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The Restless universe | |||||
| Introduction to The restless Universe 1 The lawful Universe2 The clockwork Universe4 The intangible Universe 4.1 Electromagnetism and fields 1/4 4.1 Electromagnetism and fields 2/4 4.1 Electromagnetism and fields 3/4 4.1 Electromagnetism and fields 4/4 4.2 Relativity, space, time and gravity 1/4 4.2 Relativity, space, time and gravity 2/4 » 4.2 Relativity, space, time and gravity 3/44.2 Relativity, space, time and gravity 4/4 -------------------- Other titles in the Physical World series | 4 The intangible Universe 4.2 Relativity,space,time and gravity Part 1 of 4 | Part 2 | Part 3 | Part 4For a printable version of 'The intangible Universe' click here 'Henceforth space by itself, and time by itself, are doomed to fade away into mere shadows, and only a kind of union of the two will preserve an independent reality.' The union of space and time of which Minkowski spoke is now generally referred to as space-time. It represents a kind of melding together of space and time, and since space is three-dimensional, and time is one-dimensional, space-time is four-dimensional. Any particular observer, such as you or I, will divide space-time into space and time, but the way in which that division is made may differ from one observer to another and will crucially depend on the relative motion of the observers. A very rough attempt at representing diagrammatically this change of attitude towards space and time is shown in Figure 1.23 In retrospect, special relativity can be seen as part of a gradual process in which the laws of physics attained universal significance. The earliest attempts to understand the physical world placed Man and the Earth firmly at the centre of creation. Certain laws applied on Earth, but different laws applied in the heavens. Copernicus overturned this Earth-centred view and Newton proposed laws that claimed to apply at all places, and at all times. Special relativity continues this process by insisting that physical laws should not depend on the observer's state of motion - at least so long as that motion is uniform. It is therefore not surprising that Einstein was led to ask if physical laws could be expressed in the same way for all observers, even those who were moving non-uniformly. This was the aim of his general theory of relativity. | Relevant LinksA note on powers of ten and significant figures Suggestions for further reading | |||
| S207 The Physical World | |||||