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. 2010 May 24;50(6):1140–1154. doi: 10.1093/icb/icq057

Table 1.

Swimming performance from computational results as a function of body shape, swimming mode, and Re

Re0 = 300, St0= 1.1 f0 = 5.5 Re = 4000, St0 = 0.6 f0 = 3 Re = ∞, St0 = 0.3 f0 = 1.5
M L M L M L
Stact
    C 1.10 (2) 1.72 (4) 0.61 (2) 0.71 (4) 0.25 (1) 0.41 (3)
    A 0.99 (1) 1.39 (3) 0.59 (1) 0.67 (3) 0.33 (2) 0.47 (4)
U*
    C 1.00 (3) 0.64 (1) 0.98 (3) 0.84 (1) 1.20 (4) 0.74 (2)
    A 1.11 (4) 0.79 (2) 1.01 (4) 0.90 (2) 0.92 (3) 0.64 (1)
URMS
    C 1.4 × 102 (4) 0.5 × 10−2 (2) 6.8 × 103 (4) 1.7 × 10−3 (2) 3.8 × 103 (4) 0.6 × 10−3 (2)
    A 1.3 × 10−2 (3) 0.2 × 102 (1) 4.4 × 10−3 (3) 0.6 × 103 (1) 2.2 × 10−3 (3) 0.4 × 103 (1)
CP,tot
    C 0.95 (2) 3.61 (4) 0.10 (2) 0.14 (4) 3.7 × 10−3 (2) 4.2 × 103 (4)
    A 0.73 (1) 2.26 (3) 0.08 (1) 0.11 (3) 3.5 × 103 (1) 3.9 × 10−3 (3)
CP,wake
    C 0.77 (2) 3.15 (4) 0.076 (3) 0.103 (4) 2.0 × 103 (1) 3.3 × 103(4)
    A 0.56 (1) 1.87 (3) 0.059 (1) 0.074 (2) 2.2 × 10−3 (2) 3.2 × 10−3 (3)
η
    C 0.19 (3) 0.13 (1) 0.22 (1) 0.26 (3) 0.45 (4) 0.194 (2)
    A 0.23 (4) 0.17 (2) 0.26 (2) 0.32 (4) 0.38 (3) 0.189 (1)

Values of each variable are shown as a 2 × 2 matrix of body shape and swimming mode. Numbers in parentheses indicate the rank of the value, from one (lowest) to four (highest). Lowest values are shown in italics; highest in bold. Stact, actual Strouhal number; U*, swimming speed; URMS, root-mean-square fluctuation in steady swimming speed; CP,wake, wake power coefficient; CP,tot, total propulsive power; η, Froude propulsive efficiency; M, mackerel body shape; L, lamprey body shape; C, carangiform swimming mode; A, anguilliform swimming mode. Modified from Borazjani and Sotiropoulos (2010); note that the power coefficients are normalized differently.