We report on the observed characteristics of the first-order phase transition of F-actin from the isotropic state to the nematic liquid-crystalline state. Solutions of short average filament length F-actin at appropriate concentrations phase separate to form tactoidal droplets. These tactoids are the result of the minimization of their free energy and show a bipolar director field connecting two opposite poles. The tactoids are shown to form through two distinct mechanisms: nucleation and growth and spinodal decomposition. Both mechanisms produce tactoids with final domain sizes that are of the same order of magnitude. Additionally, analysis of the system shows several features of metastability. The solution can exist in a variety of steady states near equilibrium and can be easily perturbed, settling in one prescribed by the path followed in phase space.

The phase transition from the isotropic ͑I͒ to nematic ͑N͒ liquid crystalline suspension of F-actin of average length łу3 m was studied by local measurements of optical birefringence and protein concentration. Both parameters were detected to be continuous in the transition region, suggesting that the I-N transition is higher than first order. Thus we report experimental evidence for a continuous I-N transition for a suspension of rodlike macromolecules. Our findings are consistent with a recent theory by Lammert, Rokhsar, and Toner ͓Phys. Rev. Lett. 70, 1650 ͑1993͔͒, predicting that the I-N transition may become continuous due to suppression of disclinations.

We report that the properties of the isotropic to nematic liquid crystalline phase transition of F-actin depend critically on the average filament length. For average filament lengths longer than 2 microm, we confirm previous findings that the phase transition is continuous in both alignment and concentration. For average filament lengths shorter than 2 microm, we show for the first time a first order transition with a clear discontinuity in both alignment and concentration. Tactoidal droplets of coexisting isotropic and nematic phases, differing in concentration by approximately 30%, form over the course of hours and appear to settle into near equilibrium metastable states.