A sufficiently large number of bending tests of a recrystallized silic
on carbide ceramic was performed, which gave a fundamental set of stre
ngth values. From this fundamental set, arbitrary subsets of size M we
re chosen by a Monte-Carlo procedure and the parameters of the two-par
ametric Weibull distribution were calculated by the maximum likelihood
method. The dependence of the statistical distribution of the two par
ameters, obtained by this procedure, on the size of the subset M was i
nvestigated. It was found that the variation coefficient of the scale
parameter could be well described by the equations given in the litera
ture, whereas the variation coefficient of the Weibull modulus was muc
h higher. It has been shown that the reason for this behaviour is that
the distribution of flaws and therefore the strength of the material
does not perfectly obey the Weibull statistics, for which the theoreti
cal equations were derived. Thus, in real ceramics the numerical value
for the Weibull modulus obtained from a certain number of experiments
is even more indeterminate than described by the theoretical solution
.