Abstract
In this chapter we shall construct models of stars, both static and dynamical ones, including a model of gravitational collapse. We will restrict ourselves to situations in which rotational symmetry is a reasonable approximation. Much of our attention will be focused on the so-called Schwarzschild solutions. These are rotationally symmetric solutions of the Einstein equations. Studying these solutions has led to significant insights into gravity which are still relevant today.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
Preview
Unable to display preview. Download preview PDF.
References
B. Schutz, Gravity from the Ground up, Cambridge University Press, Cambridge, UK, 2003.
Beig, R., Schmidt B. G.: Einstein’s Field Equations and their Physical Implications. Lect. Notes Phys. 540, Springer, Berlin (2000)
J. R. Oppenheimer and G. M. Volkov, Phys. Rev. 55 (1939) 374.
S. W. Hawking and G. F. R. Ellis, The Large Scale Structure of Space-Time, Cambridge University Press, Cambridge, UK, 1973.
A. S. Eddington, Nature 113 (1924) 192; D. Finkelstein, Phys. Rev.110 (1958) 965.
C. W. Misner, K. S. Thorne and J. A. Wheeler, Gravitation, Freeman, San Francisco, CA, 1973.
R. Schödel et al., Astrophys. J. 596 (2003) 1015.
A. M. Ghez et al., arXiv astro-ph/ 0306130.
J. R. Oppenheimer and H. Snyder, Phys. Rev. 56 (1939) 455.
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
Copyright information
© 2008 Springer-Verlag Berlin Heidelberg
About this chapter
Cite this chapter
Hájíček, P. (2008). Rotationally Symmetric Models of Stars. In: An Introduction to the Relativistic Theory of Gravitation. Lecture Notes in Physics, vol 750. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-78659-7_6
Download citation
DOI: https://doi.org/10.1007/978-3-540-78659-7_6
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-540-78658-0
Online ISBN: 978-3-540-78659-7
eBook Packages: Physics and AstronomyPhysics and Astronomy (R0)