The thermal conductivity (λ
F) of alumina and zirconia fibrous insulators with various bulk densities was measured by the hot wire method between room temperature and 1400°C in air. The thermal conductivity of as-received alumina fiber which consisted of δ-Al
2O
3 phase increased with increasing temperature. The temperature dependence of thermal conductivity of alumina fibers heated at temperatures above 1250°C having densities larger than 0.2g/cm
3, showed parabolic curves with a minima between 300°C and 500°C. It was found that the difference in temperature dependence of thermal conductivities was caused by the transformation of δ-Al
2O
3 into α-Al
2O
3 which has a high thermal conductivity in the low temperature region. The thermal conductivity of zirconia fiber increased with increasing temperature as in the case of δ-Al
2O
3 fiber. The low bulk density ceramic fibers showed high λ
F-values at high temperatures due to the contribution of thermal radiation, while at low temperatures λ
F-values were small. The polycrystalline fibrous insulators such as alumina and zirconia fibers showed λ
F-values lower than those of glassy one such as kaolin wool in the high temperature region because of the reflection of radiation at the fiber surfaces. The following experimental relation between λ
F (thermal conductivity) and θ (temperature) was obtained for fibrous insulators:
λ
F=
a⋅exp(
bθ).
It was found that a certain relationship exists between the constants
a and
b and the volume fraction of fiber. The λ
F-value and its temperature dependence of δ-Al
2O
3 ceramics were estimated on the basis of the relation.
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