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. Author manuscript; available in PMC: 2007 Nov 21.
Published in final edited form as: J Biomech. 2007 May 17;40(14):3070–3078. doi: 10.1016/j.jbiomech.2007.03.019

Figure 1.

Figure 1

1-D “spring and dashpot” representation of the adaptive QLV model, a parallel combination of nonlinear springs and dashpots where the spring stiffnesses and dashpot coefficients are functions of overall strain and not their individual strain. So is the initial cross section of specimen, lo is the initial length of specimen, loVi is the displacement of the hypothetical spring and ε and σ are uniaxial, linearized strain and stress, respectively.