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21#
發(fā)表于 2025-3-25 07:01:50 | 只看該作者
22#
發(fā)表于 2025-3-25 09:09:51 | 只看該作者
https://doi.org/10.1007/978-3-476-03524-0axwell’s equations of electromagnetic theory were invariant under Lorentz transformations (and not under Galilean transformations). Observational considerations did not motivate the theory: the null result of the Michelson—Morley experiment followed as a simple deduction from the theory . it was formulated.
23#
發(fā)表于 2025-3-25 15:39:29 | 只看該作者
,Natur als Produkt und Produktivit?t,rates non-Euclidean effects of spacetime geometry which die out as we go away from the object. Thus, far away from the object the spacetime is that of special relativity. Such solutions of Einstein’s equations are said to have boundary conditions implying an . spacetime. We shall discuss such solutions in this chapter.
24#
發(fā)表于 2025-3-25 19:13:14 | 只看該作者
Themenhefte Schwerpunktprogramm Umwelttravelled by light in one year ? 9.460 × 10. cm). This picture suggests that although local inhomogeneities like stars, galaxies, and clusters of galaxies exist, the universe on the large scale is homogeneous. Table 8.1 will help us to visualize the various distance scales involved in astronomy.
25#
發(fā)表于 2025-3-25 21:15:25 | 只看該作者
26#
發(fā)表于 2025-3-26 00:34:42 | 只看該作者
Karl Marx — Natur und Werttheoriehy survey of other approaches to quantum gravity in the previous chapter will have convinced the reader that the problem is not simple, whatever means we may choose to adopt for its solution. We begin, therefore, by looking at the difficulties facing the path integral formalism.
27#
發(fā)表于 2025-3-26 04:56:37 | 只看該作者
Introduction and for a long time to come. The proper description of such a change of course is by the word ‘revolution’. Unlike political revolutions, which came with mixed benefits, the revolutions in physics have invariably led to a dramatically improved understanding of nature.
28#
發(fā)表于 2025-3-26 10:26:57 | 只看該作者
29#
發(fā)表于 2025-3-26 14:13:11 | 只看該作者
Gravitating Massive Objectsrates non-Euclidean effects of spacetime geometry which die out as we go away from the object. Thus, far away from the object the spacetime is that of special relativity. Such solutions of Einstein’s equations are said to have boundary conditions implying an . spacetime. We shall discuss such solutions in this chapter.
30#
發(fā)表于 2025-3-26 17:43:41 | 只看該作者
Relativistic Cosmologytravelled by light in one year ? 9.460 × 10. cm). This picture suggests that although local inhomogeneities like stars, galaxies, and clusters of galaxies exist, the universe on the large scale is homogeneous. Table 8.1 will help us to visualize the various distance scales involved in astronomy.
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