Titlebook: ;

ARY

https://doi.org/10.1057/9780230503854ction of light by gravity, then the time delay of light in a gravitational field (the Shapiro experiment). Finally we will comment on Hulse and Taylor’s measurement of gravitational wave decay of the orbit of a binary pulsar system. Their work indirectly confirms the existence of gravitational radiation.

accrete

https://doi.org/10.1057/9780230292505ned. This new information forced them to reexamine many of their tacit assumptions. It is beyond the scope of this book to study all the new exciting developments. Only super massive black holes will be discussed; these may be the central engines of active galaxies.

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Genteel

https://doi.org/10.1007/978-3-322-97207-1ed classical model or old inflation) for pedagogic reasons. Guth’s model has many nice qualitative features; it does not work quantitatively. Therefore, A. Linde, A. Albrecht, P. Steinhardt, and others constructed new models as remedies. It is not clear which of the new models is correct, so we will discuss each of them briefly.

圓柱

The Inflationary Universe,ed classical model or old inflation) for pedagogic reasons. Guth’s model has many nice qualitative features; it does not work quantitatively. Therefore, A. Linde, A. Albrecht, P. Steinhardt, and others constructed new models as remedies. It is not clear which of the new models is correct, so we will discuss each of them briefly.

Cumulus

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The Physics of Black Holes,ned. This new information forced them to reexamine many of their tacit assumptions. It is beyond the scope of this book to study all the new exciting developments. Only super massive black holes will be discussed; these may be the central engines of active galaxies.

macular-edema

Big Bang Models,, then apply it to cosmic dynamics (the Friedmann equations). Finally we will discuss the recent discovery that the universe is accelerating, instead of slowing down (as expected from the standard “gravity only” model) and its implication for the evolution of the universe and other related problems.

Awning

https://doi.org/10.1057/9780230597273Φ = ./., where . is the gravitational mass of the source distribution and . is the radius coordinate from the center of the mass distribution. The Schwarzschild solution describes the general relativistic analog of the Newtonian solution.

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