Efforts on 1937 UB "Hermes", a long-lost Apollo Asteroid, rediscovered in 2003, now numbered: (69230) Hermes

      by  Lutz D. Schmadel, Astron.Rechen-Institut, Heidelberg, Germany,
                                  s21@ix.urz.uni-heidelberg.de
      and Joachim Schubart, Astron.Rechen-Institut, Heidelberg, Germany,
                                  s24@ix.urz.uni-heidelberg.de

Index

Remark. Unchanged text of Sept.2000 (sections 1, 2) or Dec.2001 (section 3)

1. The present situation
2. Some more recent measurements of trails
3. Orbits of variation and search lines

Note. Section 3 is maintained, since trails of Hermes happened to appear close to both the search lines derived for 2001 and 2003, although the real orbit of Hermes does not correspond to the orbits used in the derivation.

The present situation (text written in Sept.2000)

Reinmuth discovered 1937 UB Hermes on 1937 Oct. 28.9 UT. The object had left long trails on two simultaneous exposures by the Bruce Astrograph at Heidelberg. Direct attempts to get further positions failed, but trails of Hermes were found on plates exposed at Oak Ridge (Oct.25.2), Johannesburg (Oct.27.9), and Sonneberg (sky patrol plates Oct.26.9 - 29.9). MPC 5971 of May 1981 gives a list of the positions. Due to the short arc and the proximity to the earth a reliable determination of the orbit is impossible, but the effects of daily parallax allow a qualitative derivation: Brian G. Marsden published a best fit to the observations in MPC 3014 of Oct. 1969. Since the resulting orbital period is too uncertain, a prediction of the position of Hermes in its orbit is not possible. There are no known observations of Hermes from the years after 1937.

Nevertheless, we have found it interesting to do some work on the observations and on possible variations of the orbit of Hermes. Unfortunately, most of the basic plates with trails of Hermes are missing in the respective collections of plates. This is true for the better one of the pair of the discovery plates, for the Johannesburg plates, and for the four Sonneberg patrol plates with published positions. The Oak Ridge plate of 1937 Okt. 25.2 is available in the plate collection of Harvard Observatory. Only a provisional position of moderate accuracy was derived from this plate in 1937 by L.E.Cunningham. In 1994 Gareth Williams looked at this plate and found the trail of Hermes, but it is very faint and the ends of the trail are very ill-defined, the trail seems to be involved with a star near one end (personal communication by Brian G. Marsden). Apparently it is not possible to improve Cunningham's position. The published positions from Sonneberg refer to four subsequent nights, but due to the very short focal length of the patrol cameras, and to the imperfect way of guiding during the exposure, these positions are inaccurate. Marsden omitted them in his best fit mentioned above.

Some more recent measurements of trails of Hermes

The missing Sonneberg plates that correspond to the published positions of the four nights Oct. 26.9 - 29.9 were exposed for about half an hour at a Tachar camera. The plate centers, 2h;+10d in the first two and 1h;+10d in the last two cases, were favorable for catching trails of Hermes. However, due to the distances from the centers, large optical distortions have affected the trails and the stellar images, in addition to the disadvantages mentioned above. Fortunately, a photographic copy on paper is still available for the last of these plates, T2499 of Oct.29.9. The paper copy is enlarged by a factor of 3.3 and covers the part of the plate with the trail. The enlargement is favorable, but distortions in the paper are possible. The photo was copied on a film that we have measured and reduced with modern positions of the comparison stars.
The four missing plates cover a part of the +10d zone of declination, but the sky patrol at Sonneberg also used a -4d zone at that time. Three plates of this zone taken on Oct.26.9, 27.9, and 29.9 are available in the collection and show trails of Hermes as well. These trails appear in the northern part of the plates and especially the last one is close to the border between very deformed stellar images. The log book associated to the -4d zone reports "vereinzelt Wolken" for the last two of these three plates, or "sometimes single clouds". This remark does not refer to plate T2499 that was exposed later. Although nothing is reported for that plate, perturbations by clouds appear as possible.
In spite of all difficulties, we have tried to derive positions from the three plates of the -4d zone as well. Certainly the following positions from the sky patrol at Sonneberg are less accurate than indicated, although we have used only comparison stars from the PPM Catalogue that are close to the trails. The formal accuracy of our measurements is misleading. Effects of imperfect guiding are visible on two plates exposed for 60 minutes: At the centers of these plates the stellar images are not round but clearly more extended in one direction. In one of these cases the trail of Hermes appears as curved and irregular. We have used a program by Siegfried Roeser in our reductions.

