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Physics for Geologists, Second edition

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96 Stress and strain<br />

In geology, viscosities will be very large, probably of the order of 10 x<br />

10'' Pa s, but even these could lead to catastrophic rates of sliding of perhaps<br />

10m a year on quite small slopes. When Smoluchowski (1909) addressed<br />

the problems of sliding he wrote:<br />

Suppose a layer of plastic material, say pitch, interposed between the<br />

block and the underlying bed; or suppose the bed to be composed of<br />

such material: then the law of viscous liquid friction will come into play,<br />

instead of the friction of solids; there<strong>for</strong>e any <strong>for</strong>ce, however small, will<br />

succeed in moving the block. Its velocity may be small if the plasticity is<br />

small, but in geology we have plenty of time; there is no hurry.<br />

Bending and folding<br />

There are several ways of bending layered material, and it is one of the<br />

retarding influences on geology that many seem to think of bending only in<br />

terms of lateral compression (Figure 9.5). Carey (1954) in this regard is still<br />

worth reading. (Since we are concerned with geology, we shall talk about<br />

folding or de<strong>for</strong>mation rather than bending.)<br />

Folding is certainly possible by crumpling a thin sheet under lateral com-<br />

pression, but it arises more commonly from mechanical instability in the<br />

outer parts of the Earth, and in layered sequences under conditions where<br />

gravity plays a part. In an unstable layered system (such as one in which<br />

the upper layers are more dense than the lower), de<strong>for</strong>mation will result in<br />

folding of the type shown in the upper part of Figure 9.5 - and such folding<br />

may be induced in stable layers above and below the unstable layer.<br />

Folding requires compensation in space, either by sliding on surfaces, or<br />

flowing of the less viscous material, or both. Bending a beam puts the con-<br />

cave side in compression and the convex side in extension. Under some<br />

circumstances this can cause fracture, but in some cases natural rocks can-<br />

not sustain such stresses over long periods of time, and behave more like<br />

liquids.<br />

Copyright 2002 by Richard E. Chapman<br />

Figure 9.5 Folding can be by bending or buckling.

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