Author:
ESMAEELI ASGHAR,TRYGGVASON GRÉTAR
Abstract
Direct numerical simulations of the motion of two- and three-dimensional finite
Reynolds number buoyant bubbles in a periodic domain are presented. The full
Navier–Stokes equations are solved by a finite difference/front tracking method that
allows a fully deformable interface between the bubbles and the ambient fluid and
the inclusion of surface tension. The rise Reynolds numbers are around 20–30 for the
lowest volume fraction, but decrease as the volume fraction is increased. The rise of
a regular array of bubbles, where the relative positions of the bubbles are fixed, is
compared with the evolution of a freely evolving array. Generally, the freely evolving
array rises slower than the regular one, in contrast to what has been found earlier for
low Reynolds number arrays. The structure of the bubble distribution is examined
and it is found that while the three-dimensional bubbles show a tendency to line up
horizontally, the two-dimensional bubbles are nearly randomly distributed. The effect
of the number of bubbles in each period is examined for the two-dimensional system
and it is found that although the rise Reynolds number is nearly independent of
the number of bubbles, the velocity fluctuations in the liquid (the Reynolds stresses)
increase with the size of the system. While some aspects of the fully three-dimensional
flows, such as the reduction in the rise velocity, are predicted by results for two-dimensional bubbles, the structure of the bubble distribution is not. The magnitude
of the Reynolds stresses is also greatly over-predicted by the two-dimensional results.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
158 articles.
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