From Surf Wiki (app.surf) — the open knowledge base
2010 RF12
Small risk–listed near-Earth asteroid
Small risk–listed near-Earth asteroid
| Field | Value |
|---|---|
| minorplanet | yes |
| name | |
| background | #FFC2E0 |
| discovery_ref | |
| discoverer | Mount Lemmon Srvy. |
| discovery_site | Mount Lemmon Obs. |
| discovered | 5 September 2010 |
| mpc_name | |
| mp_category | NEOApollo |
| orbit_ref | |
| epoch | 2025-Nov-21 (JD 2461000.5) |
| uncertainty | 0 (MPC) 2 (JPL) |
| observation_arc | 11.98 years |
| aphelion | 1.261 AU |
| perihelion | 0.86158 AU |
| time_periastron | 2026-Mar-05 |
| semimajor | 1.0615 AU |
| eccentricity | 0.18831 |
| period | 1.094 yr (399.445 d) |
| mean_anomaly | 266.1° |
| mean_motion | / day |
| inclination | 0.88267° |
| asc_node | 163.69° |
| arg_peri | 267.44° |
| moid | 0.00060 AU |
| mean_diameter | |
| 6–12 meters (CNEOS) | |
| abs_magnitude | 28.42 |
6–12 meters (CNEOS)
**** is a very small asteroid, classified as a near-Earth object of the Apollo group, that passed between Earth and the Moon on 8 September 2010, at 21:12 UTC, approaching Earth within 79000 km above Antarctica. The asteroid was discovered by the Mount Lemmon Survey near Tucson, Arizona on 5 September 2010 along with . Based on a short 7-day observation arc from that apparation, it was listed for 12 years on the Sentry Risk Table as the asteroid with the greatest known probability (5%) of impacting Earth. was rediscovered in August 2022, and now has a 12-year observation arc and a much better known orbit. As of the December 2022 solution which accounts for nongravitational forces, there is a 1-in-10 chance of an Earth impact on 5 September 2095.
| Date | Impact | ||
|---|---|---|---|
| probability | JPL Horizons | ||
| nominal geocentric | |||
| distance (AU) | uncertainty | ||
| region | |||
| (3-sigma) | |||
| 2095-09-06 00:06 ± 00:20 | 1:10 | 0.00035 AU | ±180 thousand km |
In 2023, **** was identified as a possible dark comet. Dark comets are asteroids that exhibit comet-like acceleration, but visually appear as asteroids, with no coma or tail. Astronomers who study them believe the acceleration is caused by outgassing on the sunlit side.
Description
NASA's Near Earth Program estimates its size to be 7 m in diameter with a mass of around 500 tonnes. The power of the airburst would be somewhere between the 2–4 m Sutter's Mill meteorite and the 17 m Chelyabinsk meteor (which had 440 KT equivalent energy). The approach in 2096 is poorly known because it is dependent on the September 2095 Earth approach.
| Date | Impact | |||||
|---|---|---|---|---|---|---|
| probability | ||||||
| (1 in) | JPL Horizons | |||||
| nominal geocentric | ||||||
| distance (AU) | NEODyS | |||||
| nominal geocentric | ||||||
| distance (AU) | MPC | |||||
| nominal geocentric | ||||||
| distance (AU) | Find_Orb | |||||
| nominal geocentric | ||||||
| distance (AU) | uncertainty | |||||
| region | ||||||
| (3-sigma) | ||||||
| 2095-09-05 23:46 | 10 | 0.00035 AU | 0.0008 AU | 0.00066 AU | 130000 km | ±180 thousand km |
| 2096-09-04 21:50 | 22000 | 0.84 AU | 0.18 AU | 0.36 AU | 0.19 AU | ±414 million km |
On 17 February 2059 the asteroid will pass within 3.5 million km from Earth and reach about apparent magnitude 22.6 by late February. On 10 September 1915 it passed from Earth.
