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(367789) 2011 AG5
Near-Earth asteroid in 2040
Near-Earth asteroid in 2040
| Field | Value |
|---|---|
| minorplanet | yes |
| name | |
| background | #FFC2E0 |
| image | 2011 AG5 Goldstone radar 2023-02-04 anim.gif |
| caption | Animation of rotating in radar images by the Goldstone Solar System Radar on 4 February 2023 |
| discovery_ref | |
| discoverer | Mount Lemmon Srvy. |
| discovery_site | Mount Lemon Obs. |
| discovered | 8 January 2011 |
| mpc_name | |
| alt_names | |
| named_after | |
| mp_category | ApolloNEOPHA |
| orbit_ref | |
| epoch | 2023-Feb-25 (JD 2460000.5) |
| uncertainty | 0 |
| observation_arc | 14.2 yr (5,201 days) |
| earliest_precovery_date | 3 October 2008 |
| aphelion | 1.978 AU |
| perihelion | 0.87066 AU |
| time_periastron | 2023-Mar-17 |
| semimajor | 1.424 AU |
| eccentricity | 0.3887 |
| period | 1.7 yr (620.9 days) |
| mean_anomaly | 348.2° |
| mean_motion | / day |
| inclination | 3.6946° |
| asc_node | 135.6° |
| arg_peri | 54.02° |
| moid | 0.00038 AU |
| dimensions | |
| mass | (assumed) |
| abs_magnitude | 21.9 |
****, provisional designation , is a sub-kilometer asteroid, classified as near-Earth object and potentially hazardous asteroid of the Apollo group. It has a diameter of about 140 m. It was removed from the Sentry Risk Table on 21 December 2012 and as such it now has a rating of 0 on the Torino Scale. It was recovered in December 2022 extending the observation arc from 4.8 years to 14 years. As of 2023, the distance between the orbits of Earth and is 0.0004 AU
| Date | JPL Horizons | |
|---|---|---|
| nominal geocentric | ||
| distance (AU) | uncertainty | |
| region | ||
| (3-sigma) | ||
| 2023-Feb-03 08:51 ± 00:01 | 0.01215 AU | ± |
| 2040-Feb-04 08:29 ± 00:06 | 0.00725 AU | ± |
Description

was discovered on 8 January 2011 by the Mount Lemmon Survey at an apparent magnitude of 19.6 using a 1.52 m reflecting telescope. Pan-STARRS precovery images from 8 November 2010 extended the observation arc to 317 days. Observations by the Gemini 8.2 m telescope at Mauna Kea recovered the asteroid on 20, 21 and 27 October 2012, and extended the observation arc to 719 days.
The October 2012 observations reduced the orbit uncertainties by more than a factor of 60, meaning that the Earth's position in February 2040 no longer falls within the range of possible future paths for the asteroid. On 4 February 2040 the asteroid will pass no closer than 0.007 AU (~2.8 LD) from Earth. Until 21 December 2012 it was listed on the Sentry Risk Table with a rating on the Torino Scale of Level 1. A Torino rating of 1 is a routine discovery in which a pass near the Earth is predicted that poses no unusual level of danger. It is estimated that an impact would produce the equivalent of 100 megatons of TNT, roughly twice that of the most powerful nuclear weapon ever detonated (Tsar Bomba). This is powerful enough to damage a region at least a hundred miles wide.
Older risks
Virtual clones of the asteroid that fit the mid-2012 uncertainty region in the known trajectory showed four potential impacts between 2040 and 2047. It had a 1 in 500 chance of impacting the Earth on 5 February 2040. In September 2013, there was an opportunity to make additional observations of when it came within 0.98 AU of Earth. The 2013 observations allowed a further refinement to the known trajectory. The asteroid will also pass 0.0121 AU from the Earth on 3 February 2023. The 2023 gravitational keyhole was 227 miles (365 kilometers) wide. With a Palermo scale rating of -1.00, the odds of impact by were about 10 times less than the background hazard level of Earth impacts which is defined as the average risk posed by objects of the same size or larger over the years until the date of the potential impact.
References
|archive-url=https://archive.today/20221024145712/https://ssd.jpl.nasa.gov/tools/sbdb_lookup.html%23/?sstr=367789&view=OPC |archive-date=2022-10-24 |url-status=live
|archive-url=https://web.archive.org/web/20130108122117/http://neo.jpl.nasa.gov/risk/removed.html |url-status=dead |archive-date=2013-01-08
|archive-url=https://web.archive.org/web/20121231004831/http://neo.jpl.nasa.gov/news/news176.html |url-status=dead |archive-date=31 December 2012
|archive-url=https://web.archive.org/web/20041230031246/http://neo.jpl.nasa.gov/torino_scale1.html |url-status=dead |archive-date=30 December 2004
|url-status=dead
|archive-date=16 April 2021 |archive-url=https://web.archive.org/web/20210416083943/https://www.jpl.nasa.gov/news/news.cfm?release=2012-051 |url-status=dead
|archive-url=https://web.archive.org/web/20020321092747/http://neo.jpl.nasa.gov/risk/doc/palermo.html |url-status=dead |archive-date=21 March 2002
|archive-url=https://web.archive.org/web/20221024142219/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272011+AG5%27&START_TIME=%272023-02-03%2008:50%27&STOP_TIME=%272023-02-04%27&STEP_SIZE=%271%20day%27&QUANTITIES=%2720,39%27 |archive-date=2022-10-24 |url-status=live
|archive-url=https://web.archive.org/web/20221024141438/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%25272011+AG5%2527&START_TIME=%25272040-02-04%252008:49%2527&STOP_TIME=%25272040-02-05%2527&STEP_SIZE=%25271%2520day%2527&QUANTITIES=%252720,39%252 |archive-date=2022-10-24 |url-status=live
References
- Math: 101.00 = 10
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