Mammalian bone is a relatively tough composite consisting of aligned, compliant, collagen fibrils with attached platelets of a stiff hydroxyapatite (Ca 10 (PO 4 ) 6 (OH) 2 ) mineral phase. It is composed of two spatially distinct topologies (Fig. 1). [1] The outside consists of relatively dense, hard layer of cortical bone. The interior is cellular, referred to as cancellous or trabecular bone (Fig. 1), consisting of inter-connected struts and faces. Its open cell topology resembles that found in synthetic cellular materials, such as open-cell metallic and polymer foams. [1] Both types of bone contain collagen fibrils arranged in bundles, aligned along the longitudinal axis (Fig. 1). The mineral phase, located primarily on the outside of the collagen, is resistant to fragmentation because it consists of tiny, nano-scale platelets (Fig. 2). [2±4] Parallel to the collagen fibrils, the inelastic responses of cortical bone differ in tension and compression [1,5±10] (Fig. 3(a)). In tension, it yields, followed by (linear) hardening up to a failure strain of order 2.5 %. In compression, it also yields, but at higher stress. It strain hardens rapidly to a peak, then softens and fails at strains of about 1.5 %. Trabecular bone exhibits extensive inelastic deformation under compression ( Fig. 3(b)), often attaining strains exceeding 60 % before failure. [10] A stress peak is typical, occurring at strains of 5±10 %.Flexure tests (Fig. 4) have been designed and conducted on cortical bone with two objectives. (a) Measure the inelastic strains and parse these strains between plasticity (volume conserving permanent strain) and dilatation. (b) Deduce the hysteresis and measure changes in stiffness with permanent strain. Results and Discussion: A typical response relating the load to the axial-strain upon monotonic testing to failure is summarized on Figure 5. The corresponding stress/strain curves obtained by de-convolution [11] are plotted on Figure 6. A plot of the trends in the inelastic Poisson ratio (the ratio of the transverse to the axial inelastic strains) with inelastic strain (Fig. 7) highlights the differences in tension and compression. Such characteristics are similar to those found in other biomaterials, such as nacre, [11] and in some synthetic materials, such as oxide composites. [12] At strains beyond yield, the following features are most notable (Figs. 6±10).In tension, the material behaves as an inelastic solid with linear strain hardening (Fig. 6): tangent modulus, E H » 1 GPa. The transverse strain is negligible, signifying an inelastic Poisson ratio, m pl » 0 (Fig. 7). That is, the material dilates.In compression, the peak stress is appreciably larger than in tension, but the strain at failure is smaller (e f » 1.6 % in compression and e f » 2.4 % in tension: Fig. 6). Consequently, COMMUNICATIONS ADVANCED ENGINEERING MATERIALS 2005, 7, No. 8 Fig. 1. Schematic illustration showing the configuration of cortical and trabecular bone in a typical mammalian femur.Fig. 2. A schematic of the nano-scale organiz...