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Effective thermal conductivity of media with randomly distributed convective gas-filled spheres

•Maxwell effective conductivity (kef) model is extended to include natural convection•kef calculated by single gas-filled sphere solution and dilute medium approximation•Approximate analytical formula is proposed•For a large part of parametric space one of two analytical approximations apply One of...

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Bibliographic Details
Published in:International journal of heat and mass transfer 2023-01, Vol.200, p.123457, Article 123457
Main Authors: Nissim Sagir, Michal, Rabinovich, Avinoam
Format: Article
Language:English
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Summary:•Maxwell effective conductivity (kef) model is extended to include natural convection•kef calculated by single gas-filled sphere solution and dilute medium approximation•Approximate analytical formula is proposed•For a large part of parametric space one of two analytical approximations apply One of the most well-known models for effective thermal conductivity (kef) is the Maxwell model, which considers a medium with a dilute concentration of spherical inclusions. In this work the Maxwell model is extended to include natural convection in the spheres. We consider a medium with randomly distributed gas-filled (hollow) spheres subjected to a constant heat flux. A method for calculating kef based on the dilute medium approximation is presented and applied to investigate kef, considering a variety of dimensionless parameters of the problem. Based on a large number of kef calculations, an approximate analytical formula is proposed (βc approximation). Furthermore, in many cases the convective effects are minor and can be neglected so that the Maxwell analytical formula can be applied (βMax approximation). The applicability of βc and βMax is studied considering a wide range of dimensionless parameters. It is found that for almost the entire parametric space one of the analytical approximations apply and therefore numerical calculations can be avoided.
ISSN:0017-9310
1879-2189
DOI:10.1016/j.ijheatmasstransfer.2022.123457