Oxford Art Online 2003
DOI: 10.1093/gao/9781884446054.article.t079169
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Slavkov u Brna

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Cited by 3 publications
(4 citation statements)
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“…The total masses of the LMC and the SMC are 1.0 × 10 10 M ⊙ and 3.0 × 10 9 M ⊙ , respectively. These values were based on those derived from the latest observations (e.g., Kroupa & Bastian 1997;van der Marel et al 2002) and consistent with previous simulations (e.g., Gardiner & Noguchi 1996). In the Clouds' orbital calculations with the backward integration scheme (Gardiner et al 1994), we assume that the current space velocities (V x , V y , V z ) (or (U, V, W )) in units of km s −1 are (−5, −225, 194) and (40, −185, 171).…”
Section: Discussionsupporting
confidence: 87%
“…The total masses of the LMC and the SMC are 1.0 × 10 10 M ⊙ and 3.0 × 10 9 M ⊙ , respectively. These values were based on those derived from the latest observations (e.g., Kroupa & Bastian 1997;van der Marel et al 2002) and consistent with previous simulations (e.g., Gardiner & Noguchi 1996). In the Clouds' orbital calculations with the backward integration scheme (Gardiner et al 1994), we assume that the current space velocities (V x , V y , V z ) (or (U, V, W )) in units of km s −1 are (−5, −225, 194) and (40, −185, 171).…”
Section: Discussionsupporting
confidence: 87%
“…We base the parameter values of the LMC/SMC orbital properties on the early numerical simulations of Gardiner & Noguchi (1996), which are not only consistent with the observed location and radial velocity of the LMC/SMC system but are also successful in reproducing the observed physical properties of the Magellanic stream. The orbital parameters in the present study (and thus in Gardiner & Noguchi 1996) are broadly consistent with the Hipparcos data of Kroupa & Bastian (1997), as shown by Yoshizawa & Noguchi (2003). Therefore, the adopted parameter values can be regarded as reasonable, although the exact orbital properties of the LMC/SMC system have not been observationally determined (thus, the orbital parameters should be still free parameters).…”
Section: Tidal Interaction In the Lmc/smc Systemsupporting
confidence: 87%
“…We calculated the ASPF for the LMC using the Jones et al (1994) proper motion, however their reduction of this proper motion to an absolute reference frame was complicated by the unknown amount of rotation of the stars around the center of the LMC. If we instead calculate the ASPF using the Jones et al (1994) LMC proper motion corrected for the estimated amount of rotation in the field or with the Kroupa & Bastian (1997) LMC proper motion, we find that the ASPF in either of these cases lies almost entirely in the northern Galactic hemisphere, indicating that for the LMC, L z is positive, and opposite that of the SMC and Ursa Minor. However, since these objects are all on nearly polar orbits and are in the outer halo where the potential is more nearly spherical, the difference in the sign of L z may not be meaningful.…”
Section: Dynamical Groupsmentioning
confidence: 76%
“…We have followed the recommendation of Dinescu et al (1999b) on the proper motion of NGC 362 and adopt the Tucholke (1992b) proper motion of this object, which is calculated relative to SMC stars. However, Dinescu et al (1999b) derives an absolute proper motion for NGC 362 by correcting for the SMC's proper motion using the Kroupa & Bastian (1997) measurement. The corrected ASPF has a center more than 50 • from the center of the uncorrected proper motion's pole family.…”
Section: Pole Families From Independent Proper Motion Measurementsmentioning
confidence: 99%