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The Earth's Shifting Crust by Charles Hapgood - wire of information

The Earth's Shifting Crust by Charles Hapgood - wire of information

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i86 EARTH'S SHIFTING CRUST<br />

diminution <strong>of</strong> the tensile strength and rigidity <strong>of</strong> the rock.<br />

<strong>The</strong> decline <strong>of</strong> strength continues to the bottom <strong>of</strong> the crust.<br />

Dr. Jeffreys remarks: ". . . At some depth ... it begins to<br />

decrease and may be a tenth <strong>of</strong> that <strong>of</strong> surface rock at a depth<br />

<strong>of</strong> 30 miles. . . ." (238:202).<br />

At the bottom <strong>of</strong> the crust, perhaps about 36 miles below<br />

the surface <strong>of</strong> the earth, an important change <strong>of</strong> state<br />

apparently takes place. <strong>The</strong> heat reaches the melting point<br />

<strong>of</strong> the rocks, and the rocks can no longer crystallize. Since the<br />

strength <strong>of</strong> rocks depends mostly upon a structure <strong>of</strong> strong,<br />

interlocking crystals, the change <strong>of</strong> state implies a disappearance<br />

<strong>of</strong> strength. For this reason Pr<strong>of</strong>essor Daly considers the<br />

asthenosphere to be "essentially liquid/'<br />

". . . For it is<br />

hardly to be doubted that a rock layer, too hot to crystallize,<br />

has only a minute strength, or no strength whatever" (97:399-<br />

400).<br />

Jeffreys is in agreement that the melting point<br />

<strong>of</strong> rock<br />

should be reached about 36 miles down (238:140), judging<br />

from the heat gradient.<br />

If it were only a question <strong>of</strong> the crystalline or noncrystalline<br />

structure <strong>of</strong> the rock, we would readily conclude that<br />

the asthenosphere could <strong>of</strong>fer no serious resistance to the dis-<br />

placement <strong>of</strong> the crust. <strong>The</strong> crust would be truly (to use Einstein's<br />

term) a "floating crust."<br />

But we must also take into account another quality <strong>of</strong> mat-<br />

ter, which is viscosity. Materials possess varying degrees <strong>of</strong><br />

viscosity. Viscosity can make a liquid act like a solid. If, for<br />

diver hits the surface <strong>of</strong> the water at a bad<br />

example, a high<br />

angle he may kill himself, because the water, though liquid,<br />

requires time to flow, and if the impact is too sudden there<br />

is no flow and the liquid acts as a solid. Tar is an example<br />

<strong>of</strong> a more viscous substance. Taffy candy is highly viscous,<br />

and can be cut with scissors, and yet, given a certain amount<br />

<strong>of</strong> time, it will flow like a liquid. <strong>The</strong> effect <strong>of</strong> pressure on<br />

different substances is to increase their viscosity, to make<br />

them stiffer. <strong>The</strong>y will then resist sudden shocks better, but<br />

will flow like liquids if subjected to steady pressure for a con-

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