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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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190<br />

EARTH'S SHIFTING CRUST<br />

ago, which are still suggestive <strong>of</strong> the probable<br />

material in the asthenosphere:<br />

behavior <strong>of</strong><br />

<strong>The</strong> ingenious experiments <strong>of</strong> M. Tresca on the flow <strong>of</strong> solids<br />

have thrown considerable light on the internal deformations <strong>of</strong> rock-<br />

masses. He has proved that, even at ordinary atmospheric temperatures,<br />

solid resisting bodies like lead, cast iron, and ice may be so<br />

compressed as to undergo an internal motion <strong>of</strong> their parts, closely<br />

analogous to that <strong>of</strong> fluids. Thus a solid jet <strong>of</strong> lead has been produced,<br />

<strong>by</strong> placing a piece <strong>of</strong> the metal between the jaws <strong>of</strong> a powerful<br />

compressing machine. Iron, in like manner, has been forced to<br />

flow in the solid state into cavities and take their shape. On cutting<br />

sections <strong>of</strong> the metal so compressed, their particles <strong>of</strong> crystals are<br />

found to have arranged themselves in lines <strong>of</strong> flow which follow<br />

the contours <strong>of</strong> the space into which they have been squeezed. . . .<br />

(170:316).<br />

It seems altogether unlikely that material under the pres-<br />

sures prevailing at the bottom <strong>of</strong> the crust, and at very high<br />

temperatures, could resist the shearing movement <strong>of</strong> the crust<br />

over it. Let us remember that in a displacement <strong>of</strong> the crust<br />

very little material, comparatively speaking, would actually<br />

have to flow. <strong>The</strong> crust would simply start to slip over the<br />

the most<br />

asthenosphere. <strong>The</strong> action would be one <strong>of</strong> gliding,<br />

economical form <strong>of</strong> motion, though, as already explained,<br />

the downward protuberances <strong>of</strong> continents and mountain<br />

chains might act to slow down the movement.<br />

To conclude, then, the asthenosphere could have consid-<br />

erable viscosity, even at the top, and yet <strong>of</strong>fer no definite<br />

obstacle to the displacement <strong>of</strong> the crust. Once the crust<br />

started to move, the braking influence <strong>of</strong> the viscosity would<br />

steadily decline, for with the increasing distance <strong>of</strong> the cen-<br />

ter <strong>of</strong> mass <strong>of</strong> the icecap from the axis, the centrifugal effect<br />

would be multiplied (Chapter XII). No friction between the<br />

two layers could suffice to absorb this ever increasing thrust.<br />

It would have to continue until the motive force was removed<br />

<strong>by</strong> the melting <strong>of</strong> the icecap in the warmer latitudes.<br />

And, in the meantime, as Frankland has suggested, the fric-<br />

tion would have been productive <strong>of</strong> heat that might have<br />

further facilitated the movement.

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