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Underground Rivers - University of New Mexico

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Chapter 14 -- Hollow Earth Geophysics<br />

Such <strong>New</strong>tonian quibbling would not have phased Symmes,<br />

however, as according to J. McBride's Symmes's Theory <strong>of</strong><br />

Concentric Spheres; Demonstrating that the Earth Is Hollow,<br />

Habitable Within, and Widely Open about the Poles (1826),<br />

gravity is not an attractive force related to mass, but rather a<br />

pushing force (a pressure in modern terminology) exerted by<br />

a universal ether.<br />

DRAFT 1122//66//22001122<br />

Case 6: The pressure <strong>of</strong> ehter<br />

The hollow earth can be dismissed by any number <strong>of</strong> physical arguments, but our observation is<br />

suffice. Everywhere on the earth objects fall straight downward with the same acceleration. We<br />

can't say that we've proven the gravitational earth theory to be correct, but we can say that we've<br />

proven Teed's hollow earth theory to be incorrect.<br />

Symmes and Teed were not alone, however, in their application <strong>of</strong> alternative physics to<br />

problems <strong>of</strong> fluid flow. Although the paper was written to establish why springs emit from outsideworld<br />

-- as opposed to inside-world -- mountaintops -- the higer, the better, actually -- we see like<br />

confusion in "Why Do Springs and Wells Overflow?" Popular Science, November 1879, by<br />

Nelson W. Green.<br />

Here's the essence <strong>of</strong> the pro<strong>of</strong> with items colored to<br />

assist quick identification.<br />

Let aaa, be a great circle <strong>of</strong> the earth attained by<br />

passing a plane through the earth's center C,<br />

perpendicular to its axis, and bbb, the circle cut by<br />

the same plane through the inner surface <strong>of</strong> the<br />

earth's supposed crust. In order to obtain room for<br />

the illustration, this section is exaggerated.<br />

Let the line AB represent the force <strong>of</strong> gravity, and<br />

AE the centrifugal force at the point A, which will<br />

operate in the direction <strong>of</strong> the tangent AG. These<br />

two forces, for the purposes <strong>of</strong> this discussion,<br />

may be assumed to be equal, as the question <strong>of</strong><br />

their relative intensities does not enter into the<br />

problem.<br />

Erect upon the lone AB the square ABCD and draw the diagonal AD produced to F. By a wellknown<br />

law we shall have AD representing the resultant <strong>of</strong> the forces <strong>of</strong> AB and AE -- that is,<br />

the line AD will represent the direction <strong>of</strong> AF, and the intensity <strong>of</strong> the resultant <strong>of</strong> the force <strong>of</strong><br />

gravity and centrifugal force acting at the point A.<br />

It will be observed that since the diagonal <strong>of</strong> either square or <strong>of</strong> a parallelogram is longer than<br />

either <strong>of</strong> its sides, the resultant AD will have a greater intensity than gravity represented by AB.<br />

Now suppose the point A' to be some point inside the earth's crust, and some distance form the<br />

surface, and suppose that it is a particle <strong>of</strong> water in a body <strong>of</strong> water imprisoned by surrounding<br />

rocks. This particle will be acted upon by a continual impulse to move in the direction <strong>of</strong> A'F'',<br />

Uppddaatteess aatt hhttttpp::////www. .uunnm. .eedduu//~rrhheeggggeenn//UnnddeerrggrroouunnddRi ivveerrss. .hhttml l<br />

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