Non-Circular Duct & Annulus Convection

Calculate forced convection coefficients and outlet temperatures for non-circular pipe geometries.

Side W

Hydraulic Diameter Concept

For non-circular ducts, fluid flow parameters are evaluated by using the hydraulic diameter ($D_h$) defined as: $$D_h = \frac{4 A_c}{P}$$ where $A_c$ is the cross-sectional area and $P$ is the wetted perimeter.

Parameters Setup

📐 Geometry Selection
📐 Flow & Length
🌡️ Temperatures
💧 Fluid Properties

Results & Curves

0.028868
Hydraulic Diameter [m]
3.2338E+04
Reynolds Re
Turbulent
Regime
213.80
Nusselt Nu
4539.9335
h [W/m²K]
27239.60
Heat rate Q [W]
26.04
T_out [°C]

📈 Nusselt number vs Velocity

Engine Output

============================================
  NON-CIRCULAR DUCT & ANNULUS CONVECTION
============================================

--- INPUTS ---
  Geometry                = Equilateral Triangle
  Boundary Condition      = Uniform Heat Flux (H)
  Velocity V              =     1.0000 m/s
  Inlet Temp T_in         =      20.00 C
  Wall Temp T_wall        =      60.00 C
  Pipe Length L            =       1.00 m

--- GEOMETRY ---
  Hydraulic Diameter D_h  =     0.028868 m
  Cross Section Area A    =   1.0825E-03 m2
  Wetted Perimeter P      =     0.150000 m
  Aspect / Radius Ratio   =      1.000

--- FLUID PROPERTIES ---
  Density rho             =     997.0000 kg/m3
  Viscosity mu            =   8.9000E-04 Pa.s
  Conductivity k          =     0.613000 W/mK
  Prandtl Pr              =       6.1300

--- RESULTS ---
  Reynolds Number Re      =     3.2338E+04
  Flow Regime             = Turbulent
  Friction Factor f       =   0.023214
  Nusselt Number Nu       =       213.80
  Convection Coeff h      =    4539.9335 W/m2K
  Heat Transfer Q         =     27239.60 W
  Outlet Temperature T_out=      26.04 C
  Entry Length Le          =     0.2887 m
  Mass Flow Rate          =   1.0793E+00 kg/s

--- VELOCITY SWEEP ---
  V[m/s]     Re           Nu        h[W/m2K]   Regime
  --------------------------------------------------------
     0.100   3.234E+03      23.59     500.937  Turbulent
     0.263   8.489E+03      64.90    1378.154  Turbulent
     0.425   1.374E+04     100.91    2142.788  Turbulent
     0.588   1.900E+04     134.49    2855.922  Turbulent
     0.750   2.425E+04     166.54    3536.533  Turbulent
     0.912   2.951E+04     197.49    4193.767  Turbulent
     1.075   3.476E+04     227.59    4832.948  Turbulent
     1.238   4.002E+04     257.01    5457.529  Turbulent
     1.400   4.527E+04     285.85    6069.923  Turbulent
     1.563   5.053E+04     314.19    6671.896  Turbulent
     1.725   5.578E+04     342.12    7264.797  Turbulent
     1.887   6.104E+04     369.66    7849.688  Turbulent
     2.050   6.629E+04     396.87    8427.419  Turbulent
     2.212   7.155E+04     423.77    8998.691  Turbulent
     2.375   7.680E+04     450.39    9564.089  Turbulent
     2.538   8.206E+04     476.77   10124.104  Turbulent
     2.700   8.731E+04     502.91   10679.161  Turbulent
     2.862   9.257E+04     528.83   11229.623  Turbulent
     3.025   9.782E+04     554.55   11775.810  Turbulent
     3.188   1.031E+05     580.08   12318.002  Turbulent
     3.350   1.083E+05     605.44   12856.447  Turbulent
     3.512   1.136E+05     630.63   13391.367  Turbulent
     3.675   1.188E+05     655.66   13922.960  Turbulent
     3.838   1.241E+05     680.55   14451.404  Turbulent
     4.000   1.294E+05     705.29   14976.862  Turbulent

--- CORRELATIONS ---
  Laminar: Nu from geometry tables (Incropera Table 8.1)
  Turbulent: Gnielinski Nu=(f/8)(Re-1000)Pr/[1+12.7sqrt(f/8)(Pr^2/3-1)]
  f = (0.790 ln Re - 1.64)^-2
  Ref: Incropera Ch.8 Sec.8.6, Kothandaraman Ch.9 Sec.9.6

Calculation Methodology

Mathematical Model & Theory

Forced convection in non-circular ducts uses the hydraulic diameter: $$D_h = \frac{4 A_c}{P}$$ - Laminar Regime ($\text{Re} \le 2300$): Nusselt numbers are constants interpolated from numerical geometry tables (Incropera Table 8.1 & 8.3) based on aspect ratio (rectangular) or radius ratio (annular).

- Turbulent Regime ($\text{Re} > 2300$): Gnielinski correlation is employed: $$\text{Nu} = \frac{(f/8)(\text{Re} - 1000)\text{Pr}}{1 + 12.7\sqrt{f/8}\left(\text{Pr}^{2/3} - 1\right)}$$ where friction factor $f$ is: $$f = (0.790 \ln \text{Re} - 1.64)^{-2}$$

Academic References:

  1. Incropera, F. P., & DeWitt, D. P. (2011). Fundamentals of Heat and Mass Transfer. 7th Edition, John Wiley & Sons.
  2. Gnielinski, V. (1976). New Equations for Heat and Mass Transfer in Turbulent Pipe and Channel Flow. Int. Chem. Eng.

Worked Engineering Example

Problem Statement:
Air at $25^\circ\text{C}$ flows at $3.0\text{ m/s}$ through a rectangular duct of $100\text{ mm} \times 50\text{ mm}$ wetted walls at $80^\circ\text{C}$. Find the convection coefficient ($T_f = 52.5^\circ\text{C}$).

Step-by-step Solution:
1. Evaluate air properties at film temp:
- $\rho = 1.177\text{ kg/m}^3, \mu = 1.85 \times 10^{-5}\text{ Pa·s}, k = 0.0263\text{ W/m·K}, Pr = 0.71$.
2. Calculate wetted perimeter, wetted area, and hydraulic diameter:
- $A_c = 0.1 \times 0.05 = 0.005\text{ m}^2$
- $P = 2 \times (0.1 + 0.05) = 0.3\text{ m}$
- $D_h = 4 \times 0.005 / 0.3 = 0.0667\text{ m}$
3. Calculate Reynolds number:
$$\text{Re} = \frac{\rho V D_h}{\mu} = \frac{1.177 \times 3.0 \times 0.0667}{1.85 \times 10^{-5}} = 12,735 \quad \text{(Turbulent)}$$ 4. Compute friction factor and Nusselt number (Gnielinski):
- $f = (0.790 \ln(12,735) - 1.64)^{-2} = 0.029$
$$\text{Nu} = \frac{(0.029/8) \times (12,735 - 1000) \times 0.71}{1 + 12.7\sqrt{0.029/8}(0.71^{2/3} - 1)} = 35.8$$ 5. Calculate $h$:
$$h = \frac{\text{Nu} k}{D_h} = \frac{35.8 \times 0.0263}{0.0667} = 14.1\text{ W/m}^2\text{K}$$