Figure 1. The water strider is an insect of characteristic length 1cm and weight 10 dynes that resides on the surface of ponds, rivers, lakes and the open ocean. Its weight is supported by the surface tension force generated by curvature of the free surface. Its body and legs are covered by thousands of hairs that render its legs effectively non-wetting (Andersen 1982).
The water strider propels itself by driving its central pair of legs ina sculling motion. In order for it to move, it must transfer momentum to the underlying fluid. It was previously assumed that this transfer occurs exclusively through capillary waves excited by the leg stroke (Denny 1993). Our experiments reveal that, conversely, the strider transfers momentum to the fluid principally through dipolar vortices shed by its driving legs. The strider thus generates thrust by rowing, using its legs as oars, and the meniscii beneath its driving legs as blades.
Fig 2
Figures 2 and 3. A water layer was sprinkled with Thymol Blue, which established
the Marangoni convection responsible for the evident fine-scale texture. The layer was lit from below, giving the flow a natural luminescence. Stopping
vortices shed during the deceleration phase of the strider's motion are evident in
Figure 2. The dipolar vortices shed by the driving legs during each stroke are evident in
Figure 3, and mark the path of the strider. The starburst in Figure 3 is associated with the relatively large particle
of thymol blue evident at its centre: the Thymol Blue reduces the local surface
tension, thus prompting surface divergence that clears the surface of blue dye.The water striders are light-seeking, and so drawn to the starbursts.
References
Andersen, N.M, 1982. The Semiaquatic Bugs. Scandinavian Science Press,
Klapenborg, Denmark.
Denny, M.W., 1993. Air and Water: The Biology and Physics of Life's Media,
Princeton University Press.
.
[Home] - [Research Interests] - [Plume Dynamics]