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350 CONTRIBUTIONS TO SCIENCE<br />

true of the new generalization, which is an attempt <strong>to</strong> <strong>com</strong>prise<br />

the properties of the <strong>to</strong>tal field. In the generalized theory the<br />

procedure of deriving from the premises of the theory conclusions<br />

that Can be confronted with empirical data is so difficult<br />

that so far no such result has been obtained. In favor of this<br />

theory are, at this point, its logical simplicity and its "rigidity."<br />

Rigidity means here that the theory is either true or false, but<br />

not modifiable.<br />

The greatest inner difficulty impeding the development of<br />

the theory of relativity is the dual nature of the problem, indicated<br />

by the two questions we have asked. This duality is the<br />

reason why the development of the theory has taken place in two<br />

steps so widely separated in time. The first of these steps, the<br />

theory of gravitation, is based on the principle of equivalence<br />

discussed above and rests on the following consideration: According<br />

<strong>to</strong> the theory of special relativity, light has a constant<br />

velocity of propagation. If a light ray in a vacuum starts from<br />

a point, desigoated by the coordinates Xl, X, and Xs in a three<br />

dimensional coordinate system, at the time X., it spreads as a<br />

spherical wave and reaches a neighboring point (Xl + dx].,<br />

x, + dx" Xs + dXa) at the time x. + dx,. Introducing the<br />

velocity of light, c, we write the expression:<br />

VdXl' + dx,'+ dxs' = cdx.<br />

This can also be written in the form:<br />

dXl' + dx,' + dx,' - c' dx.' = 0<br />

This expression represents an objective relation between<br />

neighboring space· time points in four dimensions, and it holds<br />

for all inertial systems, provided the coordinate transformations<br />

are restricted <strong>to</strong> those of special relativity. The relation loses<br />

this form, however, if arbitrary continuous transformations of<br />

the coordinates are admitted in accordance with the principle<br />

of general relativity. The relation then assumes the more general<br />

form:<br />

:E g,. dx, dXk = 0<br />

'k<br />

The g'k are certain functions of the coordinates which transform<br />

in a definite way if a continuous coordinate transformation is<br />

applied. According <strong>to</strong> the principle of equivalence, these g ..

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