Asteroid 2 Pallas will be well placed, lying in the constellation Eridanus, well above the horizon for much of the night.
Regardless of your location on the Earth, 2 Pallas will reach its highest point in the sky around midnight local time.
From Cambridge however, it will not be readily observable since it will lie so far south that it will never rise more than 18° above the horizon.
The geometry of the alignment
This optimal positioning occurs when it makes its closest approach to the point in the sky directly opposite to the Sun – an event termed opposition. Since the Sun reaches its greatest distance below the horizon at midnight, the point opposite to it is highest in the sky at the same time.
At around the same time that 2 Pallas passes opposition, it also makes its closest approach to the Earth – termed its perigee – making it appear at its brightest in the night sky. This happens because when 2 Pallas lies opposite to the Sun in the night sky, the solar system is lined up so that 2 Pallas, the Earth and the Sun lie in a straight line with the Earth in the middle, on the same side of the Sun as 2 Pallas.
On this occasion, 2 Pallas will pass within 1.627 AU of us, reaching a peak brightness of magnitude 8.0. Nonetheless, even at its brightest, 2 Pallas is a faint object beyond the reach of the naked eye; binoculars or a telescope of moderate aperture are needed.
Finding 2 Pallas
The chart below indicates the path of 2 Pallas across the sky around the time of opposition.
It was produced using StarCharter and is available for download, either on dark background, in PNG, PDF or SVG formats, or on a light background, in PNG, PDF or SVG formats.
The position of 2 Pallas at the moment of opposition will be as follows:
| Object | Right Ascension | Declination | Constellation | Magnitude |
| Asteroid 2 Pallas | 04h36m50s | 29°21'S | Eridanus | 8.0 |
The coordinates above are given in J2000.0.
The sky on 14 Nov 2031
| The sky on 14 November 2031 | ||||||||||||||||||||||||||||||||||
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0% 29 days old |
All times shown in EST.
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Source
The circumstances of this event were computed from orbital elements made available by Ted Bowell of the Lowell Observatory. The conversion to geocentric coordinates was performed using the position of the Earth recorded in the DE430 ephemeris published by the Jet Propulsion Laboratory (JPL).
The star chart above shows the positions and magnitudes of stars as they appear in the Tycho catalogue. The data was reduced by the author and plotted using PyXPlot. A gnomonic projection of the sky has been used; celestial coordinates are indicated in the J2000.0 coordinate system.
Image credit
© European Southern Observatory 2021. Credit: ESO/M. Kornmesser/Vernazza et al./MISTRAL algorithm (ONERA/CNRS).