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Because there is no material in the way of the beam, it can pass through unobstructed, thus making these regions appear to be very light. Holes around the captured micro-phase can also be observed where the action of sectioning has literally pushed such a region out of its position within the matrix. The removed pieces can often be seen next to the hole, in some cases still attached to some point on the interface. Weak interfacial adhesion within NR/NBR blends has been an important theme running throughout this work: results like these have been vital to the work performed in this field (Chapters 5 to 8).

7(3) 168. M. L. (1986). Solid state carbon-13 NMR studies of vulcanized elastomers. II. Sulfur vulcanization of natural rubber. Rubber Chemistry and Technology, 60(2), 252-277.

J. and Rehner, J. (1943) Statistical mechanics of cross-linked polymer networks. II Swelling. Journal of Chemical Physics, 11(11), 521-526. J. (1950) Statistical mechanics of swelling of network structures. Journal of Chemical Physics, 18(1), 108-11I. 5. J. (1990) Crosslink distribution in vulcanised blends of NR and EPDM. Journal of Natural Rubber Research, 5(3), 157-157. 5. I. (1990) Estimation of the extent of crosslinking in the phases of vulcanized rubber blends by CW-1H NMR spectroscopy. 3.

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