Asteroid 532 Herculina will be well placed, lying in the constellation Leo, well above the horizon for much of the night.
Regardless of your location on the Earth, 532 Herculina will reach its highest point in the sky around midnight local time.
From Cambridge, it will be visible in the morning sky, becoming accessible around 18:38, when it rises to an altitude of 21° above your eastern horizon. It will then reach its highest point in the sky at 00:24, 76° above your southern horizon. It will be lost to dawn twilight around 05:46, 25° above your western 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 532 Herculina 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 532 Herculina lies opposite to the Sun in the night sky, the solar system is lined up so that 532 Herculina, the Earth and the Sun lie in a straight line with the Earth in the middle, on the same side of the Sun as 532 Herculina.
On this occasion, 532 Herculina will pass within 1.423 AU of us, reaching a peak brightness of magnitude 9.0. Nonetheless, even at its brightest, 532 Herculina is a faint object beyond the reach of the naked eye; binoculars or a telescope of moderate aperture are needed.
Finding 532 Herculina
The chart below indicates the path of 532 Herculina across the sky around the time of opposition.
The position of 532 Herculina at the moment of opposition will be as follows:
|Asteroid 532 Herculina||09h39m00s||+28°35'||Leo||9.0|
The coordinates above are given in J2000.0.
|The sky on 05 February 2019|
1 day old
All times shown in EST.
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 DE405 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.