Relationship between Modulus of Elasticity and Modulus of Rigidity

Jacob
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Modulus of elasticity (E) and the modulus of rigidity (G) are related by the following equation:

E=2G\left( 1+\nu\right)

Here, \nu represents a number called Poisson’s ratio given to the particular material. When the material is being stretched in one direction, it gets shortened in a perpendicular direction. In the direction that the material becomes elongated, the axial strain (\varepsilon_ais defined as the fractional increase in the length. In the direction that the material shortens, the transverse strain (\varepsilon_t) gives the fractional reduction in length. The diagram below illustrates these changes in shape:

Difference Between Modulus of Elasticity and Modulus of Rigidity - Poisson's_Ratio_Illustration

Defining Poisson’s ratio

In this diagram, the axial strain is:

\varepsilon_a=\frac{x'-x_0}{x_0}

The transverse strain is:

\varepsilon_t=\frac{y'-y_0}{y_0}

Note that since the object shortens in the direction perpendicular to the force, \varepsilon_t<0. Poisson’s ratio (\nu) is defined as:

\nu=-\frac{\varepsilon_t}{\varepsilon_a}

The minus sign has been introduced to ensure that \nu takes a positive value.

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