Free Convection in Enclosures

Calculate heat transfer inside cavities, rectangular slots, double-pane windows, and concentric cylinders or spheres.

Di Outer Do Thot Tcold

Cavity Natural Convection

In enclosures, fluid movement is confined. For low Rayleigh numbers ($\text{Ra} \le 10^3$), heat transfer is purely conductive ($\text{Nu} \approx 1.0$). At higher Rayleigh numbers, convective circulation cells form, which significantly increases heat exchange.

Parameters Setup

📐 Geometry Configuration
🌡️ Temperatures
💧 Fluid Properties

Results & Curves

5.344e+5
Rayleigh Ra
19.9994
Nusselt Nu
139.9961
Effective h [W/m²K]
2.7999
Effective k_eff [W/mK]
63.3327
Heat rate Q [W]

📈 Nusselt number vs Delta T (dT)

Engine Output

============================================
  FREE CONVECTION IN ENCLOSURES
============================================

--- INPUTS ---
  Enclosure Type          =    5
  Gap L                   =     0.0000 m
  Height H                =     0.0000 m
  Width W                 =     0.0000 m
  T_hot                   =      70.00 C
  T_cold                  =      25.00 C
  Delta T                 =      45.00 C

--- FLUID ---
  rho                     =   870.0000 kg/m3
  mu                      =   5.0000E-02 Pa.s
  k                       =   0.140000 W/mK
  Pr                      =   500.0000
  beta                    =   7.0000E-04 1/K

--- RESULTS ---
  Rayleigh Number Ra      =     5.3443E+05
  Nusselt Number Nu       =      19.9994
  Effective h             =     139.9961 W/m2K
  k_effective             =       2.7999 W/mK
  Heat Transfer Q         =      63.3327 W (or W/m)

--- DELTA-T SWEEP ---
  dT[C]      Ra           Nu        Q[W]
  ---------------------------------------------------
      1.00   1.188E+04      7.722        0.5434
      6.58   7.819E+04     12.369        5.7302
     12.17   1.445E+05     14.421       12.3474
     17.75   2.108E+05     15.849       19.7975
     23.33   2.771E+05     16.971       27.8666
     28.92   3.434E+05     17.906       36.4374
     34.50   4.097E+05     18.714       45.4346
     40.08   4.760E+05     19.429       54.8046
     45.67   5.423E+05     20.073       64.5077
     51.25   6.087E+05     20.660       74.5126
     56.83   6.750E+05     21.201       84.7943
     62.42   7.413E+05     21.704       95.3319
     68.00   8.076E+05     22.174      106.1081
     73.58   8.739E+05     22.616      117.1081
     79.17   9.402E+05     23.033      128.3189
     84.75   1.007E+06     23.429      139.7292
     90.33   1.073E+06     23.805      151.3292
     95.92   1.139E+06     24.165      163.1099
    101.50   1.205E+06     24.509      175.0633
    107.08   1.272E+06     24.840      187.1824
    112.67   1.338E+06     25.157      199.4605
    118.25   1.404E+06     25.463      211.8917
    123.83   1.471E+06     25.759      224.4706
    129.42   1.537E+06     26.044      237.1922
    135.00   1.603E+06     26.321      250.0517

--- CORRELATIONS ---
  Vertical rect: Catton (1978) correlations
  Horizontal hot bottom: Globe-Dropkin Nu=0.069*Ra^(1/3)*Pr^0.074
  Concentric cyl: k_eff/k=0.386(Pr/(0.861+Pr))^0.25*Ra^0.25
  Concentric sph: k_eff/k=0.74(Pr/(0.861+Pr))^0.25*Ra^0.25
  Ref: Incropera Ch.9 Sec.9.8, Kothandaraman Ch.10

Calculation Methodology

Mathematical Model & Theory

Natural convection in enclosures is governed by Rayleigh number $\text{Ra}_L = g \beta \Delta T L^3 / (\nu \alpha)$. Different correlations apply:

- Vertical Rectangular Cavities: Catton's correlations based on aspect ratio $H/L$: $$\text{Nu} = C(Pr) \text{Ra}^{0.28-0.29} (H/L)^{-0.25-0.30}$$ - Horizontal Cavities (Hot Bottom): Globe-Dropkin correlation: $$\text{Nu} = 0.069 \text{Ra}^{1/3} \text{Pr}^{0.074}$$ - Concentric Annulus: Raithby & Hollands formulation: $$\frac{k_{eff}}{k} = 0.386 \left(\frac{\text{Pr}}{0.861 + \text{Pr}}\right)^{1/4} \text{Ra}_L^{1/4}$$

Academic References:

  1. Incropera, F. P., & DeWitt, D. P. (2011). Fundamentals of Heat and Mass Transfer. 7th Edition, John Wiley & Sons.
  2. Catton, I. (1978). Natural Convection in Enclosures. Proceedings of the 6th International Heat Transfer Conference.

Worked Engineering Example

Problem Statement:
A vertical double-pane window has a gap $L = 20\text{ mm}$ and height $H = 0.5\text{ m}$. The inner glass is at $60^\circ\text{C}$ and the outer glass is at $20^\circ\text{C}$. Find the heat transfer coefficient of the air slot ($T_f = 40^\circ\text{C}$).

Step-by-step Solution:
1. Evaluate properties at $40^\circ\text{C}$:
- Air: $\nu = 1.7 \times 10^{-5}\text{ m}^2\text{/s}$, $\alpha = 2.4 \times 10^{-5}\text{ m}^2\text{/s}$, $Pr = 0.707$, $\beta = 1/313.15 = 0.00319\text{ K}^{-1}$, $k = 0.0271\text{ W/m·K}$.
2. Calculate Rayleigh number $\text{Ra}_L$:
$$\text{Ra}_L = \frac{9.81 \times 0.00319 \times (60-20) \times 0.02^3}{1.7 \times 10^{-5} \times 2.4 \times 10^{-5}} = 24,534$$ 3. Evaluate aspect ratio and choose Catton correlation ($H/L = 0.5/0.02 = 25$):
Since $H/L > 10$, we use: $$\text{Nu} = 0.42 \text{Ra}_L^{0.25} \text{Pr}^{0.012} (H/L)^{-0.3}$$ $$\text{Nu} = 0.42 \times (24,534)^{0.25} \times (0.707)^{0.012} \times (25)^{-0.3} = 0.42 \times 12.52 \times 0.996 \times 0.38 = 1.99$$ 4. Convection coefficient $h_{eff}$:
$$h_{eff} = \frac{\text{Nu} k}{L} = \frac{1.99 \times 0.0271}{0.02} = 2.70\text{ W/m}^2\text{K}$$