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The function(s) of bone ornamentation in the crocodylomorph osteoderms: a biomechanical model based on a finite element analysis

Published online by Cambridge University Press:  27 February 2019

François Clarac
Affiliation:
Sorbonne Université, Centre National de la Recherche Scientifique, Institut des Sciences de la Terre de Paris, UMR 7193, 4 place Jussieu, BC 19-75005 Paris, France; and Département Histoire de la Terre, UMR 7207, Centre de Recherche en Paléontologie–Paris, Muséum National d'Histoire Naturelle/Centre National de la Recherche Scientifique /Sorbonne Université, Bâtiment de Géologie Paris Cedex 05, F-75231, France. E-mail: francois.clarac@mnhn.fr.
Florent Goussard
Affiliation:
Département Histoire de la Terre, UMR 7207, Centre de Recherche en Paléontologie–Paris, Muséum National d'Histoire Naturelle/Centre National de la Recherche Scientifique/ Sorbonne Université, Bâtiment de Paléontologie Paris Cedex 05, F-75231, France. E-mail: florent.goussard@mnhn.fr
Vivian de Buffrénil
Affiliation:
Département Histoire de la Terre, UMR 7207, Centre de Recherche en Paléontologie–Paris, Muséum National d'Histoire Naturelle/Centre National de la Recherche Scientifique/Sorbonne Université, Bâtiment de Géologie Paris Cedex 05, F-75231, France. E-mail: vivian.de-buffrenil@mnhn.fr
Vittorio Sansalone
Affiliation:
Université Paris-Est, Laboratoire Modélisation et Simulation Multi Echelle, MSME UMR 8208 CNRS, 61 avenue du Général de Gaulle, 94010 Créteil Cedex, France. E-mail: vittorio.sansalone@u-pec.fr

Abstract

This paper aims at assessing the influence of the bone ornamentation and, specifically, the associated loss of bone mass on the mechanical response of the crocodylomorph osteoderms. To this end, we have performed three-dimensional (3D) modeling and a finite element analysis on a sample that includes both extant dry bones and well-preserved fossils tracing back to the Late Triassic. We simulated an external attack under various angles on the apical surface of each osteoderm and further repeated the simulation on an equivalent set of smoothed 3D-modeled osteoderms. The comparative results indicated that the presence of an apical sculpture has no significant influence on the von Mises stress distribution in the osteoderm volume, although it produces a slight increase in its numerical score. Moreover, performing parametric analyses, we showed that the Young's modulus of the osteoderm, which may vary depending on the bone porosity, the collagen fiber orientation, or the calcification density, has no impact on the von Mises stress distribution inside the osteoderm volume. As the crocodylomorph bone ornamentation is continuously remodeled by pit resorption and secondary bone deposition, we assume that the apical sculpture may be the outcome of a trade-off between the bone mechanical resistance and the involvement in physiological functions. These physiological functions are indeed based on the setup of a bone superficial vessel network and/or the recurrent release of mineral elements into the plasma: heat transfers during basking and respiratory acidosis buffering during prolonged apnea in neosuchians and teleosaurids; compensatory homeostasis in response to general calcium deficiencies. On a general morphological basis, the osteoderm geometric variability within our sample leads us to assess that the global osteoderm geometry (whether square or rectangular) does not influence the von Mises stress, whereas the presence of a dorsal keel would somewhat reduce the stress along the vertical axis.

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Copyright © 2019 The Paleontological Society. All rights reserved 
Figure 0

Table 1. Sampled specimens with taxonomic references.

Figure 1

Table 2. Sampled osteoderms with morphometric data. The ΔMass is calculated assuming a bone density of 2g/cm3. *Estimated scale factor based on the osteoderm real size (different from the value used for scaling the 3D model in Geomagic Studio). Osteolaemus tetraspis (a),MNHN-AC.1991.4488a; (b), MNHN-AC.1991.4488b.

Figure 2

Figure 1. A, Geometry and forces applied on a typical osteoderm (Caiman crocodilus) to simulate a bite coming from different directions. The force direction is parameterized by the pair of angles (α, λ). The five loading conditions considered in this study are depicted, and their angular coordinates are expressed in degrees. B, Finite element mesh and boundary conditions of a typical osteoderm (C. crocodilus). Elastic springs are applied on the lateral (red and green) and basal (blue) sides of the osteoderm (see text for details). X, transversal axis; Y, longitudinal axis; Z, vertical axis.

