Mechanical Properties of Biological Tissues

  • Nihat Özkaya
  • Margareta Nordin

Abstract

The material response discussed in the previous chapters was limited to the response of elastic materials, in particular to linearly elastic materials. Most metals, for example, exhibit linearly elastic behavior when they are subjected to relatively low stresses at room temperature. They undergo plastic deformations at high stress levels. For an elastic material, the relationship between stress and strain can be expressed in the following general form:
$$\sigma = \sigma (\varepsilon )$$
(9.1)
Equation (9.1) states that the normal stress σ is a function of normal strain ε only. The relationship between the shear stress τ and shear strain γ can be expressed in a similar manner. For a linearly elastic material, stress is linearly proportional to strain, and in the case of normal stress and strain, the constant of proportionality is the elastic modulus ε of the material (Figure 9.1):
$$\sigma = E\varepsilon $$
(9.2)
While investigating the response of an elastic material, the concept of time does not enter into the discussions. Elastic materials show time-independent material behavior.

Keywords

Cortical Bone Collagen Fiber Biological Tissue Elastic Material Viscoelastic Material 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer Science+Business Media New York 1999

Authors and Affiliations

  • Nihat Özkaya
    • 1
  • Margareta Nordin
    • 1
  1. 1.Occupational and Industrial Orthopaedic Center, Hospital for Joint Diseases Orthopaedic InstituteNew York University Medical CenterNew YorkUSA

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