Using off-lattice Monte Carlo simulations, the critical value of the Flory-Huggins parameter, v, for flexible-semiflexible (isotropic-isotropic) polymer systems as a function of the stiffness of the semiflexible components was estimated. The simulation data were compared with those of the mean field, and it was found that both agree very well. The interfacial tension and the width of the flexible-semiflexible polymer systems were also studied for strong and weak segregation limits. Polymer Journal (2011) 43, 751-756; doi:10.1038/pj.2011; published online 20 July 2011Keywords: isotropic-isotropic polymer; phase separation; semiflexible polymers; stiffness disparity INTRODUCTION Different kinds of polymers can be mixed into a single material in different ways, which can lead to a wide range of phase behaviors that directly influence the associated physical properties and applications of polymers. Two different polymers generally do not mix well. The factors that control polymer-polymer phase behavior are the choice of monomers, molecular architecture, composition, molecular size, interaction energies, specific interactions and the 'Equation of state effects' . The study of the structure, phase behavior and interfacial properties of polymers has found longstanding and widespread interest. 1-10 Understanding the phase behavior of mixtures of different kinds of polymers is important scientifically 11 as well as practically. The scientific importance arises from the complex behavior polymer mixtures display, and the practical importance arises from the many industrial applications of these materials. Polymer blends are generally structurally asymmetric, corresponding to species-dependent local intramolecular properties, such as monomer shape, branch content, and persistence length. Such asymmetries are expected to have a major impact on blend thermodynamics and phase diagrams and can give rise to non-Flory-Huggins miscibility behavior. The prediction of the phase behavior of semiflexible polymeric materials is an important step toward the full characterization of the structural and dynamic properties of liquid-crystalline polymeric materials. In polymer blends, it is important to know how the locations of various phases, isotropic and nematic, and their transitions depend on the properties of the two components, their rigidities, polymerization indices, interactions and so on.Differences in chemical structure may also lead to different spatial configurations of the chemical repeat units, corresponding to different persistence lengths, that is, stiffness disparities. 4 Such stiffness disparities may occur even in materials that are chemically very similar, for example, different polyolefins. Liu and Fredrickson 12 have calculated a