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Time&Eternity

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146 chapter 3<br />

speak only of space-time? Does Einstein himself draw such a conclusion? In<br />

his presentation of the general theory of relativity, after initial skepticism,<br />

Einstein expresses 165 his admiration for Minkowski’s interpretation of the<br />

special theory of relativity: “The generalization of the theory of relativity<br />

has been greatly facilitated by the form that was given to the special theory<br />

of relativity by Minkowski, the mathematician who first clearly recognized<br />

the formal equivalency of the spatial and time coordinates and used it for<br />

establishing the theory.” 166 Without Minkowski, the general theory of relativity<br />

would have “perhaps remained stuck in infancy.” 167<br />

Elsewhere, however, Einstein expressed himself much more cautiously:<br />

From a formal point of view one may characterize the achievement of the special<br />

theory of relativity thus: it has shown generally the role which the universal constant<br />

c (velocity of light) plays in the laws of nature and has demonstrated that there<br />

exists a close connection between the form in which time on the one hand and the<br />

spatial coordinates on the other hand enter into the laws of nature. 168<br />

He therefore appears to presuppose a difference between space and time<br />

despite their arithmetical unification as coordinates of one and the same<br />

system. Or is this more an emotional assertion of an elderly man rather<br />

than of a scientist? For in “A London Speech,” Einstein says when referring<br />

to Minkowski: “According to the special theory of relativity the four dimensional<br />

continuum formed by the union of space and time retains the absolute<br />

character which, according to the earlier theory, belonged to both<br />

space and time separately.” 169 Mathematically, “no statement is more banal<br />

than that our familiar world is a four-dimensional time-space continuum,”<br />

170 for it can be shown that the laws of nature, which correspond to the<br />

requirements of the theory of relativity, “assume mathematical forms in<br />

which the time coordinate plays exactly the same role as the three spatial coordinates.”<br />

171<br />

How, then, can this loss of autonomy of time and space be understood?<br />

172 Classical physics could allow itself two equally valid interpretations<br />

of a space-time continuum, namely, first as a dynamic concept of positions<br />

that change in time, and, second, as a static concept of movement as<br />

something existing. In the first case, the continuum is broken down into<br />

space and time; in the second, it is viewed as a whole. In classical physics,<br />

the oscillation between the two concepts presents no problem inasmuch as,<br />

according to the idea of absolute time, the time coordinate always remains<br />

the same. When relating to another system, only the space coordinates, but<br />

not the time coordinates, are transformed. Within the special theory of relativity,<br />

on the other hand, a space-time continuum cannot simply be split<br />

into a space and a time dimension, since in two different systems, not only

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