Приклади вживання Rotating black hole Англійська мовою та їх переклад на Українською
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Charged rotating black hole acts as a particle accelerator.
It also turned out that the M87 is a rotating black hole.
In brief, a rotating black hole can store a huge amount of energy in its rotation.
The Ergosphere is a region of space-time around a rotating black hole.
Then, in 1971, I proved that any stationary rotating black hole would indeed have such an axis of symmetry.
The presence of an ergosphere may lead to energy losses by a rotating black hole.
The net process is that the rotating black hole emits energetic particles at the cost of its own total energy.
In theory, energy can be extracted from a rotating black hole.
The“negative energy” that rotating black holes produce can be used to accelerate to near-light speeds.
They convinced me that, according to the quantum mechanical uncertainty principle, rotating black holes should create and emit particles.
There are rotating black holes, black holes with electric charge and black holes, including the features of the first two.
This feature can be used to extract energy from a rotating black hole, up to its invariant mass energy, Mc2.
Rotating black holes in astrophysics are a potential source of large amounts of energy and are used to explain energetic phenomena, such as gamma ray bursts.
A steady state solution of Einstein's equations representing a rotating black hole discovered in 1963 by the mathematician Roy Kerr.
Kerr, an Australian mathematician who worked then at the University of Texas(USA),found a complete solution of the equations of the gravitational field for a rotating black hole.
Conventional black holes occur by absorption of matter, and a rotating black hole formed by merging two of these holes. .
He showed that, provided a stationary rotating black hole had an axis of symmetry, like a spinning top, its size and shape would depend only on its mass and rate of rotation.
In both cases, Clarke andSheffield describe how advanced civilizations could extract energy from rotating black holes to meet their energy needs….
This process of removing energy from a rotating black hole was proposed by the mathematician Roger Penrose in 1969, and is called the Penrose process.
The researchers hope to intentionally create more of these long-lived‘quasi-bound' energy states, and under different conditions,to study their implications for rotating black holes.
The possibility of extracting spin energy from a rotating black hole was first proposed by the mathematician Roger Penrose in 1969 and is thus called the Penrose process.
In this article, the programmers and physicists published the basic equations they used tocreate a program describing the spread of light near a rotating black hole(as in the movie Interstellar).
Rotating black holes have surfaces where the metric appears to have a singularity; the size and shape of these surfaces depends on the black hole's mass and angular momentum.
Objects between these two horizons must co-rotate with the rotating body, as noted above;this feature can be used to extract energy from a rotating black hole, up to its invariant mass energy, Mc2.
While it is expected that the exteriorregion of the Kerr solution is stable, and that all rotating black holes will eventually approach a Kerr metric, the interior region of the solution appears to be unstable, much like a pencil balanced on its point.
For the first time in history, the gravitational wave succeededfix by scientists from the LIGO/ VIRGO experiment collaboration- space-time oscillations have resulted from the merging of two black holes andthe emergence of one supermassive rotating black hole.
While it is expected that the exteriorregion of the Kerr solution is stable, and that all rotating black holes will eventually approach a Kerr metric, the interior region of the solution appears to be unstable, much like a pencil balanced on its point.[22][11] This is related to the idea of cosmic censorship.
A rotating black hole has the same static limit at its event horizon but there is an additional surface outside the event horizon named the"ergosurface" given by( r- M) 2= M 2- J 2 cos 2 θ{\displaystyle( r-M)^{ 2}= M^{ 2}- J^{ 2}\ cos^{2}\theta} in Boyer- Lindquist coordinates, which can be intuitively characterized as the sphere where"the rotational velocity of the surrounding space" is dragged along with the velocity of light.