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. Author manuscript; available in PMC: 2009 Sep 8.
Published in final edited form as: J Fluid Mech. 2005 Dec 5;564:433–443. doi: 10.1017/S0022112005006865

Figure 8.

Figure 8

Consecutive images (Δt = 0.43 s) at plane (l) of figure 6 yielding a streamwise interpolation of figure 6. The weak distant legs of horseshoe 2 are initially entrained by the stronger vortices of horseshoe 3 (images ae). Further upstream (images fi), horseshoe 4 dominates the interaction, entraining horseshoe 2 and entraining horseshoe 3. Asymmetry results in a stronger interaction between horseshoes 2 and 3 at the top of the wake, and between horseshoes 2 and 4 at the bottom.