Calculation of normal and shear stress on a plane

Frequently it is necessary to calculate the normal and the shear stress on an arbitrary plane (with unit normal vector n) that crosses a rigid body in equilibrium. Faults or cracks that cross the rock mass and may lead to rock failure are cases that require the estimation of the stress components on a plane. Another example may be the calculation of the normal and shear stress on the failure surface of a specimen during a typical rock mechanics experiment.

The components of the stress vector T acting on any plane crossing an arbitrary point inside a rigid body may be calculated as follows:

T_{i}^{(n)}=\sigma_{ij}n_{j}(1)

where \sigma_{ij} is the stress tensor describing the stress state at that point and n_{j} are the components of the unit normal vector of the plane. The stress vector can be broken down into two components, the normal stress and the shear stress as shown in Fig. 1.

Normal and shear component of the stress vector on a plane

Figure 1: Normal and shear component of the stress vector on a plane

The magnitude of the normal component of the stress vector is calculated by:

\sigma_{n}=T_{i}^{(n)}n_{i}=\sigma_{ij}n_{i}n_{j}(2)

and the magnitude of the shear stress is calculated by:

S_{n}^{2}=(T^{(n)})^{2}-\sigma_{n}^{2}(3)

Example

The stress state at a point is given by the following stress tensor:

\sigma_{ij}=\left[\begin{array}{ccc}5 & 2 & 6 \\ 2 & 3& 4 \\ 6 & 4 & 1\end{array}\right](4)

For a plane with unit normal:

n=\left(\frac{1}{3},\frac{1}{2},\frac{\sqrt{23}}{6}\right)(5)

calculate the normal and shear components of the stress vector.

Solution

Firstly we will calculate the magnitude of the normal stress by using equation (2):

\begin{array}{rl}\sigma_{n}=&\sigma_{11}n_{1}^{2}+\sigma_{22}n_{2}^{2}+\sigma_{33}n_{3}^{2}\\ &+2(\sigma_{12}n_{1}n_{2}+\sigma_{23}n_{2}n_{3}+\sigma_{13}n_{1}n_{3})\\=&9\end{array}(6)

In order to calculate the shear component, we must calculate the components of the stress vector by virtue of equation (1):

\begin{array}{l}T_{1}=\sigma_{11}n_{1}+\sigma_{12}n_{2}+\sigma_{13}n_{3}=7.5\\T_{2}=\sigma_{21}n_{1}+\sigma_{22}n_{2}+\sigma_{23}n_{3}=5.4\\T_{3}=\sigma_{31}n_{1}+\sigma_{32}n_{2}+\sigma_{33}n_{3}=4.8\end{array}(7)

Hence, the magnitude of the stress vector squared is given by:

(T^{(n)})^{2}=T_{1}^{2}+T_{2}^{2}+T_{3}^{2}=108.45(8)

Finally, the magnitude of the shear stress component is:

|S_{n}|=\sqrt{(T^{(n)})^2-\sigma_{n}^{2}}=5.2(9)

Suggested Bibliography

L.E. Malvern. Introduction to the Mechanics of a Continuous Medium. Prentice Hall, Englewood Cliffs, New Jersey, 1969.

Y.C. Fung. A First Course in Continuum Mechanics. Prentice Hall, Englewood Cliffs, New Jersey, 3rd ed., 1994.

M. Gurtin, E. Fried and L. Anand. The Mechanics and Thermodynamics of Continua. Cambridge University Press, Cambridge, 2010.

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