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Computer simulation of thermal convection in Rayleigh-Bénard cell ...

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Hubert Jopek<br />

<strong>Computer</strong> <strong>simulation</strong> <strong>of</strong> <strong>thermal</strong> <strong>convection</strong> <strong>in</strong> <strong>Rayleigh</strong>-<strong>Bénard</strong> <strong>cell</strong><br />

are determ<strong>in</strong>ed by the sign <strong>of</strong> velocity as a result <strong>of</strong> <strong>in</strong>creas<strong>in</strong>g or decreas<strong>in</strong>g fluid<br />

<strong>in</strong> the centre <strong>of</strong> the <strong>cell</strong>. Ma<strong>in</strong>ly g-<strong>cell</strong>s appear <strong>in</strong> gasses (that is the reason why<br />

the name is g-<strong>cell</strong>) and the l-<strong>cell</strong>s can be observed <strong>in</strong> liquids (so the name is l-<br />

<strong>cell</strong>s).<br />

Fig 7.1: Schematic diagram <strong>of</strong> <strong>convection</strong> <strong>cell</strong>s (a) two-dimensional rolls. (b)<br />

Hexagonal l- and g-<strong>cell</strong>s.<br />

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