Biomedical Engineering Reference
In-Depth Information
Table 1 Elastic modulus of human cortical bone measured in monotonic tests
Orientation
Bone
Test
Modulus (GPa)
References
Longitudinal
Femur
Tension
15.6-19.4
[ 59 , 60 , 62 , 148 ]
Compression
15.2-18.1
[ 60 , 62 , 149 ]
Torsion
3.3-5.0
[ 51 , 54 ]
3pt-Bending
10.8-15.8
[ 63 - 66 ]
4pt-Bending
12.1
[ 150 ]
Tibia
Tension
18.0-29.2
[ 59 , 60 ]
Compression
25.9-35.3
[ 60 ]
Cantilever bending
10.6
[ 151 ]
Fibula
Tension
18.5
[ 59 ]
Humerus
Tension
17.2
[ 59 ]
Radius
Tension
18.5
[ 59 , 152 ]
Ulna
Tension
18.4
[ 59 ]
Compression
14.2
[ 55 ]
Radial
Ulna
Compression
3.8
[ 55 ]
Lateral
Compression
4.2
[ 55 ]
The elastic modulus of cortical bone depends strongly on its porosity [ 56 ].
Porosity also strongly influences the apparent, volumetric bone mineral density of
cortical bone, so measures of density strongly correlate with elastic modulus
[ 57 , 58 ]. In addition, modulus may vary with anatomic location, loading mode,
orientation, degree of mineralization, and specimen size. As shown in Table 1 ,
samples from human tibias tend to have a higher elastic modulus than samples
from other sites including the femur; samples from the fibula, humerus, radius and
ulna were reported to have similar tensile elastic moduli [ 59 , 60 ]. The elastic
properties may also change with anatomic locations within long bones [ 53 ]. For
instance, the elastic modulus of human cortical bone from male donors is greater
for femoral diaphysis than metaphysis [ 61 ].
Although some data suggest a difference between tensile and compressive
moduli, Reilly et al. [ 62 ] concluded that there was no significant difference
between these two loading modes based on paired comparisons from *200
samples of human femoral cortical bone. On the other hand, the flexural moduli
obtained from three-point and four-point bending tests are significantly different
(lower) from those of axial (tension or compression) tests [ 63 - 66 ]. It should be
noted that unlike a uniaxial test, the elastic modulus value obtained from bending
tests is based upon linear elastic beam theory, which may not fully reflect the true
elastic behavior of bone in bending.
Due to spatial heterogeneity and hierarchical features, the elastic behavior of
bone depends on specimen size (Table 2 ). Micro-specimens taken from osteons
and interstitial tissues of human femurs have revealed significantly different
properties when compared to those of macro-specimens. The tensile [ 67 ] and
compressive [ 68 ] moduli at the microscopic level are much lower than those
obtained at the macroscopic level. In contrast, torsion tests at the microscopic level
have obtained modulus values significantly higher than those obtained at the
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