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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 373<br />

surface. A high plateau may represent an area <strong>of</strong> deficient<br />

mass, and an ocean basin may represent an area <strong>of</strong> excess<br />

mass. We have seen that there are many oceanic areas that<br />

show positive isostatic anomalies, or the existence <strong>of</strong> local<br />

excesses <strong>of</strong> mass in the earth's crust. We can easily see the<br />

distinction between the level equipotential surface <strong>of</strong> the<br />

geoid, represented <strong>by</strong> sea level, and the surface <strong>of</strong> mass that<br />

may deviate considerably from the level surface.<br />

<strong>The</strong> mechanism for crust displacement presented in this<br />

book depends upon recognition <strong>of</strong> the fact that distortions <strong>of</strong><br />

mass on the earth's surface, <strong>of</strong> whatever if<br />

type, they consti-<br />

tute anomalous additions <strong>of</strong> mass at points on the earth's<br />

surface, will give rise to centrifugal effects like the effect <strong>of</strong><br />

the mass attached to the surface <strong>of</strong> Brown's rotating model<br />

sphere, in accordance with ordinary principles <strong>of</strong> mechanics,<br />

and measurable <strong>by</strong> the standard formula for calculating<br />

centrifugal effects.<br />

An example may serve to illustrate the difference between<br />

the surface <strong>of</strong> mass, which differs in elevation from place to<br />

place, and the equipotential, geoidal surface. Let us take a<br />

fictional case <strong>of</strong> a mass out <strong>of</strong> isostatic adjustment but with<br />

its center <strong>of</strong> gravity below the surface <strong>of</strong> the geoid. Let us<br />

that under the bottom <strong>of</strong> the Atlantic Ocean we<br />

suppose<br />

have a slab <strong>of</strong> material ten times as dense as basalt, two thou-<br />

sand miles long, one thousand miles wide, and forty miles<br />

thick. <strong>The</strong> excess <strong>of</strong> mass in this slab, as compared with other<br />

sectors <strong>of</strong> the crust, would be enormous, and gravity would<br />

be greater at the surface. Consequently, the ocean level over<br />

this area would be affected slightly, but the shape <strong>of</strong> the geoid<br />

would not be significantly changed, and the sea level would<br />

still represent an equipotential surface. <strong>The</strong> center <strong>of</strong> grav-<br />

ity <strong>of</strong> the anomalous mass <strong>of</strong> high density would be depressed<br />

far below sea level; it might be fifteen or twenty miles below<br />

the geoidal surface. Now if the slab were <strong>of</strong> average density,<br />

the depression <strong>of</strong> the center <strong>of</strong> gravity would mean an in-<br />

verse Eotvos effect, that is, a poleward centrifugal effect, the<br />

quantity <strong>of</strong> which, as we have seen, would be slight. But, now,

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