|
other query modes : |
Identifier query |
Coordinate query |
Criteria query |
Reference query |
Basic query |
Script submission |
TAP |
Output options |
Object types |
Help |
| Query : 2012MNRAS.422.2444S |
2012MNRAS.422.2444S - Mon. Not. R. Astron. Soc., 422, 2444-2464 (2012/May-3)
The symmetries and scaling of tidal tails in galaxies.
STRUCK C. and SMITH B.J.
Abstract (from CDS):
In the simplest case of an impulsive collision yielding a purely tidal disturbance the resulting tidal tails have simple structure. Scalings for their maximum lengths and other characteristics as non-linear functions of the tidal amplitude and the exponent of the power-law potentials are described. The analytic model shows that azimuthal caustics (orbit crossing zones of high density also seen in numerical models) are produced generically in these tails at a fixed azimuth relative to the point of closest approach. Long tails, with high-order caustics at their base, and ocular waveforms are also produced at larger amplitudes.
The analysis is then extended to non-linear disturbances and multiple encounters, which break the symmetries of purely tidal perturbations. The p-ellipse orbital solutions are similar to those in the linear tidal case. However, as the strength of the non-linear terms is varied the structure of the resulting forms varies from symmetric tails to one-armed plumes. Cases with two or more impulse disturbances are also considered as the simplest analytic models distinguishing between prograde and retrograde encounters. The model shows explicitly how tail growth differs in the two cases. In the prograde case a specific mechanism for the formation of tidal dwarf galaxies at the end of tails is suggested as a consequence of resonance effects in multiple or prolonged encounters. Qualitative comparisons to Arp Atlas systems suggest that the limiting analytic cases are realized in real systems. For example, we identify a few Arp systems which have multiple tidal strands meeting near the base of long tails. These may be swallowtail caustics, where dissipative gas streams are converging and triggering star formation. Ultraviolet and optical images reveal luminous knots of young stars at these `hinge clump' locations.
Abstract Copyright: 2012 The Authors Monthly Notices of the Royal Astronomical Society2012 RAS
Journal keyword(s): galaxies: evolution - galaxies: interactions - galaxies: spiral
Simbad objects: 37
| Number of rows : 37 |
| N | Identifier | Otype |
ICRS (J2000) RA |
ICRS (J2000) DEC |
Mag U | Mag B | Mag V | Mag R | Mag I | Sp type |
#ref
1850 - 2026 |
#notes |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 1 | APG 65 | IG | 00 21.9 | +22 23 | ~ | 17 | 0 | |||||
| 2 | IC 18 | EmG | 00 28 34.951 | -11 35 12.30 | 15 | 16.34 | ~ | 29 | 0 | |||
| 3 | IC 167 | GiP | 01 51 08.56 | +21 54 46.1 | 14.0 | ~ | 101 | 0 | ||||
| 4 | NGC 1097 | LIN | 02 46 19.059 | -30 16 29.68 | 10.46 | 9.97 | 9.48 | 8.72 | 9.8 | ~ | 1448 | 3 |
