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Partially miscible and immiscible blends

For partially miscible and immiscible blends, various domain/phase structures can be invoked. Unfortunately, the resonance position of a particular spin in each domain is not appreciably affected by its respective domain structure (see Section 10.2.2.1). Therefore, we cannot expect to observe highly resolved NMR resonances for different domains. Since relaxation times are different for each domain, a relaxation curve is observed to be a featureless multiexponential one and, in most of the cases, is too monotonous to include interdomain spin diffusion. Therefore, most of the experimental results have been explained by using the simplified picture of no interdomain spin diffusion and the observed multiexponential decay is fitted to a sum of exponential functions. Practically three exponentials are enough to realize the observed decay. Each relaxation time represents one domain, thus, only a few domains can be distinguished by one resonance line. Inevitably, the heterogeneous structures deduced from NMR relaxation experiments become simple. [Pg.387]


See other pages where Partially miscible and immiscible blends is mentioned: [Pg.387]    [Pg.187]    [Pg.30]   
See also in sourсe #XX -- [ Pg.2 , Pg.38 , Pg.377 ]




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And miscibility

Blends miscibility

Blends miscible and immiscible

Immiscibility

Immiscibility Immiscible

Immiscible

Immiscible and miscible

Immiscible blend

Miscibility, partial

Miscible blends

Partially miscible blends

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