A B S T R A C T The random distribution of single-fibre tensile strength has been commonly characterized by the two-parameter Weibull statistics. However, the calibrated Weibull model from one set of strength data at a given gauge length cannot accurately predicts the strength variation of the fibre at different gauge lengths. Instead of presuming the twoparameter Weibull distribution or any other specific statistical distribution for the single-fibre strength to begin with, this work proposes an approach to incorporating the appropriate spatial flaw distribution within a fibre and synchronizing multiple sets of tensile strength data to evaluate the single-fibre strength distribution. The approach is examined and validated by published single-fibre strength data sets of glass, ceramic and synthetic and natural carbon fibres. It is shown that the single-fibre strength statistics does not necessarily always follow the two-parameter Weibull distribution.Keywords fibre; fibre-reinforced composite; flaw distribution; size effect; tensile strength; weakest link model.
N O M E N C L A T U R Ea = microcrack size a max = maximum microcrack size a min = minimum microcrack size c, α, β = constants f(a) = probability density function of microcrack with respect to size a g(S) = probability density function of microcrack with respect to strength S k = resistance to fracture l = length l 0 = reference length m = shape parameter M = 1/V 0 , average number of flaws in unit volume p = pressure p (σ, V 0 ) = fracture probability of an elemental volume V 0 under stress σ P = cumulative probability of failure R 2 = coefficient of determination S = strength of an elemental volume V 0 containing a microcrack of size a, S ¼ k = ffiffi a p RMSE = root-mean-square error V = volume of fracture process zone dV, δV = differential volume element ρ = average density of flaws in unit length μ = location parameter σ = strength or stress σ 1 = maximum principal stress σ 0 = scale parameter σ th = threshold strength ξ = a stress value in the range σ th ≤ ξ ≤ σ