| 5 | UGC 2320 | IG | 02 50 10.66 | +12 52 50.4 | 15.2 | ~ | 24 | 0 | ||||
| 6 | APG 179 | EmG | 03 02 00.4114434600 | -04 41 26.041334100 | 16.12 | 14.89 | ~ | 18 | 0 | |||
| 7 | Z 362-30 | GiP | 07 02 27.5177506800 | +86 34 46.222523364 | 15.6 | ~ | 26 | 1 | ||||
| 8 | NGC 2535 | GiG | 08 11 13.484 | +25 12 24.97 | 13.5 | 12.60 | ~ | 185 | 0 | |||
| 9 | APG 82 | PaG | 08 11 14.0 | +25 12 25 | ~ | 146 | 0 | |||||
| 10 | NGC 2523 | AG? | 08 15 00.1388949576 | +73 34 44.302765908 | 12.4 | ~ | 95 | 0 | ||||
| 11 | Z 89-40 | AGN | 08 31 57.6488660112 | +19 12 41.504563224 | 14.9 | ~ | 39 | 0 | ||||
| 12 | NGC 2633 | GiG | 08 48 04.6279110889 | +74 05 55.032130996 | 12.4 | ~ | 176 | 1 | ||||
| 13 | APG 285 | GrG | 09 24.1 | +49 13 | ~ | 55 | 0 | |||||
| 14 | NGC 3068 | IG | 09 58 40.0900038984 | +28 52 39.105926688 | 15.1 | 14.05 | ~ | 33 | 0 | |||
| 15 | NGC 3189 | GiP | 10 18 05.643 | +21 49 54.98 | 12.60 | 12.12 | 11.15 | 11.14 | ~ | 422 | 2 | |
| 16 | NGC 3561 | LIN | 11 11 13.1887412409 | +28 41 47.044176908 | 14.7 | ~ | 202 | 2 | ||||
| 17 | MCG+10-17-005 | IG | 11 28 45.8500774416 | +58 35 36.676808628 | 16 | 16.10 | ~ | 16 | 1 | |||
| 18 | NGC 3718 | Sy2 | 11 32 34.8571790688 | +53 04 04.520222040 | 11.35 | 10.61 | ~ | 408 | 1 | |||
| 19 | NGC 3800 | GiC | 11 40 13.51680 | +15 20 32.4920 | 13.1 | ~ | 111 | 1 | ||||
| 20 | NGC 4016 | AG? | 11 58 29.02511 | +27 31 43.6086 | 14.6 | ~ | 79 | 0 | ||||
| 21 | NGC 4676 | IG | 12 46 10.18 | +30 43 53.7 | 14.1 | ~ | 318 | 0 | ||||
| 22 | APG 33 | IG | 13 37.6 | +06 26 | ~ | 3 | 0 | |||||
| 23 | APG 240 | PaG | 13 39 55.06 | +00 50 06.4 | 12.6 | ~ | 158 | 0 | ||||
| 24 | APG 84 | IG | 13 58 34.30 | +37 27 10.9 | ~ | 147 | 0 | |||||
| 25 | NGC 5566 | AG? | 14 20 19.94760 | +03 56 00.9240 | 11.91 | 11.46 | 10.55 | ~ | 193 | 2 | ||
| 26 | UGC 9503 | IG | 14 45 26.3385071664 | +19 27 56.453916852 | 15.00 | ~ | 35 | 0 | ||||
| 27 | APG 173 | IG | 14 51 28.8 | +09 19 38 | ~ | 12 | 0 | |||||
| 28 | UGC 10033 | IG | 15 46 56.1 | +17 52 42 | ~ | 118 | 0 | |||||
| 29 | APG 101 | IG | 16 04.5 | +14 52 | ~ | 7 | 0 | |||||
| 30 | VV 29 | IG | 16 06 03.9082292784 | +55 25 31.588100688 | 15.0 | ~ | 122 | 0 | ||||
| 31 | GCl 38 | GlC | 16 10 59.00 | +14 57 42.0 | ~ | 399 | 0 | |||||
| 32 | APG 293 | G | 16 58 27.8 | +58 56 48 | ~ | 115 | 0 | |||||
| 33 | Z 252-40 | Bla | 17 19 14.4925971408 | +48 58 49.423205136 | 15.86 | 14.81 | 9.44 | ~ | 335 | 1 | ||
| 34 | GCl 111 | GlC | 19 18 02.10 | +18 34 18.0 | ~ | 138 | 0 | |||||
| 35 | NGC 7252 | AGN | 22 20 44.7748209648 | -24 40 41.909518200 | 12.26 | 12.46 | 12.06 | 11.57 | ~ | 720 | 1 | |
| 36 | NGC 7550 | LIN | 23 15 16.0635618785 | +18 57 41.255155052 | 13.9 | 11.85 | ~ | 133 | 1 | |||
| 37 | MCG-01-60-021 | LIN | 23 41 47.285 | -03 40 01.90 | 14.88 | 14.50 | 13.57 | ~ | 95 | 1 |
To bookmark this query, right click on this link: simbad:objects in 2012MNRAS.422.2444S and select 'bookmark this link' or equivalent in the popup menu