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for events whose physical characters are unknown. Thus the spatio-temporal measurements are independent of the objectival physical characters. Furthermore the character of our knowledge of a whole duration, which is essentially derived from the significance of the part within the immediate field of discrimination, constructs it for us as a uniform whole independent, so far as its extension is concerned, of the unobserved characters of remote events. Namely, there is a definite whole of nature, simultaneously now present, whatever may be the character of its remote events. This consideration reinforces the previous conclusion. This conclusion leads to the assertion of the essential uniformity of the momentary spaces of the various time-systems, and thence to the uniformity of the timeless spaces of which there is one to each time-system. The analysis of the general character of observed nature set forth above affords explanations of various fundamental observational facts: ({alpha}) It explains the differentiation of the one quality of extension into time and space. ({beta}) It gives a meaning to the observed facts of geometrical and temporal position, of geometrical and temporal order, and of geometrical straightness and planeness. ({gamma}) It selects one definite system of congruence embracing both space and time, and thus explains the concordance as to measurement which is in practice attained. ({delta}) It explains (consistently with the theory of relativity) the observed phenomena of rotation, _e.g._ Foucault's pendulum, the equatorial bulge of the earth, the fixed senses of rotation of cyclones and anticyclones, and the gyro-compass. It does this by its admission of definite stratifications of nature which are disclosed by the very character of our knowledge of it. ({epsilon}) Its explanations of motion are more fundamental than those expressed in ({delta}); for it explains what is meant by motion itself. The observed motion of an extended object is the relation of its various situations to the stratification of nature expressed by the time-system fundamental to the observation. This motion expresses a real relation of the object to the rest of nature. The quantitative expression of this relation will vary according to the time-system selected for its expression. This theory accords no peculiar character to light beyond that accorded to other physical phenomena such as sound. There is no ground for such a dif
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