Thermal Conductivity 18 pp 733-742 | Cite as

# Error Analysis and Equations for the Thermal Conductivity of Composites

## Abstract

The overall effective thermal conductivity (K) of a composite is a function of the thermal conductivities (K_{1}) and volume fractions (ϕ_{i}) of each of the constituents. Probable errors (ΔK. and Δϕ_{i}) for each of the constituents lead to a probable error (ΔK) in the overall thermal conductivity. For realistic problems, the exact function K(K_{i}, ϕ_{i}) is not known since it depends on the way the constituents are distributed. For this reason equations which describe the bounds on the thermal conductivity, for given K_{i} and ϕ_{i}, are very useful. Using standard calculational techniques, we plot K, K + ΔK, and K − ΔK versus volume fraction of one constituent for several cases of two-phase systems. These include the series and parallel cases as “absolute bounds” and the Maxwell equations which are the bounds for systems which are isotropic and homogeneous. We find, for common values of K_{1}/K_{2}, that the bounding equations overlap when errors are considered. This implies three things: (1) A measurement of thermal conductivity of a composite, when errors are taken into account, may not allow discrimination between cases. (2) For many cases of experimental interest a rough calculation is quite sufficient. (3) The bounds on the thermal conductivity are really not unconditional when errors are taken into account. We also consider two-phase composites where cylinders are embedded in a matrix. Complications in the calculation of the thermal conductivity include the effect of radiation, the effect of moisture and convection, and thermal resistance in the interface between phases.

## Keywords

Thermal Conductivity Probable Error Effective Thermal Conductivity Effective Dielectric Constant Rough Calculation## Preview

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