Flow Across Banks of Tubes

Evaluate convection coefficients and pressure drop across inline or staggered tube banks using the Zukauskas correlation.

Flow (V) Pitch S_L Pitch S_T

Aligned vs Staggered Bundles

In crossflow over tube banks, the configuration (inline or staggered) alters the maximum velocity $V_{max}$ inside the bundle channels. Max velocity dictates the Reynolds number ($\text{Re}_{max}$) and the heat transfer rates.

Parameters Setup

📐 Geometry Setup
📐 Flow & Temperatures
💧 Fluid Properties

Results & Curves

4.257e+4
Reynolds Re_max
2.000 m/s
Max Velocity V_max
409.20
Nusselt Nu
13202.0983
h [W/m²K]
1065.17 Pa
Pressure Drop dP

📈 Convection coefficient h vs Velocity

Engine Output

============================================
  FLOW ACROSS BANKS OF TUBES
============================================

--- INPUTS ---
  Configuration           = INLINE
  Number of Rows N        =      8
  Tube Diameter D         =     0.0190 m
  Transverse Pitch S_T    =     0.0380 m
  Longitudinal Pitch S_L  =     0.0380 m
  Approach Velocity V     =      1.000 m/s
  T_inf                   =      20.00 C
  T_surface               =      80.00 C

--- GEOMETRY ---
  S_T / D                 =    2.000
  S_L / D                 =    2.000
  Maximum Velocity V_max  =      2.000 m/s

--- RESULTS ---
  Reynolds Re_max         =     4.2569E+04
  C1 (Zukauskas)          =     0.2700
  m  (Zukauskas)          =     0.6300
  C2 (row correction)     =     0.9567
  Nusselt Number Nu       =       409.20
  Convection Coeff h      =   13202.0983 W/m2K
  Pressure Drop dP        =      1065.17 Pa
  dP per row              =       133.15 Pa

--- VELOCITY SWEEP ---
  V[m/s]   Vmax[m/s]  Re_max       Nu        h[W/m2K]  dP[Pa]
  -----------------------------------------------------------------
     0.50       1.00    2.128E+04     264.42    8530.885      297.52
     0.65       1.29    2.749E+04     310.68   10023.487      476.47
     0.79       1.58    3.370E+04     353.20   11395.271      693.00
     0.94       1.87    3.991E+04     392.90   12676.077      945.90
     1.08       2.17    4.612E+04     430.36   13884.911     1234.19
     1.23       2.46    5.232E+04     466.01   15034.803     1557.05
     1.38       2.75    5.853E+04     500.11   16135.174     1913.79
     1.52       3.04    6.474E+04     532.90   17193.108     2303.82
     1.67       3.33    7.095E+04     564.55   18214.098     2726.59
     1.81       3.62    7.716E+04     595.18   19202.515     3181.63
     1.96       3.92    8.336E+04     624.92   20161.903     3668.51
     2.10       4.21    8.957E+04     653.85   21095.190     4186.83
     2.25       4.50    9.578E+04     682.04   22004.826     4736.24
     2.40       4.79    1.020E+05     709.57   22892.890     5316.41
     2.54       5.08    1.082E+05     736.48   23761.162     5927.02
     2.69       5.38    1.144E+05     762.83   24611.184     6567.79
     2.83       5.67    1.206E+05     788.65   25444.299     7238.46
     2.98       5.96    1.268E+05     813.98   26261.691     7938.76
     3.12       6.25    1.330E+05     838.86   27064.404     8668.47
     3.27       6.54    1.392E+05     863.32   27853.371     9427.35
     3.42       6.83    1.454E+05     887.37   28629.424    10215.21
     3.56       7.12    1.517E+05     911.05   29393.313    11031.82
     3.71       7.42    1.579E+05     934.37   30145.715    11877.01
     3.85       7.71    1.641E+05     957.35   30887.245    12750.59
     4.00       8.00    1.703E+05     980.02   31618.463    13652.39

--- CORRELATIONS ---
  Zukauskas: Nu = C1*C2*Re_max^m * Pr^0.36 * (Pr/Pr_s)^0.25
  Ref: Incropera Ch.7 Eq.7.58, Kothandaraman Ch.8 Sec.8.6

Calculation Methodology

Mathematical Model & Theory

Heat transfer across tube bundles is modeled using the Zukauskas correlation: $$\text{Nu}_D = C_1 C_2 \text{Re}_{max}^m \text{Pr}^{0.36} \left(\frac{\text{Pr}}{\text{Pr}_s}\right)^{0.25}$$ - $C_1$ and $m$ are constants determined from the Reynolds number range ($\text{Re}_{max} = \rho V_{max} D / \mu$). - $C_2$ is a row correction factor for banks with fewer than 20 rows ($N_L < 20$).

For aligned arrangement, maximum velocity is: $$V_{max} = V \frac{S_T}{S_T - D}$$ For staggered arrangement, if the diagonal flow area is smaller than the transverse area, then: $$V_{max} = V \frac{S_T}{2(S_D - D)}$$ Aerodynamic pressure drop is calculated using friction factors: $$\Delta P = N \chi f \frac{\rho V_{max}^2}{2}$$

Academic References:

  1. Incropera, F. P., & DeWitt, D. P. (2011). Fundamentals of Heat and Mass Transfer. 7th Edition, John Wiley & Sons.
  2. Zukauskas, A. (1972). Heat Transfer from Tubes in Crossflow. Advances in Heat Transfer.

Worked Engineering Example

Problem Statement:
Air at $25^\circ\text{C}$ flows at $5\text{ m/s}$ across an inline tube bank of 10 rows. Tubes of diameter $25\text{ mm}$ are arranged with pitches $S_T = S_L = 50\text{ mm}$. Surface temp is $100^\circ\text{C}$ ($T_f = 62.5^\circ\text{C}$). Find the convection coefficient $h$.

Step-by-step Solution:
1. Evaluate air properties at film temperature:
- $\rho = 1.177\text{ kg/m}^3, \mu = 1.85 \times 10^{-5}\text{ Pa·s}, k = 0.0263\text{ W/m·K}, Pr = 0.71$.
2. Calculate maximum velocity $V_{max}$:
$$V_{max} = V \frac{S_T}{S_T - D} = 5.0 \times \frac{0.05}{0.05 - 0.025} = 10.0\text{ m/s}$$ 3. Calculate maximum Reynolds number:
$$\text{Re}_{max} = \frac{\rho V_{max} D}{\mu} = \frac{1.177 \times 10.0 \times 0.025}{1.85 \times 10^{-5}} = 15,905$$ 4. From Zukauskas constants ($10^3 < \text{Re}_{max} < 2 \times 10^5$, inline):
- $C_1 = 0.27, m = 0.63$. For 10 rows, $C_2 = 0.97$.
$$\text{Nu}_D = 0.27 \times 0.97 \times (15,905)^{0.63} \times (0.71)^{0.36} \times 1.0 = 93.5$$ 5. Calculate convective coefficient $h$:
$$h = \frac{\text{Nu}_D k}{D} = \frac{93.5 \times 0.0263}{0.025} = 98.4\text{ W/m}^2\text{K}$$