Forced Convection Over Spheres

Determine boundary layer heat transfer coefficients and total heat rate for flows over spherical surfaces.

Flow (V) Ts Diameter D

External Flow Over Sphere

Similar to crossflow over cylinders, flow separates from the rear side of spheres, creating a low-pressure wake region. Convection is analyzed using empirical correlations that account for the fluid viscosity change near the surface ($\mu/\mu_s$).

Parameters Setup

📐 Geometry & Flow
🌡️ Temperatures
💧 Fluid Properties

Results & Curves

1.2724E+04
Reynolds Re
68.3574
Nu (Whitaker)
62.3793
Nu (Ranz-Marshall)
179.7799
h [W/m²K]
2.2592
Heat loss Q [W]

📈 Nusselt number vs Velocity

Engine Output

============================================
  CONVECTION OVER SPHERE ENGINE
============================================

  Reynolds Re             =     1.2724E+04
  Whitaker Nu             =      68.3574
  Ranz Nu                 =      62.3793
  Coeff h                 =     179.7799 W/m2K
  Transfer Q              =       2.2592 W

--- VELOCITY SWEEP ---
  V[m/s]     Re           Nu_Whitaker  Nu_Ranz      h[W/m2K]   Q[W]
  -------------------------------------------------------------------------
     0.050   3.181E+01        4.437        5.019     11.6701        0.1467
     3.381   2.151E+03       26.345       26.826     69.2865        0.8707
     6.713   4.271E+03       37.755       36.980     99.2968        1.2478
    10.044   6.390E+03       46.881       44.788    123.2977        1.5494
    13.375   8.509E+03       54.786       51.376    144.0878        1.8107
    16.706   1.063E+04       61.895       57.184    162.7829        2.0456
    20.038   1.275E+04       68.428       62.436    179.9664        2.2615
    23.369   1.487E+04       74.521       67.267    195.9897        2.4629
    26.700   1.699E+04       80.260       71.764    211.0844        2.6526
    30.031   1.911E+04       85.708       75.988    225.4130        2.8326
    33.362   2.123E+04       90.911       79.983    239.0950        3.0046
    36.694   2.335E+04       95.902       83.784    252.2212        3.1695
    40.025   2.546E+04      100.708       87.416    264.8624        3.3284
    43.356   2.758E+04      105.352       90.899    277.0756        3.4818
    46.687   2.970E+04      109.851       94.251    288.9072        3.6305
    50.019   3.182E+04      114.219       97.486    300.3955        3.7749
    53.350   3.394E+04      118.469      100.614    311.5727        3.9153
    56.681   3.606E+04      122.611      103.647    322.4664        4.0522
    60.013   3.818E+04      126.654      106.591    333.0999        4.1859
    63.344   4.030E+04      130.606      109.455    343.4938        4.3165
    66.675   4.242E+04      134.474      112.244    353.6657        4.4443
    70.006   4.454E+04      138.263      114.964    363.6315        4.5695
    73.338   4.666E+04      141.979      117.621    373.4048        4.6923
    76.669   4.878E+04      145.627      120.218    382.9982        4.8129
    80.000   5.090E+04      149.210      122.759    392.4226        4.9313

Calculation Methodology

Mathematical Model & Theory

Convective heat transfer over a spherical object is evaluated using two primary models:

1. Whitaker Correlation: $$\text{Nu}_D = 2 + \left(0.4 \text{Re}_D^{1/2} + 0.06 \text{Re}_D^{2/3}\right) \text{Pr}^{0.4} \left(\frac{\mu}{\mu_s}\right)^{1/4}$$ where fluid properties (except $\mu_s$) are evaluated at the free-stream temperature $T_\infty$.

2. Ranz-Marshall Correlation: $$\text{Nu}_D = 2 + 0.6 \text{Re}_D^{1/2} \text{Pr}^{1/3}$$ This correlation is a classical simplification widely used for droplets and evaporating sprays.

Academic References:

  1. Incropera, F. P., & DeWitt, D. P. (2011). Fundamentals of Heat and Mass Transfer. 7th Edition, John Wiley & Sons.
  2. Whitaker, S. (1972). Forced Convection Heat Transfer Correlations for Flow in Pipes, Past Flat Plates, Single Cylinders, Single Spheres, and for Flow in Packed Beds and Tube Bundles. AIChE J.

Worked Engineering Example

Problem Statement:
Air at $25^\circ\text{C}$ flows at $5.0\text{ m/s}$ past a $50\text{ mm}$ sphere maintained at $100^\circ\text{C}$. Find the convective heat loss ($T_\infty = 25^\circ\text{C}$).

Step-by-step Solution:
1. Evaluate air properties at free-stream temp $25^\circ\text{C}$:
- $\rho = 1.177\text{ kg/m}^3, \mu = 1.85 \times 10^{-5}\text{ Pa·s}, k = 0.0263\text{ W/m·K}, Pr = 0.71$.
- At $T_s = 100^\circ\text{C}$, $\mu_s \approx 2.18 \times 10^{-5}\text{ Pa·s}$.
2. Calculate Reynolds number:
$$\text{Re}_D = \frac{\rho V D}{\mu} = \frac{1.177 \times 5.0 \times 0.05}{1.85 \times 10^{-5}} = 15,905$$ 3. Evaluate Nusselt number via Whitaker correlation:
$$\text{Nu}_D = 2 + \left[0.4 \times (15,905)^{1/2} + 0.06 \times (15,905)^{2/3}\right] \times (0.71)^{0.4} \times \left(\frac{1.85}{2.18}\right)^{1/4}$$ $$\text{Nu}_D = 2 + \left[50.4 + 37.9\right] \times 0.87 \times 0.96 = 75.8$$ 4. Convection coefficient $h$:
$$h = \frac{\text{Nu}_D k}{D} = \frac{75.8 \times 0.0263}{0.05} = 39.9\text{ W/m}^2\text{K}$$ 5. Surface area $A_s = \pi D^2 = \pi \times 0.05^2 = 0.00785\text{ m}^2$. Total heat loss:
$$Q = h A_s (T_s - T_\infty) = 39.9 \times 0.00785 \times (100-25) = 23.5\text{ W}$$