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Outline of a representative shortfin mako shark Isurus oxyrinchus showing the 16 regions sampled for scale photography, angle measurement, and histology. The mean erection angle for five scales in each region is given beside the nomenclature for each region. Flank scales (B2, B5, A2) are capable of greater erection angles than dorsal (B1, B4, A1) and ventral (B3, B6, A3) regions. All regions on the pectoral fin (P 1, P 2, P 3) differed in the degree of erection possible with the leading edge scales (P 1) incapable of erection. Erection angle did not differ among the three regions on the caudal fin (C1, C2, C3). 

Outline of a representative shortfin mako shark Isurus oxyrinchus showing the 16 regions sampled for scale photography, angle measurement, and histology. The mean erection angle for five scales in each region is given beside the nomenclature for each region. Flank scales (B2, B5, A2) are capable of greater erection angles than dorsal (B1, B4, A1) and ventral (B3, B6, A3) regions. All regions on the pectoral fin (P 1, P 2, P 3) differed in the degree of erection possible with the leading edge scales (P 1) incapable of erection. Erection angle did not differ among the three regions on the caudal fin (C1, C2, C3). 

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An investigation into the separation control mechanisms found on the skin of fast-swimming sharks, with a particular focus on the shortfin mako (Isurus oxyrinchus) which is considered to be one of the fastest pelagic shark species, was carried out. Previous researchers have reported a bristling capability of the scales, or denticles, in certain spe...

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... The other more popular perspective indicates that the vortices (they are called boundary vortices in this paper) within transverse grooves change the sliding friction into the rolling friction at the solid-liquid interface, which is also named the "micro air-bearing phenomenon" [9][10][11][12][13][14][15]. In addition, the studies of Mariotti et al. [16,17], Pasqualetto et al. [18], Howard et al. [19], and Lang et al. [3,20] showed that the vortices formed in the transverse grooves (and small cavities) increase the momentum in the boundary layer near the wall, thus effectively controlling the flow separation. However, none of the qualitative descriptions of the drag-reduction is qualitatively analyzed to prove that it is also a necessary condition for obtaining the optimal drag-reduction rate. ...
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The Shortfin Mako shark (Isurus oxyrinchus) is a fast swimmer and has incredible turning agility, and has flexible scales known to bristle up to 50° in the flank regions. It is purported that this bristling capability of the scales may result in a unique pass flow control method to control flow separation and reduce drag. It appears that the scales have evolved to be only actuated when the flow over the body is reversed; thereby inducing a method of inhibiting flow reversal close to the surface. In addition, bristled scales form cavities which could induce boundary layer mixing and further assist in delaying flow separation. To substantiate the hypothesis, samples of skin from the flank region of the mako have been tested in a water tunnel facility under various strengths of adverse pressure gradient (APG). Laminar and turbulent separation over the skin was studied experimentally using time-resolved digital particle image velocimetry, where the APG was generated and varied using a rotating cylinder. Shark skin results were compared with that of a smooth plate data for a given amount of APG. Both the instantaneous and time-averaged results reveal that shark skin is capable of controlling laminar as well as turbulent separation. Under laminar conditions, the shark skin also induces an early transition to turbulence and reduces the degree of laminar separation. For turbulent separation, the presence of the shark skin reduces the amount of backflow and size of the separation region. Under both flow conditions, the shark skin also delayed the point of separation as compared to a smooth wall.