From: Elastic Bounds of Bioinspired Nanocomposites

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From: Elastic Bounds of Bioinspired Nanocomposites Date of download: 11/6/2017 Copyright © ASME. All rights reserved. From: Elastic Bounds of Bioinspired Nanocomposites J. Appl. Mech. 2013;80(6):061017-061017-6. doi:10.1115/1.4023976 Figure Legend: Typical staggered nanostructures observed in load-bearing biological materials. (a) The staggered alignment of mineral platelets in shell, also referred to as the “brick-and-mortar” structure; (b) the stairwise alignment of hydroxyapatite nanocrystals in mineralized collagen fibrils of bone; (c) the “stairwise staggering” alignment of tripocollagen molecules in collagen fibrils of tendon, with a periodic unit cell comprising four tripocollagen molecules. Note that the staggered alignment of mineral crystals in bone is a result of mineralization of collagen fibrils.

From: Elastic Bounds of Bioinspired Nanocomposites Date of download: 11/6/2017 Copyright © ASME. All rights reserved. From: Elastic Bounds of Bioinspired Nanocomposites J. Appl. Mech. 2013;80(6):061017-061017-6. doi:10.1115/1.4023976 Figure Legend: Generalized stairwise staggering alignments mimicking collagen fibrils. (a) Schematic nanostructure of biocomposites; (b) the unit cell (solid box) with staggering number n, and (c) the assumed kinematically admissible strain field under a longitudinal elongation Δ.

From: Elastic Bounds of Bioinspired Nanocomposites Date of download: 11/6/2017 Copyright © ASME. All rights reserved. From: Elastic Bounds of Bioinspired Nanocomposites J. Appl. Mech. 2013;80(6):061017-061017-6. doi:10.1115/1.4023976 Figure Legend: (a) The assumed static equilibrium stress field in the stairwise staggered nanostructure under a longitudinal elongation Δ, (b) the distribution of shear traction along a hard platelet, and (c) the distribution of normal stress in the platelet

From: Elastic Bounds of Bioinspired Nanocomposites Date of download: 11/6/2017 Copyright © ASME. All rights reserved. From: Elastic Bounds of Bioinspired Nanocomposites J. Appl. Mech. 2013;80(6):061017-061017-6. doi:10.1115/1.4023976 Figure Legend: The finite element mesh in a representative unit cell for (a) the regular “brick-and-mortar” structure with n = 2 and (b) a “stairwise staggering” structure with n = 5

From: Elastic Bounds of Bioinspired Nanocomposites Date of download: 11/6/2017 Copyright © ASME. All rights reserved. From: Elastic Bounds of Bioinspired Nanocomposites J. Appl. Mech. 2013;80(6):061017-061017-6. doi:10.1115/1.4023976 Figure Legend: Variations of elastic bounds for Young's modulus as a function of the aspect ratio of platelets for (a) the “brick-and-mortar” structure with staggering number n = 2 and (b) the “stairwise staggering” structure with n = 5. In both (a) and (b), a moderate volume fraction ϕ = 50% of mineral is adopted. The dash-dotted line is the upper bound while the solid line is the lower bound. The filled square data points are from finite element analysis. The predictions from the Voigt and Mori–Tanaka models are shown as the dashed and dotted lines, respectively.

From: Elastic Bounds of Bioinspired Nanocomposites Date of download: 11/6/2017 Copyright © ASME. All rights reserved. From: Elastic Bounds of Bioinspired Nanocomposites J. Appl. Mech. 2013;80(6):061017-061017-6. doi:10.1115/1.4023976 Figure Legend: Variation of elastic bounds for Young's modulus as a function of the aspect ratio of platelets for (a) the “brick-and-mortar” structure with staggering number n = 2 and (b) the “stairwise staggering” structure with n = 5. A large volume fraction ϕ = 90% of mineral is adopted. The dash-dotted line is the upper bound while the solid line is the lower bound. The filled square data points are from finite element analysis. The predictions from the Voigt and Mori–Tanaka models are shown as the dashed and dotted lines, respectively.