Issue 4, 2023

Influence of heat transfer and wetting angle on condensable fluid flow through nanoporous anodic alumina membranes

Abstract

The flow of isobutane and of freon 142b (1-chloro-1,1-difluoro-ethane) through anodic alumina membranes with pore diameters between 18 and 60 nm in a capillary condensation regime is experimentally and theoretically explored. The capillary condensation effect increases the membrane permeance for condensable gases from 25 to 150 m3(STP) m−2 bar−1 h−1 at certain conditions. To describe the experimental results, a model is suggested accounting for heat transfer from the condensing to the evaporating meniscus, different boundary conditions for the heat transfer between the environment and the membrane, and wettability of the pore wall. The proposed model indicates a large influence of heat supply from the environment to the membrane on the permeance in the capillary condensation regime and a moderate influence of condensate contact angle in the range of 0–60°. Measuring the temperature of the permeate side of the membrane allows to find a suitable boundary condition to describe heat transfer. The obtained boundary condition yields an excellent fit of experimental results of condensate flow through membranes with different pore diameters for the two utilized fluids. Also, confocal Raman spectroscopy gave evidence on the fraction of pores filled with condensate.

Graphical abstract: Influence of heat transfer and wetting angle on condensable fluid flow through nanoporous anodic alumina membranes

Supplementary files

Article information

Article type
Paper
Submitted
30 Sep 2022
Accepted
26 Dec 2022
First published
10 Jan 2023
This article is Open Access
Creative Commons BY license

Phys. Chem. Chem. Phys., 2023,25, 3240-3250

Influence of heat transfer and wetting angle on condensable fluid flow through nanoporous anodic alumina membranes

T. Loimer, S. K. Podgolin, J. Sodagar-Abardeh, D. I. Petukhov and A. A. Eliseev, Phys. Chem. Chem. Phys., 2023, 25, 3240 DOI: 10.1039/D2CP04577J

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