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Huinink HP, Pel L, Michels MA, et al. Drying processes in the presence of temperature gradients--pore-scale modelling. Eur Phys J E Soft Matter. 2002;9(5):487-98doi: 10.1140/epje/i2002-10106-1.
Huinink, H. P., Pel, L., Michels, M. A., & Prat, M. (2002). Drying processes in the presence of temperature gradients--pore-scale modelling. The European physical journal. E, Soft matter, 9(5), 487-98. https://doi.org/10.1140/epje/i2002-10106-1
Huinink, H P, et al. "Drying processes in the presence of temperature gradients--pore-scale modelling." The European physical journal. E, Soft matter vol. 9,5 (2002): 487-98. doi: https://doi.org/10.1140/epje/i2002-10106-1
Huinink HP, Pel L, Michels MA, Prat M. Drying processes in the presence of temperature gradients--pore-scale modelling. Eur Phys J E Soft Matter. 2002 Dec;9(5):487-98. doi: 10.1140/epje/i2002-10106-1. PMID: 15011097.
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Eur Phys J E Soft Matter. 2002 Dec;9(5):487-98. doi: 10.1140/epje/i2002-10106-1.

Drying processes in the presence of temperature gradients--pore-scale modelling.

The European physical journal. E, Soft matter

H P Huinink, L Pel, M A J Michels, M Prat

Affiliations

  1. Department of Applied Physics, Technische Universiteit Eindhoven, Postbus 513, 5600 MB Eindhoven, The Netherlands. [email protected]

PMID: 15011097 DOI: 10.1140/epje/i2002-10106-1

Abstract

The influence of temperature gradients on the drying of water-saturated porous networks has been studied. We have focussed on the influence of the temperature on the drying process via the equilibrium vapor density rhoe, because this is the most sensitive parameter with respect to variations of the temperature T. We have used a 2D model which accounts for both capillary and buoyancy forces. Invasion events by air or water are handled by standard rules of invasion percolation in a gradient (IPG). Vapor fluxes are calculated by solving a discretized version of the Laplace equation. In the model the temperature T varies linearly from the open side T0 to the closed side TL. The temperature gradients strongly influence the cluster evolution during the process, because they facilitate vapor transport through wet regions. When T0TL, the front movement is enhanced and the air ingress in the wet region behind the front is inhibited. The behavior of 3D systems differs from that of 2D systems, because the point where air percolates the system and the point where the water network breaks up in isolated clusters do not coincide. Before the latter fragmentation point the temperature will mainly influence the drying rates. After this point also the water distribution becomes sensitive to the temperature profile.

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