Transient and steady convection in two dimensions
arXiv:2503.03080 · doi:10.1017/jfm.2025.10357
Abstract
We simulate thermal convection in a two-dimensional square box using the no-slip condition on all boundaries, and isothermal bottom and top walls and adiabatic sidewalls. We choose 0.1 and 1 for the Prandtl number and vary the Rayleigh number between and . We particularly study the temporal evolution of integral transport quantities towards their steady states. Perhaps not surprisingly, the velocity field evolves more slowly than the thermal field, and its steady state -- which is nominal in the sense that large-amplitude low-frequency oscillations persist around plausible averages -- is reached exponentially. We study these oscillation characteristics. The transient time for the velocity field to achieve its nominal steady state increases almost linearly with the Reynolds number. For large , the Reynolds number itself scales almost as , and the Nusselt number as .
To appear in the Journal of Fluid Mechanics
References in corpus (21)
- Scaling in thermal convection: A unifying theory
- Thermal convection for large Prandtl numbers
- Radial boundary layer structure and Nusselt number in Rayleigh-Benard convection
- A Comparison of Turbulent Thermal Convection Between Conditions of Constant Temperature and Constant Flux
- Comparison between two and three dimensional Rayleigh-Bénard convection
- Transition to the ultimate regime in two-dimensional Rayleigh-Bénard convection
- Prandtl and Rayleigh number dependence of heat transport in high Rayleigh number thermal convection
- Phenomenology of buoyancy-driven turbulence: recent results
- Resolving the fine-scale structure in turbulent Rayleigh-Benard convection
- Connecting flow structures and heat flux in turbulent Rayleigh-Bénard convection
- Scaling of large-scale quantities in Rayleigh-Bénard convection
- Global and local statistics in turbulent convection at low Prandtl numbers
- Steady Rayleigh--Bénard convection between stress-free boundaries
- Thermal boundary layer structure in low-Prandtl-number turbulent convection
- Absence of Evidence for the Ultimate Regime in Two-Dimensional Rayleigh-Bénard Convection
- Absence of Evidence for the 'Ultimate' State of Turbulent Rayleigh-Bénard Convection
- Dynamics of large-scale quantities in Rayleigh-Bénard convection
- Similarities between 2D and 3D convection for large Prandtl number
- No sustained mean velocity in the boundary region of plane thermal convection
- Convective heat transport in slender cells is close to that in wider cells at high Rayleigh and Prandtl numbers
- Similarities between characteristics of convective turbulence in confined and extended domains