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    Temperature dependence of droplet breakup in 8CB and 5CB liquid crystals

    Daniel Porter*, John R. Savage, and Itai Cohen

    Patrick Spicer and Marco Caggioni

    • Department of Physics, Cornell University, Ithaca, New York 14853, USA

    • Complex Fluid Microstructures, Procter & Gamble, West Chester, Ohio 45069, USA

    • *dgp57@cornell.edu

    Phys. Rev. E 85, 041701 – Published 6 April, 2012

    DOI: https://doi.org/10.1103/PhysRevE.85.041701

    Abstract

    Droplet breakup of many Newtonian fluids is well described by current experiments, theory, and simulations. Breakup in complex fluids where interactions between mesoscopic structural features can affect the flows remains poorly understood and a burgeoning area of research. Here, we report on our investigations of droplet breakup in thermotropic liquid crystals. We investigate breakup in the smectic, nematic, and isotropic phases of 4-cyano 4-octylbiphenyl (8CB) and the nematic and isotropic phases of 4-cyano 4-pentylbiphenyl (5CB). The experiment consists of varying the ambient temperature to control liquid crystalline phase and imaging breakup using a fast video camera at up to 110000 frames/s. We expand on previous work [John R. Savage et al., Soft Matter 6, 892 (2010)] that shows breakup in the smectic phase is symmetric, producing no satellite droplets, and is well described by a similarity solution for a shear-thinning power-law fluid. We show that in the nematic phase the breakup occurs in two stages. In the first stage, the breakup is symmetric and the power-law exponent for the minimum radius dependence on the time left to breakup is 1.2<n<1.9. In the second stage the drop develops two minima and the minimum radii shrink with a power-law exponent 0.6<n<1. We find that the exponents vary with temperature across the nematic phase. These results are surprising because rheological measurements of 8CB and 5CB in the nematic phases indicate Newtonian behavior that cannot account for the observed breakup dynamics. Finally, in the isotropic phase, the exponents are consistent with theoretical predictions and experiments for Newtonian fluid breakup in the inertial viscous regime.

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