52 Deformation of Tissues

Stress vs. Strain Curves

If you apply some to a material and measure the resulting , or vice versa, you can create a stress vs. strain curve like the one shown below for a typical metal.

Figure shows a stress-strain plot. When the strain is below 1%, point H, stress grows linearly. Plastic deformation, marked as P, takes place between 1% and 30%. Further increase in strain results in fracture.
Typical stress-strain plot for a metal: The graph ends at the fracture point. The arrows show the direction of changes under an ever-increasing stress. Points H and E are the linearity and elasticity limits, respectively.  The green line originating at P illustrates the metal’s return to a greater than original length when the stress is removed after entering the plastic region. Image Credit: OpenStax University Physics

[1]

We see that the metal starts off with stress being proportional to strain, which means that the material is operating in its . We have graphed stress on the vertical axis and strain on the horizontal axis, so the value of stress/strain is equal to the rise/run of the graph. We saw in the previous chapter that within the stress/strain is equal to the the and we know the rise/run of a graph is the slope, therefore the elastic modulus of a material is equal to the slope of the linear portion its stress vs. curve. Let’s discuss the important features of the stress vs. strain curve:

  1. The absolute highest point on the graph is the , indicating the onset of failure toward or .
  2. Notice that after reaching the ultimate strength, but before full failure, the stress can actually decrease as strain increases, this is because the material is changing shape by breaking rather than stretching or compressing the distance between molecules in the material.
  3. In the first part of the , the strain is proportional to the stress, this is known as the . The slope of this region is the .
  4. After the stress reaches the linearity limit (H) the slope is no longer constant, but the material still behaves elastically.
  5. The ends and the begins at the (E). In the plastic region, a little more stress causes a lot more strain because the material is changing shape at the molecular level. In some cases  the stress can actually decrease as strain increases,  because the material is changing shape by re-configuring molecules rather than just stretching or compressing the distance between molecules.
  6. The green line originating at P illustrates the metal’s return to non-zero strain value  when the stress is removed after being stressed into the plastic region (permanent deformation).

Stress and Strain in Tendons

Tendons (attaching muscle to bone) and ligaments (attaching bone to bone) have somewhat unique behavior under .  Functionally, tendons and ligaments  must stretch easily at first to allow for flexibility, corresponding to the of the stress-train curve shown below, but then resist significant stretching under large stress to prevent hyper-extension and dislocation injuries.

Line graph of change in length versus applied force. The line has a constant positive slope from the origin in the region where Hooke’s law is obeyed. The slope then decreases, with a lower, still positive slope until the end of the elastic region. The slope then increases dramatically in the region of permanent deformation until fracturing occurs.
Typical stress-strain curve for mammalian tendon. Three regions are shown: (1) toe region (2) linear region, and (3) failure region. Image adapted from OpenStax College Physics.

[2]

The structure of the tendon creates this specialized behavior. To create the toe region, a small stress causes the fibers in the tendon begin to align in the direction of the stress, or , and the re-alignment provides additional length. Then in the , the fibrils themselves will be stretched.

Stress and Strain Injuries

beyond the will cause permanent deformation and stress beyond the will cause or . These occurrences in body tissues are known as injuries. For example, sprains occur when a ligament (connects bone to bone) is torn by a stress greater than its ultimate strength, or even just stretched beyond its . The same event occurring in a tendon (connects muscle to bone) is called known as strain.[3] We already know that has a different, but related meaning to physicists and engineers, so that discrepancy in terminology is something to watch out for.

Reinforcement Activity


  1. OpenStax University Physics, University Physics Volume 1. OpenStax CNX. Aug 2, 2018 http://cnx.org/contents/d50f6e32-0fda-46ef-a362-9bd36ca7c97d@11.1.
  2. OpenStax, College Physics. OpenStax CNX. Aug 6, 2018 http://cnx.org/contents/031da8d3-b525-429c-80cf-6c8ed997733a@13.1.
  3. "Sprains and Strains" by Patient Care and Health InformationMayo Clinic

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