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Technical Brief

Thermal Conductivity of Suspensions Based on Core–Shell Particles

[+] Author and Article Information
G. I. Sukhinin

Kutateladze Institute of Thermophysics,
Novosibirsk 630090, Russia;
Physics Department,
Novosibirsk State University,
Novosibirsk 630090, Russia

M. A. Serebryakova, S. A. Novopashin

Kutateladze Institute of Thermophysics,
Novosibirsk 630090, Russia

Contributed by the Heat Transfer Division of ASME for publication in the JOURNAL OF HEAT TRANSFER. Manuscript received May 12, 2015; final manuscript received January 9, 2016; published online March 22, 2016. Assoc. Editor: Andrey Kuznetsov.

J. Heat Transfer 138(6), 064501 (Mar 22, 2016) (4 pages) Paper No: HT-15-1334; doi: 10.1115/1.4032735 History: Received May 12, 2015; Revised January 09, 2016

An analytical solution of the problem of the thermal conductivity of a suspension containing core–shell particles was found. Solutions were found under the thickness of the shell tending to zero while the thermal conductivity of the shell was tending to zero and infinity. In the first case, the solution is shown to be equivalent to the solution that takes into account Kapitza interfacial thermal resistance. The role of contact Kapitza resistance in the processes of the thermal conduction of nanofluids is discussed.

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References

Figures

Grahic Jump Location
Fig. 1

The influence of the particle shell on the thermal conductivity of a suspension at φ = 0.1 and (a/b)3 = 0.5

Grahic Jump Location
Fig. 2

The influence of thermal conductivity and the thickness of the shell on the thermal conductivity of a suspension when φ = 0.1 and α = 100

Grahic Jump Location
Fig. 3

The effect of contact Kapitza resistance on the thermal conductivity of a nanofluid for aluminum oxide nanoparticles in water

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