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principles and applications of microearthquake networks

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6.2. Frrult-Plutie Solution 139<br />

(1980). We expect that many techniques resulting from these advances<br />

will be applied to <strong>microearthquake</strong> data in the near future.<br />

6.2. Fault-Plane Solution<br />

The elastic rebound theory <strong>of</strong> Reid (1910) is commonly accepted as an<br />

explanation <strong>of</strong> how most earthquakes are generated. This theory has been<br />

concisely described by Stauder (1 962, p, 1) as follows: earthquakes<br />

occur in regions <strong>of</strong> the earth that are undergoing deformation. Energy is<br />

stored in the form <strong>of</strong> elastic strain as the region is deformed. This process<br />

continues until the accumulated strain exceeds the strength <strong>of</strong> the rock,<br />

<strong>and</strong> then fracture or faulting occurs. The opposite sides <strong>of</strong> the fault rebound<br />

to a new equilibrium position, <strong>and</strong> the energy is released in the<br />

vibrations <strong>of</strong> seismic waves <strong>and</strong> in heating <strong>and</strong> crushing <strong>of</strong> the rock. If<br />

earthquakes are caused by faulting, it is possible to deduce the nature <strong>of</strong><br />

faulting from an adequate set <strong>of</strong> seismograms, -<strong>and</strong> in turn, the nature <strong>of</strong><br />

the stresses that deform the region.<br />

Let us now consider a simple earthquake mechanism as suggested by<br />

the 1906 San Francisco earthquake. Figure 26 illustrates in plan view a<br />

Fig. 26. Plan view <strong>of</strong> the distribution <strong>of</strong> compressions ( + ) <strong>and</strong> dilatations (-) resulting<br />

from a right lateral displacement along a vertical fault FF'.

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