We present a simple mathematical model based on classical theories of
macroscopic elasticity that provides a fundamental description of the
liquid crystal polymer (LCP) fiber break-up instability that is observ
ed during the annealing of in-situ liquid crystal-thermoplastic polyme
r composites. The thermodynamic model is solved using a number of cons
istent simplifying assumptions, and is restricted to thin liquid cryst
al polymer fibers. A significant feature of the liquid crystal surface
energy incorporated in the model is the elastic storage due to deviat
ions of the macroscopic orientation and of the orientational order fro
m the preferred equilibrium values. The model predicts that thin LCP f
ibers are unstable to periodic surface perturbations that eventually w
ould produce fiber break-up and lead to an array of LCP droplets, as i
n the case of Rayleigh's fiber instability. The additional liquid crys
talline elastic storage modes incorporated in the model, but not prese
nt in isotropic melts, tend to increase the magnitude of the critical
wave-length for fiber break-up over that given by the Rayleigh criteri
a (i.e., fiber circumference) by a relatively small factor that depend
s on the ratio of the interfacial tension and the nematic anchoring en
ergy.