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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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EARTH'S SHIFTING CRUST<br />

real events would not correspond to this. <strong>The</strong> crust would<br />

be under bursting stress, and this would be relieved spasmodically,<br />

during the movement <strong>of</strong> the crust, <strong>by</strong> fractures at<br />

the weakest points. A fracture through the crust at one point<br />

would relieve the stress for perhaps hundreds <strong>of</strong> miles. Since<br />

the elasticity <strong>of</strong> the crust is slight, the stretching or extension<br />

<strong>of</strong> the crust would consist <strong>of</strong> the drawing apart, to varying<br />

distances, <strong>of</strong> the fractured blocks. Generally speaking, the<br />

fewer the fractures, the farther their sides would draw apart.<br />

It would be possible that the total amount <strong>of</strong> the stretching<br />

<strong>of</strong> the earth's circumference would be concentrated in rela-<br />

tively few critical areas.<br />

It must also be kept in mind that some parts <strong>of</strong> this area<br />

being displaced toward the equator will be displaced farther<br />

than others. <strong>The</strong> greatest displacement will occur along the<br />

line, or meridian, drawn from the pole through the center <strong>of</strong><br />

mass <strong>of</strong> the icecap and so around the earth; or, if any unex-<br />

pected factor should deflect the direction <strong>of</strong> the movement,<br />

the greatest displacement will occur along whatever meridian<br />

represents the direction <strong>of</strong> the movement. As I have pointed<br />

out, at two pivot points on the equator 90 degrees away from<br />

this meridian there will be little or no movement, and the<br />

points in between will move proportionately to their distances<br />

from the meridian. <strong>The</strong> tension, or stretching, will be<br />

proportional to the amount <strong>of</strong> displacement. It therefore will<br />

be greatest along the central meridian <strong>of</strong> movement, and it<br />

is here that Mr. Campbell expects the first major fractures<br />

<strong>of</strong> the crust to develop.<br />

It is important to visualize the nature <strong>of</strong> the crust on which<br />

this tension is exerted. <strong>The</strong> crust is comparatively rigid, hav-<br />

ing little elasticity, but it is not strong. It varies in thickness<br />

and strength from place to place. As we shall see, it is even<br />

now penetrated <strong>by</strong> great systems <strong>of</strong> deep fractures <strong>of</strong> unex-<br />

plained origin. <strong>The</strong>se inequalities <strong>of</strong> strength will be very<br />

important in determining the reactions <strong>of</strong> the crust from<br />

place to place to the tension exerted upon it; they<br />

will de-

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