Several recent experiments investigate the orientational and transport behavior of self-driven bacteria and colloidal particles in nematic liquid crystals. Correspondingly, we study theoretically the dynamics of a minimal model microswimmer in a uniaxially anisotropic fluid. As a first step, the hydrodynamic Green's function providing the resulting fluid flow in response to a localized force acting on the anisotropic fluid is derived analytically. On this basis, the behavior of both puller-and pusher-type microswimmers in the anisotropic fluid is analyzed. Depending on the propulsion mechanism and the relative magnitude of different involved viscosities, we find alignment of the swimmers parallel or perpendicular to the anisotropy axis. Particularly, also an oblique alignment is identified under certain circumstances. The observed swimmer reorientation results from the hydrodynamic coupling between the self-induced fluid flow and the anisotropy of the surrounding fluid, which distorts the self-generated flow field. We support parts of our results by a simplified linear stability analysis. Our theoretical predictions are in qualitative agreement with recent experimental observations on swimming bacteria in nematic liquid crystals. They support the objective of utilizing the, possibly switchable, anisotropy of a host fluid to guide individual microswimmers and active particles along a requested path, enabling controlled active transport.
I. INTRODUCTIONActive particles have the ability to move autonomously in a surrounding fluid by converting energy into directed motion. Artificial self-propelled nano-and microscale machines hold great promise for future medical research to reach otherwise inaccessible areas of the body to perform delicate and precise tasks. Prospective biomedical applications are precision nanosurgery, biopsy, and transport of radioactive substances to tumor areas and inflammation sites 1-3 . Over the last few decades, significant research efforts have been devoted to investigate the behavior of self-propelling active particles due to their importance and relevance as model systems for transport and locomotion in the micro-and nano-scale world; for recent reviews see Refs. 4-12. Unusual macroscopic signatures and intriguing spatiotemporal patterns emerge from the interaction between several active particles. For instance, the onset of collective motion 13-19 , formation of dynamic clusters 20-26 , wave patterns 27-30 , laning 31-35 , motility-induced phase separation 36-41 , swarming 42-44 , and active turbulence 45-52 are observed. In many cases, artificial self-driven particles and swimming microorganisms have to propel through complex fluids, such as polymer gels and viscoelastic microemulsions [53][54][55][56][57][58][59][60][61][62][63] . Notable examples include sperm navigation through the mammalian female reproductive tract 64,65 , bacteria locomotion in biofilm matrices composed of extracellular polymeric substances 66,67 , nematode movement in soil 68,69 , and the motion of synthetic mic...