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The computation of turbulent natural convection flows - Turbulence ...

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Introduction 42<br />

1.2 Turbulent flow<br />

1.2.1 Characteristics<br />

Most <strong>flows</strong> found in industrial applications are <strong>turbulent</strong> <strong>flows</strong>. Among<br />

these industrial applications, we can identify boundary layers growing on air-<br />

craft wings, combustion processes, <strong>natural</strong> gas and oil flow in pipelines and<br />

the wakes <strong>of</strong> ships, cars, submarines and aircraft.<br />

It is difficult to state a definition for <strong>turbulent</strong> flow. <strong>The</strong> best way is to<br />

explain different characteristics <strong>of</strong> the turbulence. <strong>The</strong> first feature <strong>of</strong> turbu-<br />

lent flow is irregularity. That is why analytical methods are not suitable for<br />

<strong>turbulent</strong> flow and statistical and numerical methods are employed to resolve<br />

the <strong>turbulent</strong> flow. Another characteristic <strong>of</strong> turbulence is its diffusivity. <strong>The</strong><br />

turbulence diffusivity is used to denote the mixing <strong>of</strong> momentum, mass and<br />

thermal energy by the <strong>turbulent</strong> eddies. <strong>The</strong> diffusivity <strong>of</strong> turbulence is the<br />

most important effect <strong>of</strong> turbulence in industrial applications. For example it<br />

will delay separation in <strong>flows</strong> over airfoils at high angles <strong>of</strong> attack, or will in-<br />

crease heat transfer rates etc.<br />

Two major dimensionless numbers in forced and mixed <strong>convection</strong> are the<br />

Rayleigh and Reynolds numbers. <strong>The</strong>y are defined as:<br />

Ra = βg∆ΘL3<br />

να<br />

Re = UL<br />

ν<br />

where the symbols are defined as: β: volumetric expansion coefficient,g: grav-<br />

ity acceleration, ∆Θ: temperature difference, L: length scale, ν: kinetic viscos-<br />

ity, α: thermal diffusivity and U: velocity scale.<br />

Turbulent <strong>flows</strong> occur at high Reynolds numbers in the case <strong>of</strong> forced con-<br />

vection and at high Rayleigh numbers in the case <strong>of</strong> <strong>natural</strong> <strong>convection</strong>. Be-<br />

cause <strong>of</strong> the inherent apparent randomness and the nonlinearity <strong>of</strong> <strong>turbulent</strong><br />

<strong>flows</strong>, the phenomenon is almost intractable. Both mathematical models and

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