We have measured the fracture toughness, G(o), of an interface between
polystyrene (PS) and poly (2-vinylpyridine) (PVP) reinforced with tri
block copolymers (PVP-b-dPS-b-PVP) as a function of the areal chain de
nsity, Sigma, of the copolymers at the interface. The failure mechanis
ms of the interface are studied by transmission electron microscopy an
d forward recoil spectrometry. For triblock copolymers with long PVP b
locks (N-PVP > N-ePVP, where N-ePVP is the entanglement polymerization
index of PVP), a transition from chain scission at low Sigma to crazi
ng at high Sigma is observed. By comparing the areal chain density Si
gma for the transition from chain scission to crazing for the tribloc
k copolymers (Sigma = 0.015 chains/nm(2)) to that for the diblock cop
olymers, PVP-dPS (Sigma = 0.03 chains/nm(2)), we show that most of th
e triblock copolymers form a ''staple'' structure at the interface wit
h the dPS block making a loop on the PS side of the interface and the
PVP ends anchoring the ''staple'' in the PVP side. As a result of the
''staple'' structure, the saturation areal chain density of the triblo
ck copolymer (Sigma(sat)) at the interface is half of that for the dib
lock copolymer of similar molecular weight. For Sigma < Sigma(sat) in
the crazing regime, the fracture toughness of the interface is control
led by the areal joint density, Sigma(cross), where Sigma(cross) is th
e number density of the copolymer excursions across the interface. For
Sigma > Sigma(sat), the triblock copolymers appear to reinforce the c
raze fibrils at the crack tip better than the corresponding diblock co
polymers, leading to an interface fracture toughness approaching that
of the PS homopolymer itself. For a triblock copolymer with short PVP
blocks (N-PVP < N-ePVP), there is a transition in the fracture mechani
sm from pull out of the PVP block to crazing with increasing Sigma. Sh
ort triblock copolymers can form two chain conformations: one in which
two PVP blocks anchor the copolymer on the homopolymer PVP side (stap
le structure) and one in which one PVP block anchors the copolymer on
the PVP side (tail structure) of the interface. Comparison of G(c) bet
ween the triblock copolymer and the corresponding diblock copolymer is
made. The larger G(c) values of the triblock copolymer reinforced int
erface in the crazing regime are observed as a result of enhancement i
n entanglements between the dPS loops of the triblock copolymer and th
e homopolymer PS.