A Prograde Gravitational Capture Model for a Sizeable Volcanoid Planetoid (or Asteroid) for Mars

2020 ◽  
pp. 75-104
Author(s):  
Robert Malcuit
2008 ◽  
Vol 391 (2) ◽  
pp. 675-684 ◽  
Author(s):  
R. A. N. Araujo ◽  
O. C. Winter ◽  
A. F. B. A. Prado ◽  
R. Vieira Martins

2018 ◽  
Vol 14 (S343) ◽  
pp. 416-418
Author(s):  
Jeong-Eun Heo ◽  
Hee-Won Lee ◽  
Rodolfo Angeloni ◽  
Tali Palma ◽  
Francesco Di Mille

AbstractWe present a high-resolution optical spectrum of the symbiotic nova RR Tel obtained with MIKE at Magellan-Clay telescope. RR Tel is a wide binary system of a hot white dwarf and a Mira with an orbital period of a few decades, where the white dwarf is accreting through gravitational capture of some fraction of material shed by the Mira. We find broad emission features at 6825, 7082, 7023, and 7053 Å, which are formed through Raman scattering of far-UV O VI ⋋⋋ 1032 and 1038 Å, C II ⋋⋋ 1036 and 1037 Å with atomic hydrogen. Raman O VI features exhibit clear double-peak profiles indicative of an accretion flow with a characteristic speed ∼ 30 km s−1, whereas the Raman C II features have a single Gaussian profile. We perform a profile analysis of the Raman O VI by assuming that O VI emission traces the accretion flow around the white dwarf with a fiducial scale of 1 AU. A comparison of the restored fluxes of C II ⋋⋋ 1036 and 1037 from Raman C II features with the observed C II ⋋ 1335 multiplet is consistent with the distance of RR Tel ∼ 2.6 kpc based on interstellar extinction of C II.


1998 ◽  
Vol 07 (06) ◽  
pp. 957-967 ◽  
Author(s):  
JEAN-PIERRE DE VILLIERS ◽  
VALERI FROLOV

The gravitational interaction of an infinitely long cosmic string with a Schwarzschild black hole is studied. We consider a straight string that is initially at a great distance and moving at some initial velocity v (0 < v < c) towards the black hole. The equations of motion of the string are solved numerically to obtain the dependence of the capture impact parameter on the initial velocity.


2015 ◽  
Vol 55 (2) ◽  
pp. 668-681 ◽  
Author(s):  
P.I.O. Brasil ◽  
A.F.B.A. Prado ◽  
R. Deienno ◽  
T. Yokoyama

2003 ◽  
Vol 26 (4) ◽  
pp. 635-642
Author(s):  
Scott R. Dahlke

Universe ◽  
2021 ◽  
Vol 7 (8) ◽  
pp. 307
Author(s):  
Bobomurat Ahmedov ◽  
Ozodbek Rahimov ◽  
Bobir Toshmatov

We study the capture cross-section of massless (photon) and massive test particles by the Schwarzschild–Tangherlini black hole, which is a solution of pure general relativity in higher dimensional spacetime with R×SD−2 topology. It is shown that an extra dimension weakens the gravitational attraction of a black hole, and consequently, radii of all the characteristic circular orbits, such as the radius of a photonsphere decrease in the higher dimensions. Furthermore, it is shown that in higher dimensions, there are no stable and bounded circular orbits. The critical impact parameters and capture cross-sections of photons and massive particles are calculated for several higher dimensions and it is shown that they also decrease with increasing dimension. Moreover, we calculate the capture cross-section of relativistic and non-relativistic test particles in the higher dimensions..


Author(s):  
Prasenjit Saha ◽  
Paul A. Taylor

Astronomy and recording of the motion of celestial objects are ancient practices, but what is now called astrophysics arguably began with Newtonian gravity and the concept of orbits as dynamical phenomena. This chapter provides a modern perspective on the early problems of gravitational dynamics, from Kepler’s laws up to the virial theorem for an arbitrary number of gravitating bodies. Even a simple gravitating system with only two bodies turns out to have many interesting features, such as the gravitational capture of material by protoplanets. The study of orbital motions also includes applications to observing extrasolar planets and stars near the black hole at the centre of the Milky Way.


1980 ◽  
Vol 90 ◽  
pp. 199-204
Author(s):  
E.N. Kramer ◽  
V.I. Musiy ◽  
E.A. Timchenko-Ostroverkhova ◽  
I.S. Shestaka

The radius for gravitational capture of meteoroids by the Earth is where R is the Earth's radius, h is the height where marked deceleration of meteor bodies begins, α0 is the average distance of the Earth from the Sun, v∞ and vg are preatmospheric and geocentric (undisturbed) velocities of the body.


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