TL;DR: In this article, it was shown that there is an upper bound to the energy of the gravitational radiation emitted when one collapsed object captures another, in the case of two objects with equal masses and zero intrinsic angular momenta.
Abstract: It is shown that there is an upper bound to the energy of the gravitational radiation emitted when one collapsed object captures another. In the case of two objects with equal masses $m$ and zero intrinsic angular momenta, this upper bound is $(2\ensuremath{-}\sqrt{2})m$.
TL;DR: In this article, the authors studied the nonlinear evolution of the instability at the event horizon of an extreme Reissner-Nordstrom (RN) black hole and found that generically the endpoint of instability is a non-extreme RN solution, but there exist fine-tuned initial perturbations for which the instability never decays.
Abstract: A massless scalar field exhibits an instability at the event horizon of an extreme black hole. We study numerically the nonlinear evolution of this instability for spherically symmetric perturbations of an extreme Reissner–Nordstrom (RN) black hole. We find that generically the endpoint of the instability is a non-extreme RN solution. However, there exist fine-tuned initial perturbations for which the instability never decays. In this case, the perturbed spacetime describes a time-dependent extreme black hole. Such solutions settle down to extreme RN outside, but not on, the event horizon. The event horizon remains smooth but certain observers who cross it at late time experience large gradients there. Our results indicate that these dynamical extreme black holes admit a C1 extension across an inner (Cauchy) horizon.
TL;DR: In this paper, the effects of the strong gravitational field of a supermassive black hole on small objects, such as a comet or an asteroid, were studied. But the authors focused on the radio source Sagittarius A (Sgr A) at the centre of our Galaxy.
Abstract: The compact radio source Sagittarius A (Sgr A) at the centre of our Galaxy harbours a supermassive black hole, whose mass has been measured from stellar orbital motions. Sgr A is therefore the nearest laboratory where super-massive black hole astrophysics can be tested, and the environment of black holes can be investigated. Since it is not an active galactic nucleus, it also offers the possibility of observing the capture of small objects that may orbit the central black hole. We study the effects of the strong gravitational field of the black hole on small objects, such as a comet or an asteroid. We also explore the idea that the flares detected in Sgr A might be produced by the final accretion of single, dense objects with mass of the order of 10^20 g, and that their timing is not a characteristic of the sources, but rather of the space-time of the central galactic black hole in which they are moving. We find that tidal effects are strong enough to melt the solid object, and present calculations of the temporal evolution of the light curve of infalling objects as a function of various parameters. Our modelling of tidal disruption suggests that during tidal squeezing, the conditions for synchrotron radiation can be met. We show that the light curve of a flare can be deduced from dynamical properties of geodesic orbits around black holes and that it depends only weakly on the physical properties of the source.
TL;DR: In this paper, the geodesic deviation equations for radially falling bodies toward the charged black hole were solved and it was shown that the radial component of the deviation vector starts decreasing inside the event horizon unlike in the Schwarzschild case.
Abstract: We analyze the tidal forces produced in the spacetime of Reissner–Nordstrom black holes. We point out that the radial component of the tidal force changes sign just outside the event horizon if the charge-to-mass ratio is close to 1, unlike in Schwarzschild spacetime of uncharged black holes, and that the angular component changes sign between the outer and inner horizons. We solve the geodesic deviation equations for radially falling bodies toward the charged black hole. We find, for example, that the radial component of the geodesic deviation vector starts decreasing inside the event horizon unlike in the Schwarzschild case.