Evaporation of liquids from structured and non-structured mixtures (original) (raw)

2004

The work presented in this thesis describes the evaporation rates of a wide variety of samples obtained under a controlled gas flow using a gravimetric technique. Evaporation rates for pure liquids with vapour pressures ranging from 0.1 to 500 Torr, water contained in silica particles, alkane/squalane mixtures, hexane gelled with silica particles, surfactant/water mixtures, immiscible layered liquid mixtures and emulsions have been determined. For pure liquids and simple unstructured liquid mixtures, the evaporation rate is limited by diffusion through a stagnant vapour layer at the liquid surface. As the degree of structure within the liquid mixture increases, the time taken for concentration gradients developing in the evaporation process to relax becomes longer relative to the time taken for diffusion through the stagnant vapour layer. For highly structured liquid mixtures, the rate limiting process switches to diffusion and convection within the liquid mixture. In the case of cr...

A comparison between the experimental and estimated evaporation paths from emulsions

Flavour and …, 2009

The evaporation paths in linalool emulsions were experimentally determined using a rotary evaporator coupled to a vacuum pump and calculated from vapour pressures for a series of emulsions with varied oil/water (O/W) ratios. The evaporation paths were comparable to an acceptable degree, suggesting that determination of the evaporation path under reduced pressure, combined with a straightforward calculation using vapour pressures, can be used to estimate the evaporation under different relative humilities. Copyright © 2009 John Wiley & Sons, Ltd.

Interface conditions governing evaporation of stored liquids in presence of non-condensable gas

International Journal of Heat and Mass Transfer, 2006

Experiments were conducted to determine the variation of interface temperatures during the storage and draining of liquid nitrogen from large containers in the presence of the non-condensable gas. A chilled layer was seen to be formed at the interface in the presence of the non-condensable gas and this layer advanced into the warm liquid at speeds higher than the characteristic

Loading...

Loading Preview

Sorry, preview is currently unavailable. You can download the paper by clicking the button above.