Flow patterns generated by oblate medusan jellyfish: field measurements and laboratory analyses

SUMMARY Flow patterns generated by medusan swimmers such as jellyfish are known to differ according the morphology of the various animal species. Oblate medusae have been previously observed to generate vortex ring structures during the propulsive cycle. Owing to the inherent physical coupling between locomotor and feeding structures in these animals, the dynamics of vortex ring formation must be robustly tuned to facilitate effective functioning of both systems. To understand how this is achieved, we employed dye visualization techniques on scyphomedusae (Aurelia aurita) observed swimming in their natural marine habitat. The flow created during each propulsive cycle consists of a toroidal starting vortex formed during the power swimming stroke, followed by a stopping vortex of opposite rotational sense generated during the recovery stroke. These two vortices merge in a laterally oriented vortex superstructure that induces flow both toward the subumbrellar feeding surfaces and downstream. The lateral vortex motif discovered here appears to be critical to the dual function of the medusa bell as a flow source for feeding and propulsion. Furthermore, vortices in the animal wake have a greater volume and closer spacing than predicted by prevailing models of medusan swimming. These effects are shown to be advantageous for feeding and swimming performance, and are an important consequence of vortex interactions that have been previously neglected.

[1]  Sean P Colin,et al.  Morphology, swimming performance and propulsive mode of six co-occurring hydromedusae. , 2002, The Journal of experimental biology.

[2]  N. Didden On the formation of vortex rings: Rolling-up and production of circulation , 1979 .

[3]  John H. Costello,et al.  In situ time budgets of the scyphomedusae Aurelia aurita, Cyanea sp., and Chrysaora quinquecirrha , 1998 .

[4]  Brian J. Cantwell,et al.  Viscous starting jets , 1986, Journal of Fluid Mechanics.

[5]  Jeremy M. V. Rayner,et al.  On the Vortex Wake of an Animal Flying in a Confined Volume , 1991 .

[6]  M. McHenry,et al.  The ontogenetic scaling of hydrodynamics and swimming performance in jellyfish (Aurelia aurita) , 2003, Journal of Experimental Biology.

[7]  B. K. Sullivan,et al.  Prey selection by the scyphomedusan predator Aurelia aurita , 1994 .

[8]  John H. Costello,et al.  Swimming and feeding by the scyphomedusa Chrysaora quinquecirrha , 1997 .

[9]  S. Vogel,et al.  Life in Moving Fluids , 2020 .

[10]  Morteza Gharib,et al.  Sensitivity analysis of kinematic approximations in dynamic medusan swimming models , 2003, Journal of Experimental Biology.

[11]  John O. Dabiri,et al.  Vortex ring pinchoff in the presence of simultaneously initiated uniform background co-flow , 2003 .

[12]  John O. Dabiri,et al.  Fluid entrainment by isolated vortex rings , 2004, Journal of Fluid Mechanics.

[13]  C. Willert,et al.  Digital particle image velocimetry , 1991 .

[14]  M. Gharib,et al.  A universal time scale for vortex ring formation , 1998, Journal of Fluid Mechanics.

[15]  T. Daniel Mechanics and energetics of medusan jet propulsion , 1983 .

[16]  R. Wood,et al.  Vortex Rings , 1901, Nature.

[17]  J. Costello,et al.  Flow and feeding by swimming scyphomedusae , 1995 .

[18]  W. Gladfelter A comparative analysis of the locomotory systems of medusoid Cnidaria , 1973, Helgoländer wissenschaftliche Meeresuntersuchungen.

[19]  H. J.,et al.  Hydrodynamics , 1924, Nature.

[20]  John H. Costello,et al.  Morphology, fluid motion and predation by the scyphomedusa Aurelia aurita , 1994 .

[21]  John O. Dabiri,et al.  Starting flow through nozzles with temporally variable exit diameter , 2005, Journal of Fluid Mechanics.

[22]  Paul S. Krueger,et al.  The significance of vortex ring formation to the impulse and thrust of a starting jet , 2003 .