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

1.5905E+04
Reynolds Re
76.1093
Nu (Whitaker)
69.5061
Nu (Ranz-Marshall)
40.0335
h [W/m²K]
23.5817
Heat loss Q [W]

📈 Nusselt number vs Velocity

Engine Output

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

  Reynolds Re             =     1.5905E+04
  Whitaker Nu             =      76.1093
  Ranz Nu                 =      69.5061
  Coeff h                 =      40.0335 W/m2K
  Transfer Q              =      23.5817 W

--- VELOCITY SWEEP ---
  V[m/s]     Re           Nu_Whitaker  Nu_Ranz      h[W/m2K]   Q[W]
  -------------------------------------------------------------------------
     0.050   1.591E+02        7.706        8.751      4.0534        2.3877
     0.881   2.803E+03       29.757       30.341     15.6523        9.2200
     1.712   5.448E+03       42.326       41.507     22.2636       13.1144
     2.544   8.092E+03       52.442       50.150     27.5847       16.2487
     3.375   1.074E+04       61.230       57.462     32.2068       18.9713
     4.206   1.338E+04       69.144       63.916     36.3698       21.4236
     5.037   1.602E+04       76.426       69.759     40.2003       23.6799
     5.869   1.867E+04       83.223       75.136     43.7750       25.7856
     6.700   2.131E+04       89.629       80.144     47.1447       27.7705
     7.531   2.396E+04       95.713       84.850     50.3448       29.6556
     8.363   2.660E+04      101.524       89.302     53.4018       31.4563
     9.194   2.925E+04      107.102       93.539     56.3356       33.1844
    10.025   3.189E+04      112.475       97.587     59.1619       34.8492
    10.856   3.453E+04      117.668      101.471     61.8932       36.4581
    11.688   3.718E+04      122.699      105.209     64.5397       38.0170
    12.519   3.982E+04      127.586      108.817     67.1100       39.5310
    13.350   4.247E+04      132.341      112.306     69.6111       41.0043
    14.181   4.511E+04      136.976      115.688     72.0492       42.4405
    15.012   4.776E+04      141.501      118.973     74.4295       43.8426
    15.844   5.040E+04      145.925      122.168     76.7564       45.2133
    16.675   5.304E+04      150.255      125.280     79.0340       46.5549
    17.506   5.569E+04      154.497      128.315     81.2656       47.8694
    18.337   5.833E+04      158.659      131.279     83.4545       49.1587
    19.169   6.098E+04      162.744      134.177     85.6032       50.4244
    20.000   6.362E+04      166.757      137.012     87.7143       51.6680

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:
$$Q = h A_s (T_s - T_\infty) = 39.9 \times 0.00785 \times (100-25) = 23.5\text{ W}$$