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Given two dimensionless parameters, λ and ρ, that define the orthotropy of the material, the elastic response is unique.
For this material, the elastic constants were determined by ultrasound phase spectroscopy and show transverse isotropy with C11 = 40, C12 = 20, C13 = 13.1, C33 = 18.2, C44 = 1.8 GPa.
By applying the point-force Green's function for a three-dimensional anisotropic elastic material, the elastic displacement induced by a dislocation of polygonal shape is derived in terms of a simple line integral.
Although the as-fabricated iron part possesses a higher tensile strength even than that of bulk iron material, the elastic modulus of the annealed specimens decreased to 188 ± 10 GPa and the ultimate tensile strength was much improved from 357 ± 22 MPa up to 401 ± 23 MPa.
For a linearly elastic material, the elastic modulus is defined as the slope of the stress-strain curve.
Similar(55)
For elastic and isotropic materials, the elastic constants are interrelated.
For such materials the elastic limit marks the end of elastic behaviour and the beginning of plastic behaviour.
When tan is high (G″ > G′) a material has stronger viscous character, on the contrary when tan is low (G′ > G″) in a materials the elastic behavior is dominant.
In these materials the elastic modulus of the gel increases orders of magnitude as the applied strain increases such that the resistance that a cell feels would be a strong function of the strain that it applies.
These thermal changes in the material affect the elastic and creep properties of the material, and in turn, the stress fields within the structure.
The two indicators of bone material properties, the elastic modulus and stress at the yielding point, were significantly reduced.
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