1990
DOI: 10.1098/rspa.1990.0088
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Thermal transport properties of carbon-carbon fibre composites III. Mathematical modelling

Abstract: Measured thermal transport data are interpreted using data obtained by careful microstructural characterization concerning the porosity distribution and graphite grain sizes. The separate thermal conductivity components for one-dimensional composites are deduced using a simple series addition to determine ג f1 and ג m1 and using an adaptation of the Bruggeman analysis for calculating ג f┴ and … Show more

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Cited by 19 publications
(7 citation statements)
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“…(A8) describes transverse heat conduction through a two-phase medium: the matrix material is treated as a continuous phase and the cylindrical fibres as a discontinuous phase. The shape factor X = 1 relates to a regular array of cylindrical fibres (Whittaker and Taylor, 1990). Rearrangement of Eq.…”
Section: Discussionmentioning
confidence: 99%
“…(A8) describes transverse heat conduction through a two-phase medium: the matrix material is treated as a continuous phase and the cylindrical fibres as a discontinuous phase. The shape factor X = 1 relates to a regular array of cylindrical fibres (Whittaker and Taylor, 1990). Rearrangement of Eq.…”
Section: Discussionmentioning
confidence: 99%
“…This expression, which can be found as eqn (12) in Mottram & Taylor (1987), has its origins in the work of Rayleigh (1892) and subsequently that of Bruggeman (1935). This development has been reviewed by Clayton (1971) and formalized by Mottram & Taylor (1987) and Whittaker & Taylor (1990). Equation (3.3) describes transverse heat conduction through a two-phase medium: the inner matrix material is treated as the continuous phase and the cylindrical fibres as the discontinuous phase.…”
Section: (B) Transverse Thermal Response Of a Uni-directional Towmentioning
confidence: 99%
“…Equation (10) describes transverse heat conduction through a two-phase medium: the matrix material is treated as a continuous phase and the cylindrical fibres as a discontinuous phase. The shape factor X ¼ 1 relates to a regular array of cylindrical fibres (Whittaker and Taylor, 1990). Rearrangement of equation (10) Table B2 from Tang et al (2011b) b. Degradation of tow transverse thermal conductivity with strain due to matrix cracking and wake debonding: A unidirectional tow, Figure 2(a), can be divided into many identical blocks of a length equal to the matrix crack spacing, w, as shown in Figure 2(b).…”
Section: Initialmentioning
confidence: 99%
“…is the transverse thermal conductivity for the fibre or discontinuous phase; k im is the thermal conductivity for the continuous phase or inner matrix; and the parameter X is a shape factor for the discontinuous phase. The development of equation (10) has been formalised by Whittaker and Taylor (1990). Equation (10) describes transverse heat conduction through a two-phase medium: the matrix material is treated as a continuous phase and the cylindrical fibres as a discontinuous phase.…”
Section: Initialmentioning
confidence: 99%
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