      1937 UB, positions from patrol plates taken at Sonneberg

 Plate   1937,  UT       RA  (2000.0)  Decl   Comp.Stars,  Center    Remarks
                                                number    of plate
                         h  m  s      d  m  s
 E3775   Oct.26.92188   2 08 15.7  +06 31 11      17        2 h         1
             26.94549   2 08 05.9  +06 30 57      17       -4 d         1

 E3779       27.91817   1 58 37.8  +07 08 33      30        2 h         2,3,4
             27.95984   1 58 12.9  +07 11 22      30       -4 d         2,4

 E3795       29.85266   0 43 15.0  +11 32 02      26        1 h         2,5
             29.89433   0 38 26.4  +11 47 27      26       -4 d         2,5

 T2499,  Oct.29.91875   0 35 09.1  +11 55 50      10        1 h         3
  copy       29.9       0 34 13.6  +11 58 27      10      +10 d         6
             29.9       0 32 59.6  +12 01 51      10                    6
             29.93958                                                   7


                       Remarks

  1. Bad definition of ends of faint trail

  2. Visible effects of imperfect guiding; Perturbations by clouds of unknown
     duration

  3. Bad definition of beginning of trail

  4. Irregular form of trail

  5. Long trail not far from edge of plate

  6. Point within trail, that fades towards an apparent end in a stellar image

  7. End of exposure, the visible trail has ended before


Orbits of variation and search lines

According to the circumstances mentioned above the geocentric distance of Hermes at a given epoch in 1937 results with some uncertainty. A variation of this distance in some range is possible. We have adopted a number of values for this distance and derived for each of them a corresponding orbit of variation. For the epoch JD 2428834.5 the values of the semi-major axis of our set of orbits cover the range from 1.624 to 1.661 au . Marsden's result corresponds to 1.639 au at this epoch. Forward integrations of our set of orbits lead to further close approaches in many cases: approaches to the earth are possible at both the nodes, close approaches to Venus are possible as well. We have searched files of observations for later observations of Hermes, but in vain. If another close approach to earth has occurred at all, a missing movement towards opposition or bright moonlight can have prevented observations. Furthermore, both the incoming and the outgoing branches of the orbit of Hermes are turned to the south of the ecliptic.

There is a subset of orbits that has avoided very close approaches to the inner planets until now and will lead to the vicinity of earth not before Oct. 2003. In this subset the range covered by the mean longitudes increases at first, due to the different mean motions, but later on special perturbations stop and reverse this process. Therefore, a comparatively large set of orbits corresponds to an approach in Oct. 2003. This seems to indicate a larger probability for a return of Hermes in that year, if compared with other years. Anyway, an orbit of this subset is useful to represent the quality of the orbit of Hermes at the present time, or to allow the derivation of search lines. An example for this is given below.

Actually, according to a search along lines computed for August 2001, Hermes does probably not move on an orbit of this subset. At Siding Spring Observatory, NSW, Australia, Dr.Robert H. McNaught tried to find Hermes in the vicinity of these search lines, but did not find the object. More details on this are given in a special section.

          1937 UB, incoming branch of the orbit, search lines

     according to a special orbit of variation integrated to Sept. 2003.

  Elements of this orbit for the epoch    JDATE= 2452900.5  = 2003 Sept.18.0,
  angles are given in degrees :

  a= 1.654884    e= 0.626246    M= 317.0

  omega,node,incl.: 92.0503 ,  34.6105 ,  6.1673   (2000.0)

  V magnitude from    H = 16.8     G = 0.15  , H depends on 3 trails of 1937
                                               and  B-V = 0.8 .

 The round value given for the mean anomaly, M, of this orbit is varied from
 315.0 to 319.0 at 1.0 deg intervals to generate 5 subsequent ephemeris places
 for some dates in Sept./Oct. 2003. The first four places derived for a date
 correspond to the subset of our orbits of variation mentioned above. It is
 meaningful to derive more places by use of smaller values of M.
   However, the resulting search lines are approximately valid for Sept./Oct.
 of other years as well. To be more accurate in 2001, for instance, subtract
 12 hours from the time given for an ephemeris place of 2003. This fits the
 position of the earth, but the elements of the orbit of Hermes will differ
 in other years, especially in case of strong perturbations by Earth or Venus,
 see the Note given at the end of the search lines.

   1937UB Hermes, search lines generated by variation of mean anomaly,
                  they are approximately valid for the same dates of
                  years preceding or following 2003.

  0 h TT       R.A. (2000) Decl.       Delta       r        Mag.(V)     Phase

 03  9 18     1 54.7        3  0       .538      1.482       17.4        22.3
 03  9 18     2  6.9        4 22       .529      1.462                   24.6
 03  9 18     2 19.6        5 47       .521      1.441                   27.0
 03  9 18     2 32.9        7 13       .515      1.421                   29.5
 03  9 18     2 46.7        8 40       .510      1.400       17.4        32.0

 03  9 22     1 53.9        2 47       .485      1.444       17.0        20.3
 03  9 22     2  7.7        4 19       .475      1.424                   23.0
 03  9 22     2 22.2        5 54       .466      1.403                   25.7
 03  9 22     2 37.4        7 31       .460      1.383                   28.7
 03  9 22     2 53.3        9  8       .455      1.362       17.1        31.7

 03  9 26     1 52.2        2 29       .434      1.406       16.7        18.1
 03  9 26     2  7.8        4 12       .423      1.386                   21.1
 03  9 26     2 24.4        5 59       .413      1.365                   24.4
 03  9 26     2 42.0        7 50       .406      1.344                   27.8
 03  9 26     3   .6        9 41       .400      1.322       16.8        31.5

