2000
DOI: 10.1016/s0032-3861(00)00057-4
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Ternary polymer blend with core–shell dispersed phases: effect of the core-forming polymer on phase morphology and mechanical properties

Abstract: Phase morphology and mechanical properties of ternary blends consisting of PS (polystyrene), SBR (styrene butadiene rubber) and different polyolefins (POs) have been studied. PS, systematically forms the matrix, SBR and PO being combined in the dispersed phase. Although POs of various melt viscosity and stiffness are used, the binary (SBR/PO) dispersed phase is of a core-shell structure, in which PO forms the core. Upon increasing the viscosity of PO, the average size of the cores and the SBR domains including… Show more

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Cited by 74 publications
(50 citation statements)
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“…However, in some cases, the “multicore structure,” i.e., several subinclusions of one minor phase are embedded in a larger particle of the second minor phase morphology cannot be successfully predicted by employing the spreading coefficient theory. Also, the morphology of subinclusions formation is related to various factors such as viscosity ratio, elastic effect, composition ratio effect, interfacial reaction, etc. Luzinov et al investigated the morphologies of ternary polystyrene/styrene–butadiene rubber/polyethylene (PS/SBR/PE) blends with a constant content of the major component (PS: 75 wt %), and found that according to the predication of spreading coefficients theory, the PE/SBR core–shell structure should be formed.…”
Section: Introductionmentioning
confidence: 99%
“…However, in some cases, the “multicore structure,” i.e., several subinclusions of one minor phase are embedded in a larger particle of the second minor phase morphology cannot be successfully predicted by employing the spreading coefficient theory. Also, the morphology of subinclusions formation is related to various factors such as viscosity ratio, elastic effect, composition ratio effect, interfacial reaction, etc. Luzinov et al investigated the morphologies of ternary polystyrene/styrene–butadiene rubber/polyethylene (PS/SBR/PE) blends with a constant content of the major component (PS: 75 wt %), and found that according to the predication of spreading coefficients theory, the PE/SBR core–shell structure should be formed.…”
Section: Introductionmentioning
confidence: 99%
“…Obviously, the degree of success to achieve such polymer blends with prescribed properties is strongly influenced by their interfacial interaction. Therefore understanding the role of parameters which control the morphology development of the blends has become important issue for both academic researchers and manufacturers [1][2][3][4][5][6][7][8][9][10].…”
Section: Introductionmentioning
confidence: 99%
“…In both polypropylene (PP)/ polyamide‐6 (PA‐6) binary and PP/PA‐6/Poly(styrene‐b‐(ethylene‐ co ‐butylene)‐b‐styrene) (SEBS) ternary systems, using maleated SEBS (SEBS‐ g ‐MAH) as a compatibilizer, strongly influenced the blend morphology and mechanical properties by variation in the degree of interfacial reaction between the succinc anhydride groups of the SEBS‐ g ‐MAH and the terminal amino groups of PA6 2–4. Recently, the study of ternary blends has raised the attention of researches cause of wide range of variation in mechanical and morphological properties in these systems 5–17. It is observed that for the systems containing two minor phases, three distinct types of phase morphology have to be specified.…”
Section: Introductionmentioning
confidence: 99%
“…For some ternary systems, one of the minor components formed an encapsulating layer around domains of another minor component, whereas in other systems, two minor components formed independent phases separately. The third type is the intermediate case, where mixed phases of the two components are formed without any ordered structures 5–11. To predict the tendency for one minor phase to encapsulate a second one, the alternative form of Harkin's equation have been used as follows: where γ AC , γ AB , and γ BC are the interfacial tension for each component pair, and λ BC is defined as the spreading coefficient for the shell forming component B on the core of component C. The index A corresponds to the matrix continuous phase.…”
Section: Introductionmentioning
confidence: 99%
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