
D_h = 4WH/[2(W+H)] (duct)
Laminar: Re < 2300, Turbulent: Re > 4000

๐Ÿ“Š Results

Configure inputs and click Compute to view results.

๐Ÿ“˜ Methodology

Reynolds Number

Re = ฯVD_h/ฮผ is the ratio of inertial to viscous forces. It determines the flow regime: laminar (Re < 2300 for internal flow, Re < 5ร—10โต for external), transition, or turbulent.

Hydraulic Diameter

For non-circular cross-sections, the hydraulic diameter D_h = 4A/P (4ร— cross-sectional area / wetted perimeter) is used. For an annulus D_h = D_o โˆ’ D_i, for a rectangular duct D_h = 2WH/(W+H).

Entry Length

The hydrodynamic entry length is the distance for the velocity profile to fully develop. Laminar: L_e โ‰ˆ 0.05ยทReยทD. Turbulent: L_e โ‰ˆ 4.4ยทRe^(1/6)ยทD (shorter relative to pipe diameter).

๐Ÿ“˜ Calculation Methodology: Reynolds Number & Flow Regime Classification

Mathematical Model & Theory

The Reynolds number $Re$ represents the fundamental ratio of inertial forces to viscous forces in a fluid flow, determining the boundary between laminar, transitional, and turbulent regimes:

$$Re = \frac{\rho V D}{\mu} = \frac{V D}{\nu} = \frac{4 \dot{m}}{\pi D \mu}$$
$$\text{Internal Pipe Flow: } Re < 2300\ (\text{Laminar}), \quad 2300 \le Re \le 4000\ (\text{Transitional}), \quad Re > 4000\ (\text{Turbulent})$$

Assumptions

  • Newtonian fluid with constant dynamic viscosity $\mu$.
  • Characteristic length $D$ defined as internal pipe diameter or hydraulic diameter $D_h = 4A/P$.

Academic References

  1. Reynolds, O. (1883): An experimental investigation of the circumstances which determine whether the motion of water shall be direct or sinuous, Phil. Trans. Roy. Soc.
  2. White, F. M.: Fluid Mechanics, Ch. 6.

Worked Engineering Example

Problem Statement:
Fuel oil ($\rho = 890\text{ kg/m}^3$, $\mu = 0.080\text{ Pa}\cdot\text{s}$) flows through a pipeline of diameter $D = 150\text{ mm}$ at flow rate $Q = 45\text{ m}^3/\text{h}$ ($0.0125\text{ m}^3/\text{s}$). Determine the flow regime.

Step-by-step Solution:
1. Calculate mean velocity: $V = 4 Q / (\pi D^2) = 4(0.0125) / (\pi \times 0.15^2) = 0.050 / 0.07069 \approx 0.7073\text{ m/s}$.
2. Compute Reynolds number: $Re = (890 \times 0.7073 \times 0.15) / 0.080 = 94.42 / 0.080 \approx 1180$.
3. Classify regime: $Re = 1180 < 2300 \implies$ **Laminar Flow**.
Final Result:
$Re = \mathbf{1180}$ (Strictly Laminar Flow with parabolic velocity profile).