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• Print publication year: 2011
• Online publication date: June 2012

# 2 - Stress

## Summary

Aims

Fractures form when the stress in the rock becomes so high that the rock breaks. Stress is thus of fundamental importance for understanding rock fractures. Stress has already been defined (Chapter 1). Here the focus is on those aspects of stress analysis that are most useful for understanding rock fractures. The primary aims of this chapter are to:

Explain some of the concepts from stress analysis, particularly those relevant to rock fractures.

Clarify the difference between a stress vector (traction vector) and a stress tensor and the relationship between these concepts.

Define the principal stresses and principal stress axes and planes.

Explain the stress ellipsoid.

Discuss stresses on an arbitrary plane and Mohr's circles of stress.

Define mean stress and deviatoric stress.

Indicate and explain the use of some special stress states.

Define stress fields and stress trajectories and explain their use in stress analysis.

Some basic definitions

Stress at a point is a tensor of the second rank, whereas the stress on a plane is a vector, that is, the stress vector or traction (Chapter 1). The magnitude of a stress, given as, say, 10 MPa, is a scalar. Before we discuss the concept of stress in more detail, it is necessary to recall some basic definitions that are assumed to be known. This section, of necessity, must be brief. More details on tensors, vectors, and scalars are provided in some of the books listed at the end of this chapter.

### Related content

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, , and , 2007. Fundamentals of Rock Mechanics, 4th edn. Oxford: Blackwell.
, 1969. Introduction to the Mechanics of a Continuous Medium. Upper Saddle River, NJ: Prentice-Hall.
, 1970. Continuum Mechanics. New York: McGraw-Hill.
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