We consider the system of a network formed by crosslinking a polymer b
lend. In such a system there is a competition between monomer-monomer
interactions and elastic energy which may result in a microphase separ
ation. We first treat the problem by adapting a model due to de Gennes
to include the effect of concentration fluctuations 'frozen in' by th
e crosslinking process. This yields an expression for the scattering s
tructure factor which gives finite scattering in the limit of low wave
number (this has been observed in experiments on crosslinked blends).
The expression also shows that the frozen-in fluctuations 'seed' the p
hase transition, so that the structure factor diverges as (chi(s) - ch
i)(-2) on approaching the spinodal. We then reconsider the problem at
a molecular level. We model the network as a blend of interacting chai
ns anchored at either end to fixed points in space. The system is trea
ted using a variant of the Random Phase Approximation (RPA) which deal
s with the quenched chain-end variables but which does not resort to r
eplica methods. The resulting structure factor has an identical form t
o that obtained by modifying the de Gennes model, but allows us to inv
estigate the effect of varying composition, crosslink density, and app
lied strain. We find that the characteristic lengthscale for the early
stages of microphase separation is controlled by the least concentrat
ed component or the one with the shortest chain length between crossli
nks, depending on which parameter shows the strongest difference betwe
en the two chain types. We also find that strain produces a phase sepa
ration with wavevectors in the direction(s) of least stretching (or gr
eatest compression).