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The horizontal boundaries of the convection cell are a rhodiumplated copper mirror on the bottom and a sapphire window on the top.
To model an unbounded system, we have therefore been led to conduct the present experiments in an annular convection cell.
It is possible to make a convection cell with mean circumference of greater than 100 times the cell height.
These density differences result in rising and/or falling currents, which are the key characteristics of a convection cell.
A convection cell is most notable in the formation of clouds with its release and transportation of energy.
Such movement is called convection, and the moving body of liquid is referred to as a "convection cell".
Such hexagons are one example of a convection cell.
It is the "sinking" limb of a convection cell.
One obvious method to suppress higher-dimensional behaviour in convection in rectangular containers is t o use narrow convection cells.
The z-independent perturbation to the stream function is positive in the region near the wall where the convection cells are strongest.
In this investigation an initial disturbance of the form of the counter-rotating convection cells predicted by linear theory was used.
However, the linear results have counter-rotating convection cells, and experiments have only revealed cells that all rotate in the same direction.
The instabilities that evolved consisted only of co-rotating convection cells.
The heat is dissipated through large-scale convection cells.
By its very nature the linear stability analysis predicts counter-rotating convection cells.