Optical determination of anisotropic material properties of bovine articular cartilage in compression
Introduction
As the load-bearing material of diarthrodial joints, articular cartilage helps to absorb mechanical shocks and distribute high joint loads more evenly across the underlying bony structures, while maintaining minimal friction and wear (Mankin et al., 1994; Mow and Ateshian, 1997; Ateshian et al., 1998). Articular cartilage is a structurally and compositionally complex material. Most of the biochemical constituents of articular cartilage (e.g., glycosaminoglycans, collagen and water) are inhomogeneously distributed, giving the tissue a layered character (Weiss et al., 1968; Redler and Zimny, 1970; Bullough and Jagannath, 1983; Maroudas et al., 1969; Venn and Maroudas, 1977; Muir, 1980; Buckwalter et al., 1985; Hardingham and Fosang, 1992). These variations in the structure and composition of cartilage are closely related to the inhomogeneous and anisotropic mechanical and electrochemical properties of the tissue.
Despite the intensive study of articular cartilage in the field of biomechanics, the exact nature of cartilage as a material remains to be elucidated. There are still no established answers to some of the most basic questions such as the nature of the material's symmetry that are commonly asked for a classical material. As greater efforts have been placed on the study of tissue anisotropy in tension, it has been shown that the equilibrium tensile modulus of articular cartilage is significantly greater for specimens harvested parallel to the split-line directions than for those perpendicular to the split lines (Kempson et al (1968), Kempson et al. (1973); Woo et al (1976), Woo et al (1979); Roth and Mow, 1980; Huang et al., 1999); the tensile modulus has also been investigated along the depth-direction (Basser et al., 1998; Narmoneva et al., 1999), but has not yet been related to the other two directions. Nevertheless, since the tensile properties of cartilage have been found to differ along two of these three mutually perpendicular directions (Huang et al., 1999; Narmoneva et al., 1999; Korhonen et al., 2001), it is likely that the highest symmetry of cartilage is at best orthotropic, with its three planes of symmetry defined in situ by the split-line direction in a plane tangent to the surface (1-direction), the direction perpendicular to the split-line direction in the same tangent plane (2-direction), and the direction normal to this plane (3-direction), i.e. the “radial” (or depth) direction of the cartilage layer (Soltz and Ateshian, 2000). In further support of cartilage anisotropy in tension, several studies (Woo et al., 1979; Chang et al., 1999; Elliott et al., 1999; Huang et al., 1999) have demonstrated that Poisson's ratio for cartilage in uniaxial tension exceeds 0.5, which is permissible only for anisotropic materials (e.g., Lai et al., 1993). For human humeral head cartilage, Huang et al. (1999) reported an average Poisson's ratio value of ν+12=1.3 for uniaxial tension along the 1-direction and measurement of the contraction along the 2-direction, and a similar average of ν+21=1.3 for the converse configuration, in the superficial zone of cartilage; in the middle zone, these values reduced to ν+12=1.2 and ν+21=1.0. For human patellar cartilage, Chang et al. (1999) reported average values of ν+12=0.9 and ν+13=1.8 in the surface-to-middle zone, and ν+12=0.5 and ν+13=0.7 in the deep zone, whereas Elliott et al. (1999) reported ν+12=2.2 in the superficial zone and ν+12=0.6 in the middle zone.
In contrast to tensile measurements, there are only a few preliminary studies that have investigated the anisotropy of cartilage in compression. Jurvelin et al. (1996) have reported measurements of the compressive modulus of cartilage in unconfined compression, on cylindrical specimens whose axis was oriented either along the radial 3-direction (which is the most commonly tested direction in compression studies) or along a direction parallel to the cartilage surface (though no relation to the split-line direction was reported). They found the compressive modulus of human knee cartilage in the 3-direction to be smaller (0.58 MPa versus 0.85 MPa), suggesting that cartilage is also anisotropic in compression. However, in a study by Soltz et al. (1999) where immature bovine carpometacarpal joint cartilage cubes were tested in unconfined compression along the 1-, 2-, and 3-directions, no significant differences were found in the compressive moduli among the three direction (with mean values ranging from 0.41 MPa along the 1-direction to 0.47 MPa in the 3-direction). From compression experiments, Poisson's ratio at equilibrium has been found to be small in human and bovine articular cartilage (Jurvelin et al., 1997; Wang et al., 2000b; Wong et al., 1998; Wong, 1999). Optical measurements from unconfined compression have yielded an average equilibrium Poisson's ratio of 0.18 in bovine humeral head cartilage (Jurvelin et al., 1997) and 0.06 in bovine carpometacarpal joint cartilage (Wang et al., 2000b).
While these results suggest that cartilage does not exhibit the same anisotropy in compression as it does in tension, the nature of the anisotropy of cartilage in compression remains undetermined. The primary objective of this study, therefore, is to determine the equilibrium compressive Young's moduli and Poisson's ratios of bovine cartilage along multiple directions (1-, 2- and 3-directions) by loading cubic specimens in unconfined compression, with the expectation that the material symmetry of cartilage can be determined more accurately with the help of a more complete set of material properties. Optimized digital image correlation (DIC) is adopted to accurately determine the resultant strain fields within the specimens under loading. It is noted that the studies reported above on the tensile and compressive properties of articular cartilage confirm that the cartilage moduli and Poisson ratios can be very different in tension and compression. Thus, the second objective of this study is to investigate how the tension-compression nonlinearity of cartilage might alter the interpretation of material symmetry (Curnier et al., 1995; Soltz and Ateshian, 2000). Based on previous findings in the literature as reviewed above, it is hypothesized in the current study that the material symmetry of cartilage is no lower than orthotropic.
Section snippets
Specimen preparation
Healthy shoulder joints from 2- to 3-month-old calves were obtained from a local slaughterhouse 4–8 h post-mortem. A steel trephine with a 4-mm diameter core was used to harvest cartilage-bone plugs with the core axis perpendicular to the articular surface. The plugs were then rinsed with phosphate buffered saline (PBS) and protease inhibitors (PI) and frozen at −80°C for storage until the day of use. On the day of testing, plugs were thawed to room temperature by immersion in freshly prepared
Results
Prior to each of the six tests performed on the cubic specimens, specimen dimensions were re-measured. No permanent deformation was observed and the specimens were found to recover fully to their original dimensions after load removal from previous loading. The determination of material properties relies on the description of the deformation inside a tissue specimen under loading. The displacement distributions resulting from the six tests on a typical cubic sample are plotted in Fig. 4 as a
Discussion
The testing configuration employed in this study allowed the characterization of three Young's moduli and six Poisson's ratio on the same specimen, using an optical technique and digital image correlation analysis to measure the tissue strains. The inhomogeneity of articular cartilage through its depth (the 3-direction) increases the complexity of characterizing its intrinsic material properties. Among all six tests performed on the cubic specimens, compression along the 3-direction produced
Acknowledgements
This study was supported by funds from the National Institute of Arthritis and Musculoskeletal and Skin Diseases of the National Institutes of Health (AR46532, AR46568).
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