TY - JOUR
T1 - Fractography of unfilled and particulate-filled epoxy resins
AU - Cantwell, W. J.
AU - Roulin-Moloney, A. C.
AU - Kaiser, T.
PY - 1988/5
Y1 - 1988/5
N2 - The objective of this work was to analyse and understand the types of fracture surface morphology found in unfilled and particulate-filled epoxy resins in the light of the thermomechanical history of the specimen (loading rate or duration of loading, temperature, strain at break). Short-term tensile tests and long-term creep tests were conducted at four different temperatures. The fracture surface features were analysed using the scanning electron and optical microscopes and, where suitable, an image analyser. In order to correlate these morphologies with certain regimes of crack velocity, fracture mechanics tests were also conducted, varying the crack speed between 10-7 and 102 m sec-1. In the case of the filled resin, the lifetime under static loading is governed by a phase of slow, sub-critical crack growth which is manifested by resin-particle debonding. Thereafter, the crack accelerates and finally may reach terminal velocities depending on the amount of stored elastic energy available at the moment of fracture.
AB - The objective of this work was to analyse and understand the types of fracture surface morphology found in unfilled and particulate-filled epoxy resins in the light of the thermomechanical history of the specimen (loading rate or duration of loading, temperature, strain at break). Short-term tensile tests and long-term creep tests were conducted at four different temperatures. The fracture surface features were analysed using the scanning electron and optical microscopes and, where suitable, an image analyser. In order to correlate these morphologies with certain regimes of crack velocity, fracture mechanics tests were also conducted, varying the crack speed between 10-7 and 102 m sec-1. In the case of the filled resin, the lifetime under static loading is governed by a phase of slow, sub-critical crack growth which is manifested by resin-particle debonding. Thereafter, the crack accelerates and finally may reach terminal velocities depending on the amount of stored elastic energy available at the moment of fracture.
UR - http://www.scopus.com/inward/record.url?scp=0024014085&partnerID=8YFLogxK
U2 - 10.1007/BF01115700
DO - 10.1007/BF01115700
M3 - Article
AN - SCOPUS:0024014085
SN - 0022-2461
VL - 23
SP - 1615
EP - 1631
JO - Journal of Materials Science
JF - Journal of Materials Science
IS - 5
ER -