Spelling suggestions: "subject:"black home"" "subject:"black hope""
1 |
Extended objects, solitons and Bogomol'nyi boundsLondon, Lee Alexander James January 1994 (has links)
No description available.
|
2 |
Two problems relating to cosmic censorshipNeedham, T. January 1986 (has links)
No description available.
|
3 |
Initial data for axially symmetric black holes with distorted apparent horizonsTonita, Aaryn 05 1900 (has links)
The production of axisymmetric initial data for distorted black holes at a moment
of time symmetry is considered within the (3+1) context of general relativity. The
initial data is made to contain a distorted marginally trapped surface ensuring that,
modulo cosmic censorship, the spacetime will contain a black hole. The resulting
equations on the complicated domain are solved using the piecewise linear finite element method which adapts to the curved surface of the marginally trapped surface.
The initial data is then analyzed to calculate the mass of the space time as
well as an upper bound on the fraction of the total energy available for radiation.
The families of initial data considered contain no more than few percent of the
total energy available for radiation even in cases of extreme distortion. It is shown
that the mass of certain initial data slices depend to first order on the area of the
marginally trapped surface and the gaussian curvature of prominent features.
|
4 |
Anti-de Sitter black holes in supergravityChong, Zhiwei 02 June 2009 (has links)
In this dissertation, we systematically construct non-extremal charged rotating
anti-de Sitter black hole solutions in four, five and seven dimensions. In four dimensions,
we first obtain the rotating Kerr-Taub-NUT metric with four independent
charges, as solutions of N = 2 supergravity coupled to three abelian vector multiplets
by the solution generating technique. Then we generalise the four-dimensional rotating
solutions to the solutions of gauged N = 4 supergravity with charges set pairwise
equal. In five dimensions, the most general charged rotating black hole solution has
three charge and two rotation parameters. We obtain several special cases of the general
solution. To be specific, we obtain the first example of a non-extremal rotating
black hole solution with two independent rotation parameters, which has two charge
parameters set equal and the third vanishing. In another example, we obtain the nonextremal
charged rotating black hole solution with three charge parameters set equal
and non-equal rotation parameters. We are also able to construct the single-charge
solution with two independent rotation parameters. In seven dimensions, we obtain
the solution for non-extremal charged rotating black holes in gauged supergravity, in
the case where the three rotation parameters are set equal. There are two independent
charges, corresponding to gauge fields in the U(1) × U(1) abelian subgroup of
the SO(5) gauge group.
|
5 |
Cosmological environment study of a black hole : A closer look on the science of InterstellarGustafsson, Anton January 2015 (has links)
This report looks closer on the physics of black holes and their related phenomena. Particularly, this report studies a certain black hole called Gargantua that is portrayed in the movie Interstellar. By using this as a source of inspiration we look at Gargantua’s effect on time, planetary orbits and tidalforces. The following report showed that the physics studied here corresponded fully to the physics represented in Interstellar, making the movie very credible from a physics point of view. I show that the black hole portrayed in Interstellar needed to spin at a rate of 1.33*10^-14 percent less than its maximum possible to achieve a timedilation of 61320 at the distance where stable planetary orbits are found. At a spin this high, planets can have stable orbits as close as half the Schwarzschild radius which means they are located just outside the event horizon of a maximally rotating black hole. The enormous timedilation at planets orbiting near the event horizon is a result of the planets close proximity to the black hole, its orbital velocity and frame dragging. Frame dragging describes the effects on spacetime on account of the rotation of the black hole. Looking at the tidal forces on objects surrounding the black hole it was found that an increasing mass would actually decrease the tidal forces on objects outside the event horizon. For a sufficiently large mass on the black hole, a planet could avoid being ripped apart but this restricted its size to a radial extension of about 5500 km which corresponds to 0.86 earth radiuses.
|
6 |
Initial data for axially symmetric black holes with distorted apparent horizonsTonita, Aaryn 05 1900 (has links)
The production of axisymmetric initial data for distorted black holes at a moment
of time symmetry is considered within the (3+1) context of general relativity. The
initial data is made to contain a distorted marginally trapped surface ensuring that,
modulo cosmic censorship, the spacetime will contain a black hole. The resulting
equations on the complicated domain are solved using the piecewise linear finite element method which adapts to the curved surface of the marginally trapped surface.
The initial data is then analyzed to calculate the mass of the space time as
well as an upper bound on the fraction of the total energy available for radiation.
The families of initial data considered contain no more than few percent of the
total energy available for radiation even in cases of extreme distortion. It is shown
that the mass of certain initial data slices depend to first order on the area of the
marginally trapped surface and the gaussian curvature of prominent features.
|
7 |
Initial data for axially symmetric black holes with distorted apparent horizonsTonita, Aaryn 05 1900 (has links)
The production of axisymmetric initial data for distorted black holes at a moment
of time symmetry is considered within the (3+1) context of general relativity. The
initial data is made to contain a distorted marginally trapped surface ensuring that,
modulo cosmic censorship, the spacetime will contain a black hole. The resulting
equations on the complicated domain are solved using the piecewise linear finite element method which adapts to the curved surface of the marginally trapped surface.
The initial data is then analyzed to calculate the mass of the space time as
well as an upper bound on the fraction of the total energy available for radiation.
The families of initial data considered contain no more than few percent of the
total energy available for radiation even in cases of extreme distortion. It is shown
that the mass of certain initial data slices depend to first order on the area of the
marginally trapped surface and the gaussian curvature of prominent features. / Science, Faculty of / Physics and Astronomy, Department of / Graduate
|
8 |
Modified Gravity in Cosmology and Fundamental Particle PhysicsDai, De-Chang 02 April 2008 (has links)
No description available.
|
9 |
A Self-consistent Model of the Black Hole Evaporation and Entropy in Gravity / ブラックホールの蒸発の自己無撞着模型と重力におけるエントロピーYokokura, Yuki 24 March 2014 (has links)
京都大学 / 0048 / 新制・課程博士 / 博士(理学) / 甲第18077号 / 理博第3955号 / 新制||理||1570(附属図書館) / 30935 / 京都大学大学院理学研究科物理学・宇宙物理学専攻 / (主査)教授 川合 光, 准教授 福間 將文, 教授 畑 浩之 / 学位規則第4条第1項該当 / Doctor of Science / Kyoto University / DGAM
|
10 |
Black hole visualization and animationKrawisz, Daniel Gregory 25 October 2010 (has links)
Black hole visualization is a problem of raytracing over curved spacetimes. This paper discusses the physics of light in curved spacetimes, the geometry of black holes, and the appearance of objects as viewed through a relativistic camera (the Penrose-Terrell effect). It then discusses computational issues of how to generate images of black holes with a computer. A method of determining the most efficient series of steps to calculate the value of a mathematical expression is described and used to improve the speed of the program. The details of raytracing over curved spaces not covered by a single chart are described. A method of generating images of several black holes in the same spacetime is discussed. Finally, a series of images generated by these methods is given and interpreted. / text
|
Page generated in 0.144 seconds