Figure 3

Figure 2. A, Parametric analysis with respect to the Young's modulus of the osteoderm (Eo). Left: von Mises stress; color scale: 0 (blue; light gray) to 100 MPa (red; dark gray). Right: High-stress volume fractions VF1 (blue; dark gray) and VF2 (purple; light gray) as a function of the Young's modulus of the osteoderm (Eo). Relevant reference parameters are: Eb = 0.1 GPa (Young's modulus of the basal tissue); N = 1 (number of lateral osteoderms); and α, λ = 0° (force orientation). An asterisk (*) denotes the reference value of Eo. B, Parametric analysis with respect to the Young's modulus of the basal tissue (Eb). Left: von Mises stress; color scale: 0 (blue; light gray) to 100 MPa (red; dark gray). Right: High-stress volume fractions: VF1 (blue; dark gray) and VF2 (purple; light gray) as a function of the Young's modulus of the basal tissue (Eb). Relevant reference parameters are: Eo = 10 GPa (Young's modulus of the osteoderm); N = 1 (number of lateral osteoderms); and α, λ = 0° (force orientation). An asterisk (*) denotes the reference value of Eb, which was used for the simulation on the full sample (presented in Table 1).

Figure 4

Figure 3. Parametric analysis in Caiman crocodilus with respect to the Young's modulus of the osteoderm (Eo; A, B) and of its basal tissue (Eb; C, D). A, Average von Mises stress in the osteoderm as a function of the Young's modulus of the osteoderm (Eo). B, High-stress volume fractions VF1 (blue/dark gray line; right-side scale) and VF2 (purple/light gray line; left-side scale) as a function of the Young's modulus of the osteoderm (Eo). Relevant reference parameters are: Eb = 0.1 GPa (Young's modulus of the basal tissue); N = 1 (number of lateral osteoderms); and α, λ = 0° (force orientation). C, Average von Mises stress in the osteoderm as a function of the Young's modulus of the basal tissue (Eb). D, High-stress volume fractions VF1 (blue/dark gray line; right-side scale) and VF2 (purple/light gray line; left-side scale) as a function of the Young's modulus of the basal tissue (Eb). Relevant reference parameters are: Eo = 10 GPa (Young's modulus of the osteoderm); N = 1 (number of lateral osteoderms); and α, λ = 0° (force orientation). See text for details.

Figure 5

Figure 4. Principal component analysis of the sampled osteoderm stress variables: VF1, VF2, σ̅VM with variation of α (0°, 45°, −45°) and λ (0°, 90°, −90°); PC1 explains 94% of the variance, 5% of the variance is explained by PC2. Performed using PAST v. 2.17c (Hammer et al. 2001).

Figure 6

Table 3. Mechanical indexes quantifying the von Mises stress distribution in the ornamented and smoothed specimens for each loading condition (α, λ) and in the average. ${{\bar {\rm \sigma}}} _{{\rm VM}}$, average von Mises stress in the osteoderm; VF1 and VF2, volume fractions of the regions where the von Mises stress exceeds the stress thresholds σ1 and σ2, respectively. See text for details. Osteolaemus tetraspis (a), MNHN-AC.1991.4488a; (b), MNHN-AC.1991.4488b.

Figure 7

Figure 5. von Mises stress in the 3D-modeled osteoderms (in MPa). A, Ornamented osteoderm of Caiman crocodilus; A1, view of the mid-osteoderm transversal cross section. Scale bar, 4mm. B, Smoothed osteoderm of C. crocodilus; B1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. C, Ornamented osteoderm of Osteolaemus tetraspis (MNHN-AC.1991.4488a); C1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. D, Smoothed osteoderm of O. tetraspis (MNHN-AC.1991.4488a); D1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. E, Ornamented osteoderm of O. tetraspis (MNHN-AC.1991.4488b); E1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. F, Smoothed osteoderm of O. tetraspis (MNHN-AC.1991.4488b); F1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. G, Ornamented osteoderm of Sarcosuchus imperator; G1, view of the mid-osteoderm transversal cross section. Scale bar, 10 mm. H, Smoothed osteoderm of S. imperator; H1, view of the mid-osteoderm transversal cross section. Scale bar, 10 mm. I, Ornamented osteoderm of Hyposaurus rogersii; I1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. J, Smoothed osteoderm of H. rogersii; J1, view of the mid-osteoderm transversal cross section. Scale bar, 4 mm. K, Ornamented osteoderm of Aetosaurus sp.; K1, view of the mid-osteoderm transversal cross section. Scale bar, 10 mm. L, Smoothed osteoderm of Aetosaurus sp.; L1, view of the mid-osteoderm transversal cross section. Scale bar, 10 mm. X, transversal axis; Y, longitudinal axis; Z, vertical axis. All plots refer to (α, λ) = (0°, 0°). Color scale: 0 (blue; light gray) to 100 MPa (red; dark gray).

Figure 8

Figure 6. von Mises stress in Caiman crocodilus osteoderm presented in both longitudinal and transversal cross sections for different loading conditions parameterized by the pair of angles (α, λ). Color scale: 0 (blue; light gray) to 100 MPa (red; dark gray).

Figure 9

Table 4. Differences between the mechanical indexes of the ornamented and smoothed osteoderms (positive values indicate that the index is higher in the actual osteoderm) for each loading condition (α, λ) and on average. See text for details. Osteolaemus tetraspis (a), MNHN-AC.1991.4488a; (b), MNHN-AC.1991.4488b.