Reynolds numbers: Difference between revisions

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== Reynolds number ==
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<div class="definition"><div class="short_definition">The dimensionless ratio of the [[inertial force]] (&sim;''U''<sup>2</sup>/''L'') to the [[viscous force]] (&sim; &#x003bd;''U''/''L''<sup>2</sup>) in the [[Navier&ndash;Stokes equations]], where ''U'' is a [[characteristic velocity]],  ''L'' is a [[characteristic length]], and &#x003bd; is the [[kinematic viscosity]] of the fluid; thus,  <div class="display-formula"><blockquote>[[File:ams2001glos-Re39.gif|link=|center|ams2001glos-Re39]]</blockquote></div></div><br/><div class="paragraph">The Reynolds number is of great importance in the theory of [[hydrodynamic stability]] and the  origin of [[turbulence]]. The inertia force generates [[vortex stretching]] and [[nonlinear]] interactions  and hence creates [[randomness]]. Turbulence occurs when the inertia term dominates the viscous  term, that is, when the Reynolds number is large. For many engineering flows, turbulence occurs  when Re &gt; Re<sub>c</sub>, where the critical Reynolds number is roughly Re<sub>c</sub> = 2100. <br/>''See'' [[large Reynolds number flow]].</div><br/> </div>
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