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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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CAMPBELL'S MECHANISM 341<br />

will overcome the inertia <strong>of</strong> the crust and its friction with<br />

the layer below it, to continue the displacements to distances<br />

<strong>of</strong> the order <strong>of</strong> several thousand miles. It is essential to have<br />

a force that will not be absorbed and exhausted <strong>by</strong> the work<br />

<strong>of</strong> moving the crust. It is clear that the mechanism <strong>of</strong> cen-<br />

trifugal effect postulated <strong>by</strong> Campbell can meet this requirement<br />

because the effect increases in proportion as the<br />

uncompensated mass <strong>of</strong> the is icecap moved farther from the<br />

axis <strong>of</strong> rotation. At the same time, as I have already men-<br />

tioned, a cause <strong>of</strong> displacement is called for that will cease to<br />

exert these centrifugal effects at some distance from the pole,<br />

but long before the equator is reached. To accomplish this,<br />

the mechanism must provide that the mass responsible for<br />

the displacement must itself disappear en route, and, as we<br />

have seen, it must disappear rapidly.<br />

It seems that the melting<br />

<strong>of</strong> the icecap, as the movement brings it into warmer<br />

latitudes, provides not only a sufficient but perhaps the only<br />

conceivable method <strong>of</strong> explaining the facts.<br />

Campbell has made this clear <strong>by</strong> computing the increase<br />

<strong>of</strong> the centrifugal effect with increasing distance from the axis<br />

for the present Antarctic icecap, assuming it to be uncom-<br />

pensated, and assuming its displacement, without melting,<br />

as far as the equator. He has shown (Table III, opposite p.<br />

341, and Figure XII, p. 343) that if the icecap should be displaced<br />

as far as the 45th parallel <strong>of</strong> South Latitude, the<br />

tangential component <strong>of</strong> its centrifugal effect would be mul-<br />

tiplied about six times. After this point,<br />

centrifugal effect operating at right angles<br />

while the total<br />

to the axis con-<br />

tinues to increase until the equator is reached, the tangential<br />

component declines, and yet it is clear that the movement,<br />

if the uncompensated mass itself remains intact, must con-<br />

tinue to the vicinity <strong>of</strong> the equator itself. <strong>The</strong> geological<br />

evidence already presented shows that this did not occur, but<br />

that the movements terminated at points about one third <strong>of</strong><br />

the distance from the pole to the equator.<br />

In view <strong>of</strong> the apparently inescapable logic <strong>of</strong> the geological<br />

evidence and <strong>of</strong> the centrifugal mechanics, we must

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