This paper deals with some results on the creep behaviour of a 2.5D C-f-SiC
composite. This material fabricated by CVI was tested in tension under an
argon partial pressure for temperatures ranging from '1273 to 1673 K and st
resses between 110 and 220 MPa. Results regarding creep curves (strain-time
) and strain rate-time curves tend to confirm the existence of a secondary
stage. Damage-stress and damage-time curves are also presented. The limits
of the Dorn's formalism are evidenced as well as the occurrence of a damage
process leading to a so-called damage-creep mechanism. In order to explain
this macroscopic creep behaviour of the composite, investigations at the m
esoscopic, microscopic and nanoscopic scales were necessary. Five modes of
matrix microcracking are observed together with different pull-out features
regarding the extracted fibre surface. The damage accumulation via matrix
microcracking appears to be a time dependent mechanism. Two modes of interf
acial sliding are evidenced: at 1473 K and 220 MPa, the pyrocarbon (PyC) in
terphase is fractured leading to debonding between carbon layers, while at
1673 K, there is a loss of anisotropy of the PyC layer close to the matrix
and, thus, an interfacial sliding appearing as a viscous flow. To elucidate
the role of the carbon fibres, a nanoscale study via HREM has been conduct
ed. An increase of the mean diameters of the basic structural units (BSUs)
and of the areas of local molecular orientation (LMOs) within the fibres ha
s been observed when increasing temperature under 220 MPa. In fact, these c
hanges do not contribute to the macroscopic strain. Therefore, this restruc
turation effect has been called "nanocreep" of the carbon fibre as it appea
rs to have a negligible contribution to the macroscopic creep behaviour of
the 2.5D Cf-SiC composite, (C) 1999 Kluwer Academic Publishers.