A. Hampe et C. Marotzke, THE ENERGY-RELEASE RATE OF THE FIBER POLYMER MATRIX INTERFACE - MEASUREMENT AND THEORETICAL-ANALYSIS/, Journal of reinforced plastics and composites, 16(4), 1997, pp. 341-352
A new method for the experimental determination of the fracture toughn
ess in the fiber/matrix interface by means of the single fiber pull ou
t test is presented. To achieve this aim, two problems had to be overc
ome: the measurement of the compliance of a partial debonded fiber, wh
ich necessitates a stable crack propagation, and the determination of
the corresponding crack length. Stable crack propagation along the int
erface of a single fiber is achieved using an advanced test equipment
exhibiting an extremely high stiffness. This is obtained by using a pi
ezo translator and a piezo force cell in combination with a very short
free fiber length. The experimental data and a theoretical analysis o
f the pull out process under these conditions reveal that the commonly
used compliant pull out equipment is hiding important details of the
force displacement trace and, thus, leading to a wrong interpretation
and wrong results.The most important result is that in the case of a b
rittle interfacial fracture the maximal force cannot be used for the d
etermination of an interfacial strength as it is common practise till
now. The crack length is measured with the aid of a polarisation micro
scope. A combination of the advanced pull out experiment with a simult
aneous monitoring of the photoelastic patterns of the embedded fiber e
nables the determination of G(c)-values as a function of the crack len
gth. For the calculation of G(c) the compliance data are obtained by t
he force displacement trace and the crack length data by the correlate
d photo-elastic patterns. The discrimination between the failure modes
is obtained by finite element analysis. The energy release rates for
different fiber/matrix combinations are presented. In addition the pho
toelastic patterns give evidence, that in the case of a glass fiber th
e crack starts at the matrix surface and in the case of a carbon fiber
with an embedded length < 150 mu m the crack starts at the fiber tip.