EFFECT OF END-ANCHORED CHAINS ON THE ADHESION AT A THERMOSET-THERMOPLASTIC INTERFACE

Citation
Lj. Norton et al., EFFECT OF END-ANCHORED CHAINS ON THE ADHESION AT A THERMOSET-THERMOPLASTIC INTERFACE, Macromolecules, 28(6), 1995, pp. 1999-2008
Citations number
32
Categorie Soggetti
Polymer Sciences
Journal title
ISSN journal
00249297
Volume
28
Issue
6
Year of publication
1995
Pages
1999 - 2008
Database
ISI
SICI code
0024-9297(1995)28:6<1999:EOECOT>2.0.ZU;2-W
Abstract
The asymmetric double cantilever beam fracture test was used to measur e the critical energy release rate, or fracture toughness, G(c), of an epoxy-polystyrene (PS) interface as a function of the grafting densit y, Sigma, and degree of polymerization, N, of carboxylic acid terminat ed deuterated polystyrene chains (dPS-COOH). The chain ends anchor to the epoxy, and their tails penetrate into the PS homopolymer. Forward recoil spectrometry (FRES) on the fracture surfaces provided a method to determine the total Sigma as well as the mechanism of interface fai lure. For N = 159 the grafted chains were too short to entangle and pu ll out of the PS, leading to no enhancement in G(c) over that of a bar e interface. When the chain length was increased to N = 412 and 535, t here was sufficient stress transfer to initiate crazes in the PS that break down by either disentanglement or scission of dPS-COOH chains in the craze fibrils. For long, well-entangled chains of N = 688, 838, a nd 1478 the chains broke near the epoxy-PS interface at low Sigma befo re significant crazing of the PS occurs. A transition from chain sciss ion to crazing occurred at Sigma(c) = 0.03 chains/nm(2) for all three chain lengths, agreeing with experiments on diblock copolymer modified thermoplastic-thermoplastic interfaces' and with the prediction from the fracture mechanism map(2) that the transition is independent of ch ain length. We observed a nearly linear decrease in the maximum achiev able Sigma as N increased that can be explained in part by an entropic barrier that opposes the addition of new chains to the grafted brush. The toughest interfaces occurred with intermediate length grafted cha ins, N = 838, when the chains were well entangled and the grafted brus h was dense enough, Sigma > Sigma(c), to cause energy dissipation thro ugh craze formation.