The nature of the physical world / by A.S. Eddington.

  • Eddington, Arthur Stanley, Sir, 1882-1944.
Date:
1928
Catalogue details

Licence: In copyright

Credit: The nature of the physical world / by A.S. Eddington. Source: Wellcome Collection.

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    light as it is a gauge for the rod. The light track is in fact controlled by the curvature in such a way that it is incapable of exposing the sham law of curvature. And so wherever the sun, moon and earth may have got to, the light will not give them away. If the law of curvature predicts an eclipse the light will take such a track that there is an eclipse. The law of gravitation is not a stern ruler controlling the heavenly bodies; it is a kind- hearted accomplice who covers up their delinquencies. I do not recommend you to try to verify from Fig. 6 that the number of rods in >S1E1 (full line) and E2 (dotted line) is the same. There are two dimensions of space-time omitted in the picture besides the extra dimensions in which space-time must be supposed to be bent; more¬ over it is the spherical, not the cylindrical, curvature which is the gauge for the length. It might be an instructive, though very laborious, task to make this direct verification, but we know beforehand that the measured distance of the earth from the sun must be the same for either track. The law of gravitation, ex¬ pressed mathematically by GfJLV=\gflv, means nothing more nor less than that the unit of length everywhere is a constant fraction of the directed radius of the world at that point. And as the astronomer who predicts the future position of the earth does not assume anything more about what the earth will choose to do than is expressed in the law G^v =AgILVf so we shall find the same position of the earth, if we assume nothing more than that the practical unit of length involved in measure¬ ments of the position is a constant fraction of the directed radius. We do not need to decide whether the track is to be represented by EEX or EE2, and it would convey no information as to any observable phenomena if we knew the representation.