THE
DYNAMICS OF
WINE
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We have demonstrated that this spoke pattern results from ridge-like elevations
of the free surface supported by evaporatively-driven
Marangoni convection within the thin film. The ridges are evident in Figure 2,
which is an oblique perspective looking along the meniscus region
adjoining the reservoir (left) and the thin film (right). Tears roll
from right to left in Figure 2. Vortices associated
with small-scale convective motions are aligned in the streamwise direction
by the surface tension gradient responsible for the sustenance of
the tears. The convective motions are revealed by adding Kalliroscope to
the fluid, and are evident in Figure 3, a plan view of a wine glass
in which the reservoir is at the bottom, the thin film in the middle
and the incipient tear line at the top. Finally, when the angle of
inclination of the glass is very small, the meniscus region is marked by
a dendritic free-surface structure (Figure 4).
The results of our combined experimental, theoretical and numerical models of evaporatively-driven convective instabilities in climbing films is
presented in
Hosoi
& Bush (2001).
In a wine glass, evaporation of alcohol creates Marangoni stresses
that cause the wine to climb to the top of the thin film, where it
accumulates in a band that grows until becoming gravitationally
unstable and releasing the `tears of wine'. The tears of wine are evident
in Figure 1, a plan view of a wine glass. Also evident in
Figure 1 is a fine radial spoke pattern in the meniscus, which accompanies
the tears of wine in strong alcoholic beverages.
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