Toomre and Toomre, 1972

In Galactic Bridges and Tails, Toomre and Toomre (hereafter, TT) considered encounters between pairs of galaxies on parabolic orbits; each galaxy was idealized as just a disk of noninteracting test particles initially in orbit about a central mass points. As a result, all explicit self gravity of the disk was neglected; this was justified on two grounds:

TT modeled 4 interacting systems - Arp 295, M51 and NGC 5195, NGC 4676 and NGC 4038/9 - but it was their reconstuction of the ``Antennae'' that gave them ``the most pleasure'', despite using a highly idealized model. This stemmed from prior concerns regarding whether ``it was possible to obtain seemingly crossed tails from tidal interactions''.

Survey of Tails

In section IV of TT, Survey of Tails, it is noted that ``proper tail making in the sense of escape to infinity of particles from the antitidal side of a victim disk requires the perturbing mass to be at least comparable to the perturbed''. Hence, if we observe an interacting system with two prominent tidal tails emanating from the disks of both galaxies then we may conclude that the masses involved were comparable and that the separation at periapse was small. With this assumption in mind, a mass ratio of exactly unity was assumed in a survey of 3 dimensional tails. This suvery was of particular importance for analysis of NGC 4038/9; figure 18 of this section plays a central theme and is shown below.

 figure11

Figure 1: Figure 18 on page 623 of Galactic Bridges and Tails. This is part of the tail survey; in this case, the ellipticity was tex2html_wrap_inline103 for equal mass passages of fixed inclination tex2html_wrap_inline30 but with different orbital arguements of tex2html_wrap_inline107. The viewing time is t=6.086 in their units, corresponding to tex2html_wrap_inline109 of orbit travel since pericenter. The viewing angles are normal and edge on to the orbit plane; in this case, the edge on views are from directions which exactly superpose the centers of victim and satellite.

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Figure 2: Figure 18 on page 624 of Galactic Bridges and Tails.

The Antennae, NGC 4038/9

TT observed that if every bare companion carried an tex2html_wrap_inline30 tail of its own (chosen from amongst the four possibilities after a tex2html_wrap_inline32 visual rotation about the axis normal to the orbital plane), then no tail crossings were to be found in any view that was roughly perpendicular to the orbits. In addition to this, they were able to exclude all other views from near the great circle normal to the line connecting the masses; this was because of the precondition that no part of one tail could be closer to the other than the distance between the hulks themselves.

Views from along the connecting line, however, produce a pair of crossed tails which TT compare to a ``pair of symmetric gull wings''. In this case, they utilised the tex2html_wrap_inline34 tail in figure 18 together with its identical twin attached to the perturbing mass. Similar results are possible for both the tex2html_wrap_inline36 and tex2html_wrap_inline38 cases, and almost the same for either case partnered with tex2html_wrap_inline34 ribbon. The result is illustrated in figure 23 of TT, as shown.

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Figure 3: Figure 23 of Galactic Bridges and Tails. In this instance we see two identical disks of radious 0.75 tex2html_wrap_inline123 which have undergone an tex2html_wrap_inline125 encounter with orbit angles tex2html_wrap_inline127 and arguement at pericenter tex2html_wrap_inline129 that appeared the same to both. The subscripts refer to the galaxies NGC 4038 and NGC 4039 respectively. The upper view is exactly normal to the orbit plane, while the lower view is edge on to the orbit plane with a viewing direction tex2html_wrap_inline131 from the line connecting the two pericenters. The viewing time is at t=15 in their units, just slightly past apocenter.

The precise orbital parameters used in figure 23 were chosen by TT to produce a result in accord with their 1971 NGC 4038/9 movie.

The forces from each massive body were softened gradually at close range by varying the potential at small radius as:

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where tex2html_wrap_inline42 as opposed to the standard tex2html_wrap_inline135. This gravity softening was essential in the mimicing of the mass distribution; if neglected, too many of the near side particles would have been extracted from both of the disks. In addition, this gravity softening facilitated further thinning of the tails.

Model Shortcomings

Whilst the models successfully reproduced the hallmark crossed tails of the ``Antennae'', TT noted several deficiencies:
(1) the real tails are unequal in length.
(2) the actual NGC 4038 tail is more curved than its model counterpart.
(3) the rotation of the real hulks seem to be such that their adjacent ends approach and recede alike; the opposite holds true for the models.
In an attempt to remedy these shortcomings, TT made three suggestions:

Despite the shortcomings, the Toomres captured the essence of the Antennae with a simplified 3-body model, and as they indicated, if further progress was to be made then a full N-Body self consistent code was necessary.


Chris Power, 29th August 1999