FRACTURE-TOUGHNESS OF POLYMER INTERFACE REINFORCED WITH DIBLOCK COPOLYMER - EFFECT OF HOMOPOLYMER MOLECULAR-WEIGHT

Citation
Ca. Dai et al., FRACTURE-TOUGHNESS OF POLYMER INTERFACE REINFORCED WITH DIBLOCK COPOLYMER - EFFECT OF HOMOPOLYMER MOLECULAR-WEIGHT, Macromolecules, 29(23), 1996, pp. 7536-7543
Citations number
24
Categorie Soggetti
Polymer Sciences
Journal title
ISSN journal
00249297
Volume
29
Issue
23
Year of publication
1996
Pages
7536 - 7543
Database
ISI
SICI code
0024-9297(1996)29:23<7536:FOPIRW>2.0.ZU;2-J
Abstract
We have measured the fracture toughness, G(c), of an immiscible polyme r/polymer [polystyrene (PS) and poly(2-vinylpyridine) (PVP)] interface reinforced with deuterium-labeled dPS-b-PVP diblock copolymers as a f unction of the number average molecular weight, <(M)over bar (n)>, of the polystyrene homopolymer, either monodisperse homopolymer PS (MPS) or polydisperse homopolymer PS (PPS). The dependence of G(c) on the PS molecular weight was investigated at different areal chain densities, Sigma of the copolymers. These values of Sigma were chosen to be in e ither one of two fracture mechanism regimes: chain scission or crazing . In the chain scission regime, G(c) is independent of the molecular w eight of MPS and PPS. In contrast in the crazing regime (for Sigma les s than or equal to Sigma(sat), where Sigma(sat) is the saturation Sigm a for the copolymer at the interface), <(M)over bar (n)> of MPS has a strong effect on the fracture toughness. For this case, G(c) increases sharply around <(M)over bar (n)> x 100 000 and then levels off at hig her <(M)over bar (n)> values. The polydisperse PS/PVP interface has a fracture toughness consistent with its <(M)over bar (n)> rather than i ts weight-average molecular weight, <(M)over bar (w)>. When the interf ace is covered with copolymer lamellae (Sigma much greater than Sigma( sat)), G(c) is found to be independent of <(M)over bar (n)>, of the MP S and is substantially larger than that for the PPS/PVP interface at t he same Sigma. For the PPS/PVP interface, the low molecular weight por tion of PPS swells the lamellar structure, resulting in a decrease in G(c) compared to that of the MPS/PVP interface. We have also measured G(c) as a function of composition of a blend of high and low <(M)over bar (n)> MPS, where <(M)over bar (n)> of the low molecular weight PS i s below the entanglement molecular weight of PS. Dilution of the entan glement density of the homopolymer polystyrene results in a strong dec rease in G(c). Our results are compared with recent models for craze f ailure. A continuum craze model using the full stress field proposed b y Sha et al.(20) predicts the fracture toughness better than models(2, 9) using the asymptotic stress field.