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. 2015 Oct 6;12(111):20150343. doi: 10.1098/rsif.2015.0343

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© 2015 The Authors.

Published by the Royal Society under the terms of the Creative Commons Attribution License http://creativecommons.org/licenses/by/4.0/, which permits unrestricted use, provided the original author and source are credited.

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Figure 3. — (a) Force versus stretch along the first direction for a sample treated by Mooney–Rivlin biomechanical energy and fully disordered fibres in the CB mode (T = 1/2). The shear modulus is chosen as unit, ρ and ρ₁ varies in order to change the curvature at the origin according to equation (4.6). (b) Force versus stretch along the first direction for a sample treated with Mooney–Rivlin biomechanical energy and oriented fibres. The shear modulus is chosen as unit, ρ and ρ₁ are fixed to give a priori a negative curvature with ρ = −0.85 and ρ₁ = 3, but the fibre orientation varies.

Inline graphic — (a) Force versus stretch along the first direction for a sample treated by Mooney–Rivlin biomechanical energy and fully disordered fibres in the CB mode (T = 1/2). The shear modulus is chosen as unit, ρ and ρ₁ varies in order to change the curvature at the origin according to equation (4.6). (b) Force versus stretch along the first direction for a sample treated with Mooney–Rivlin biomechanical energy and oriented fibres. The shear modulus is chosen as unit, ρ and ρ₁ are fixed to give a priori a negative curvature with ρ = −0.85 and ρ₁ = 3, but the fibre orientation varies.