Volume 66, Number 6, June 2004
|Page(s)||812 - 818|
|Section||Electromagnetism, optics, acoustics, heat transfer, classical mechanics, and fluid dynamics|
|Published online||01 June 2004|
Pattern formation without heating in an evaporative convection experiment
Departamento de Física y Matemática Aplicada, Facultad de Ciencias Universidad de Navarra - 31080 Pamplona, Spain
Corresponding author: firstname.lastname@example.org
Accepted: 19 April 2004
We present an evaporation experiment in a single fluid layer reproducing conditions of volatile fluids in nature. When latent heat associated to the evaporation is large enough, the heat flow through the free surface of the layer generates temperature gradients that can destabilize the conductive motionless state giving rise to convective cellular structures without any external heating. Convective cells can be then observed in the transient range of evaporation from an initial depth value to a minimum threshold depth, after which a conductive motionless state appears until the evaporation finishes with an unwetting sequence. The sequence of convective patterns obtained here without heating is similar to that obtained in Bénard-Marangoni convection. This work presents the sequence of spatial bifurcations as a function of the layer depth. The transition between square-to-hexagonal pattern, known from non-evaporative experiments, is obtained here with a similar change in wavelength.
PACS: 47.54.+r – Pattern selection; pattern formation / 47.20.Dr – Surface-tension-driven instability / 47.20.Hw – Morphological instability; phase changes
© EDP Sciences, 2004
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.