 03  9 30     1 49.2        2  6       .386      1.368       16.3        15.5
 03  9 30     2  7.0        4  3       .373      1.347                   19.0
 03  9 30     2 26.3        6  5       .362      1.325                   22.8
 03  9 30     2 46.9        8 12       .354      1.304                   26.9
 03  9 30     3  8.9       10 19       .348      1.282       16.4        31.4

 03 10  4     1 44.6        1 37       .339      1.329       15.8        12.6
 03 10  4     2  5.1        3 49       .324      1.307                   16.5
 03 10  4     2 27.7        6 11       .312      1.285                   21.0
 03 10  4     2 52.4        8 39       .303      1.264                   26.1
 03 10  4     3 18.9       11  8       .297      1.242       16.0        31.5

 03 10  8     1 38.1        1  1       .295      1.289       15.3         9.5
 03 10  8     2  1.9        3 32       .278      1.267                   13.7
 03 10  8     2 28.8        6 19       .264      1.245                   19.0
 03 10  8     2 58.9        9 15       .254      1.223                   25.3
 03 10  8     3 31.7       12 12       .248      1.200       15.5        32.2

 03 10 12     1 28.9        0 15       .252      1.248       14.8         7.0
 03 10 12     1 56.6        3 10       .233      1.226       14.7        10.5
 03 10 12     2 29.3        6 30       .217      1.204       14.8        16.8
 03 10 12     3  7.1       10  6       .206      1.181       14.9        24.8
 03 10 12     3 49.4       13 40       .201      1.159       15.0        33.9

 03 10 16     1 15.9      - 0 45       .212      1.207       14.4         7.8
 03 10 16     1 48.3        2 39       .189      1.185       14.1         7.5
 03 10 16     2 29.1        6 47       .171      1.162       14.1        14.3
 03 10 16     3 19.0       11 24       .159      1.139       14.3        25.1
 03 10 16     4 16.2       15 49       .156      1.116       14.5        37.6


                                   Note

  In years different from 2003 the above search lines approximately describe
a possible approach of Hermes near the ascending node of its orbit, but then
the original elements of 1937 and the perturbations do not correspond to the
orbits used above. We have used other orbits of variation of our set to model
approaches of Hermes near the ascending or descending node in some years. We
can try to do this for other years. September and October of a year offer the
best chance to rediscover this long-lost asteroid, but observers south of the
equator have a second chance in May and June.
  Ask for more information by use of one of the e-mail addresses given above.


An attempt to find Hermes in the morning sky in August 2001

To get an early decision about the presence of Hermes within the subset of orbits mentioned above, an extended subset of about 14 percent of our most probable orbits of variation was integrated to a suitable epoch in 2001, and search lines, as shown below for two dates in Aug. 2001, were derived. The range of elongation at 80 deg. is limited, but the predicted brightness is low and subject to uncertainty.
Nevertheless, Dr. Robert H. McNaught has kindly agreed to cooperate with us in an attempt to look for Hermes according to search lines prepared for Aug. 2001. Although he lost several nights by unfavourable weather conditions, he could use the 1.0-m telescope with CCD at Siding Spring Observatory to look along the computed lines. Unfortunately, Hermes did not appear in this search. Probably its orbit differs from those considered here.

Here we give some of the numerical details used in this project:
The following five orbits represent the subset at the epoch JD 2452100.5 and demonstrate the range covered by the elements. The second orbit corresponds to a minimum of the mean anomaly, M, at this epoch. The minimum results from the action of the perturbing planets. The angles are given in degrees.


    M            a           e         Peri.      Node      Incl.    (2000.0)

 303.76713   1.6551120   0.6260578   92.05172   34.61524   6.15859
 302.73818   1.6564481   0.6263287   92.04297   34.62198   6.15908
 304.73875   1.6558763   0.6262860   92.02089   34.63375   6.16246
 306.73529   1.6547045   0.6262063   92.00276   34.63727   6.16741
 307.56633   1.6545808   0.6262315   92.01415   34.62452   6.16721

  V magnitude from    H = 16.8     G = 0.15  , H depends on 3 trails of 1937
                                               and  B-V = 0.8 .


Four positions derived from the four last orbits, respectively, represent search lines given below for two subsequent dates in August 2001. Places from the first orbit are close to these lines.


         TT    R.A.(J2000) Decl.      Delta       R       El.     Ph.      V

 01  8 25.0   4 22.5       18 40       .905      1.295    84.9    51.0    19.0
 01  8 25.0   4 40.8       19 51       .924      1.251    80.5    52.8
 01  8 25.0   4 59.5       20 54       .945      1.205    76.0    54.5
 01  8 25.0   5  7.1       21 17       .955      1.186    74.2    55.0    19.1

 01  8 26.0   4 27.1       18 55       .892      1.285    84.8    51.5    19.0
 01  8 26.0   4 45.8       20  5       .912      1.241    80.2    53.4
 01  8 26.0   5  4.8       21  6       .934      1.195    75.7    55.0
 01  8 26.0   5 12.6       21 29       .945      1.176    73.8    55.6    19.1



Text of sections last modified: 2001 Dec. 6
Changes in main title and index: 2003 Nov.