Modeling of a non-Newtonian thin film passing a thin porous medium

This theoretical study deals with asymptotic behavior of a coupling between a thin film of fluid and an adjacent thin porous medium. We assume that the size of the microstructure of the porous medium is given by a small parameter 0 < ε ≪ 1, the thickness of the thin porous medium is defined by a parameter 0 < hε ≪ 1, and the thickness of the thin film is defined by a small parameter 0 < ηε ≪ 1, where hε and ηε are devoted to tend to zero when ε → 0. In this paper, we consider the case of a non-Newtonian fluid governed by the incompressible Stokes equations with power law viscosity of flow index r ∈ (1,+∞), and we prove that there exists a critical regime, which depends on r, between ε, ηε and hε. More precisely, in this critical regime given by hε ≈ ηε2r−1/r−1ε−(r/r−1), we prove that the effective flow when ε → 0 is described by a 1D Darcy law coupled with a 1D Reynolds law.

Publication Details

Journal
Springer Link (Chiba Institute of Technology)
Published
2025-09-22
DOI
https://doi.org/10.1051/mmnp/2025020/pdf
Primary Topic
Fluid Dynamics and Thin Films
Type
article
Field-Weighted Citation Impact
0.00
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

Modeling of a non-Newtonian thin film passing a thin porous medium

Springer Link (Chiba Institute of Technology)
Fluid Dynamics and Thin Films
article

Modeling of a non-Newtonian thin film passing a thin porous medium

article en

Abstract

This theoretical study deals with asymptotic behavior of a coupling between a thin film of fluid and an adjacent thin porous medium. We assume that the size of the microstructure of the porous medium is given by a small parameter 0 < ε ≪ 1, the thickness of the thin porous medium is defined by a parameter 0 < hε ≪ 1, and the thickness of the thin film is defined by a small parameter 0 < ηε ≪ 1, where hε and ηε are devoted to tend to zero when ε → 0. In this paper, we consider the case of a non-Newtonian fluid governed by the incompressible Stokes equations with power law viscosity of flow index r ∈ (1,+∞), and we prove that there exists a critical regime, which depends on r, between ε, ηε and hε. More precisely, in this critical regime given by hε ≈ ηε2r−1/r−1ε−(r/r−1), we prove that the effective flow when ε → 0 is described by a 1D Darcy law coupled with a 1D Reynolds law.

Springer Link (Chiba Institute of Technology)
Peace, Justice and strong institutions
Openalex Percentile: Top 31%
Fluid Dynamics and Thin Films
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.