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. 2018 Mar 5;115(12):2936–2941. doi: 10.1073/pnas.1714795115

Fig. 4.

Fig. 4.

Comparison of the theoretical predictions to experimental data. (A) Surface area S of nasal cavities as a function of body mass M. Shown are experimentally measured respiratory turbinal surface areas in canid and arctoid carnivorans (18) (blue dots) and in humans (orange cross; bars indicate standard deviation; parameters in Table 2). Our predictions (green lines) follow from the optimal gap width of parallel plates given in Eq. 7 (dark green) and a numerical solution based on a rectangular geometry (light green; dashed part indicates square geometry). Here, we assumed E=1 and used the scalings given in Table 1. (Inset) The associated volumes V of the nasal cavities as a function of M together with the scaling given in Table 1. (B) Local gap width, given by the shape diameter function (24), for the standardized nasal cavity (23). (C) Hydraulic radius Rh along the main axis z of the standardized cavity (23) (blue line) compared with the predicted given by Eq. 7 (green line), which was calculated for E=1 and the parameters given in Table 2. (Inset) The cross-sectional area A of the standardized cavity as a function of z.