Laminar Thermal-Driven Cavity
Analysis Characteristics
- Steady-state
- 2D internal flow
- Laminar
- Incompressible
- Natural convection
Reference
Davis, G. De Vahl and Jones, I.P., “Natural convection in a square cavity: a comparison exercise”, Inter. Jour. for Num. Meth. in Fluids, 3, (1983).
Problem Description
Temperature and velocity distributions are calculated for laminar, buoyancy-driven flow in a square cavity. The top and bottom walls are insulated, and the left and right walls are at fixed temperatures differing by 1 K.
The Rayleigh number is computed from:

is the coefficient of volumetric expansion, defined as: 
g is the acceleration of gravity
is the density
is the specific heatL is the length of the cavity
and
are the temperatures of the left and right walls, respectivelyk is the conductivity of the fluid
is the viscosity.Here, the Rayleigh number is 10,000.
This problem is analyzed to verify the fluid flow and heat transfer modeling capabilities of Autodesk® CFD. Accuracy is assessed by comparing velocity components at specific locations in the cavity. Velocities and coordinates are normalized in accordance with Davies, et al. (1983) as follows:

Geometry and Boundary Conditions

Results
Using the expressions defined above for
,
,
and
, the following results are computed:
| Benchmark | 2018: Build 20170308 | % Error | 2019: Build 20180130 | % Error | |
![]() | 16.178 | 16.191 | 0.079 | 16.185 | 0.04399 |
![]() | 0.823 | .825 | .243 | .825 | .243 |
![]() | 19.617 | 19.666 | .251 | 19.651 | .175 |
![]() | 0.119 | .120 | .840 | .120 | .840 |




