Australian Sky & Telescope — January 01, 2018

(WallPaper) #1

50 AUSTRALIAN SKY & TELESCOPE January 2018


COMETS by David Seargent

Close encounter with the Sun


Will comet C/2017 T1 (Heinze) survive its perihelion passage?


O


n October 2 last year, Aren
Heinze of the University of
Hawaii Asteroid Terrestrial-
impact Last Alert System (ATLAS),
discovered an 18.2-magnitude comet
sporting a coma approximately 7
arseconds in diameter and a tail about
10 arcseconds long. The comet was
found in images secured with the 0.5-m
f/2 Schmidt telescope at Mauna Loa.
Orbital computations revealed the
new object to be moving in an almost
parabolic orbit toward perihelion on
February 21, 2018 at a rather small
0.58 astronomical units (a.u.) from the

Sun. On its way to perihelion, C/2017
T1 (Heinze) will pass just over 0.2 a.u.
from Earth on January 4.
Although the comet favours
northern latitudes at the time of closest
approach, it should be visible during
late December and during the first few
days of January as it moves northward
from Cancer into Lynx across the New
Year period. Observers in the north of

Australia will be favoured, although
thosefurthersouthwhoareblessed
withaclearnorthernhorizonshould
be able to locate the comet at low
elevation. On present indications, it will
probably be about magnitude 9.5–10 at
the time.
Following perihelion, C/2017 T1
willtheoreticallyemergeintothe
southern morning sky in March.
Normally,aperiheliondistanceof
around0.5a.u.shouldholdpromiseof
afairlyimpressiveobject,eventhough
this comet will then be on the farthest
sideoftheSolarSystem.Nevertheless,
present indications
suggestthatthisis
an intrinsically faint
object that may not
survive its encounter
with the Sun.

Survival instincts
Back in the 1980s,
veteran comet observer
John Bortle found
that comets that are
either dynamically
new (as this one
appears to be) or of
very long period, fail
to survive perihelion
if their absolute
magnitude—thatisto
say, the hypothetical
brightness that they
would have if located
at1a.u.frombothEarthandSun—
isfainterthanavaluedefinedbythe
formula H 0 = 7 + 6q, where H 0 is the
absolute magnitude and q is the comet’s
perihelion distance in a.u.
This formula holds quite well for
very long-period comets, although it is
less well-defined for those of moderate
period and is not applicable at all for
short-period objects. Indeed, the few

instances where very long-period/
dynamically new objects have departed
from the formula’s predictions involved
comets brighter than the ‘survival limit’
disintegrating, rather than fainter ones
surviving! Maybe these comets were
experiencing prolonged outbursts that
made them seem brighter than their
‘true’ value?
Be that as it may, for C/2017 T1,
the ‘Bortle Limit’ (as it has come to be
known) is 10.5. However, according
to the estimates available thus far, the
comet’s absolute brightness seems to
be about two magnitudes fainter than
this! Admittedly, all available estimates
are derived from CCD observations
made for astrometric purposes and
are most probably rather conservative.
Yet, it is questionable whether they are
sufficiently pessimistic for the comet to
be rescued. Visual observations during
December and January, especially
binocular brightness estimates as the
comet passes close to Earth, will be
important in assessing the survival
prospects of this object.
As mentioned in our Nov/Dec issue,
C/2016 R2 (PANSTARRS) should also
be visible through moderate-sized
telescopes during January as it drifts
toward its May 9 perihelion at 2.6
a.u. from the Sun. Recent brightness
estimates suggest that the magnitude
predictions given in that issue may
have been a little optimistic, and that
the comet might be closer to 12 than
10 during January. However it should
be well-condensed in appearance and
rather well placed in Taurus. As January
opens, the comet will be found within
the Hyades open cluster, slowly trekking
northward as the month progresses.

■ DAVID SEARGENT is the discoverer of
comet 1978 XV. His book, Snowballs in the
Furnace, is available from Amazon.com.

S Comet C/2017 T1 should briefly be visible at the beginning of
January, and hopefully again in March. This image was taken by
Michael Jäger on October 15.
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