Notes
References
|access-date = 2014-04-17}} (K10R12F)
|archive-url = https://archive.today/20221223224337/https://ssd.jpl.nasa.gov/tools/sbdb_lookup.html%23/?sstr=2010RF12&view=OPC |archive-date= 2022-12-23 |url-status = live |access-date = 2022-12-23}}
|access-date = 21 January 2020}}
|archive-url = https://web.archive.org/web/20100911072645/http://news.nationalgeographic.com/news/2010/09/100908-asteroids-earth-nasa-catalina-sky-survey-science-space |url-status = dead |archive-date = 11 September 2010 |access-date = 21 January 2020}}
|archive-url = https://web.archive.org/web/20100909142420/http://www.boston.com/news/local/breaking_news/2010/09/harvard_scienti_1.html |archive-date= 9 September 2010 |access-date = 21 January 2020}}
|archive-url = https://web.archive.org/web/20170122151206/http://neo.jpl.nasa.gov/risk/2010rf12.html#?des=2010%20RF12 |archive-date = 22 January 2017 |url-status = live |access-date = 2022-12-23}}
|archive-url = https://web.archive.org/web/20100911052418/http://neo.jpl.nasa.gov/risk/ |archive-date = 11 September 2010 |url-status = live |access-date = 2022-12-23}}
|archive-url=https://web.archive.org/web/20221223231926/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272010+RF12%27&START_TIME=%272095-09-05%2023:46%27&STOP_TIME=%272095-09-06%27&STEP_SIZE=%272%20days%27&QUANTITIES=%2720,39%27 |archive-date=2022-12-23 |url-status=live
|archive-url=https://web.archive.org/web/20221223232436/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272010+RF12%27&START_TIME=%272095-09-06%2000:06%27&STOP_TIME=%272095-09-07%27&STEP_SIZE=%272%20days%27&QUANTITIES=%2720,39%27 |archive-date=2022-12-23 |url-status=live
|archive-url=https://web.archive.org/web/20220707092915/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272010+RF12%27&START_TIME=%272096-09-04+21%3A50%27&STOP_TIME=%272096-09-05%27&STEP_SIZE=%272+days%27&QUANTITIES=%2720%2C39%27 |archive-date=2022-07-07 |url-status=live
|archive-url=https://web.archive.org/web/20220706182711/https://www.projectpluto.com/cgi-bin/fo/fo_serve.cgi?obj_name=2010+RF12&year=2095-09-06&n_steps=1&stepsize=1 |archive-date=2022-07-06 |url-status=live
|archive-url=https://archive.today/20221223230808/https://www.projectpluto.com/cgi-bin/fo/fo_serve.cgi?obj_name=2010+RF12&year=2096-09-05&n_steps=1&stepsize=1 |archive-date=2022-12-23 |url-status=live
|access-date = 21 January 2020}} (1 in 12)
|archive-url = https://web.archive.org/web/20220706185615/https://newton.spacedys.com//neodys/index.php?pc=1.1.3.1&n=2010RF12&oc=500&y0=2095&m0=9&d0=5&h0=12&mi0=0&y1=2095&m1=9&d1=6&h1=12&mi1=0&ti=1.0&tiu=hours |archive-date= 2022-07-06 |url-status = live |access-date = 21 January 2020}} (NEODyS Close Approach Table))
|archive-url = https://archive.today/20221223092947/https://newton.spacedys.com//neodys/index.php?pc=1.1.3.1&n=2010RF12&oc=500&y0=2096&m0=9&d0=4&h0=12&mi0=0&y1=2096&m1=9&d1=5&h1=12&mi1=0&ti=1.0&tiu=hours |archive-date= 2022-12-23 |url-status = live |access-date = 23 December 2022}}
|archive-url = https://web.archive.org/web/20220102014840/https://www.nasa.gov/feature/five-years-after-the-chelyabinsk-meteor-nasa-leads-efforts-in-planetary-defense/ |archive-date = 2 January 2022 |url-status=live |access-date = 2022-01-19}}
References
- Many small and harmless asteroids (less than ~10 meters in diameter) impact Earth every year but very few are discovered and predicted, see [[Asteroid impact prediction]].
- Seligman, Darryl Z.. (2023-02-15). "Dark Comets? Unexpectedly Large Nongravitational Accelerations on a Sample of Small Asteroids". The Planetary Science Journal.
- (2025-05-01). "Dark Comets". Scientific American.
- {{mp. 2010 RF. 52000. 180000. airbursts]] in the upper atmosphere. Pebble sized fragments would likely fall to the ground at terminal velocity.[http://www.oecd.org/dataoecd/18/40/2493218.pdf How a Near-Earth Object Impact Might Affect Society, 9 January 2003, Clark R. Chapman, SwRI, Boulder CO USA]
This article was imported from Wikipedia and is available under the Creative Commons Attribution-ShareAlike 4.0 License. Content has been adapted to SurfDoc format. Original contributors can be found on the article history page.
Ask Mako anything about 2010 RF12 — get instant answers, deeper analysis, and related topics.
Research with MakoFree with your Surf account
Create a free account to save articles, ask Mako questions, and organize your research.
Sign up freeThis content may have been generated or modified by AI. CloudSurf Software LLC is not responsible for the accuracy, completeness, or reliability of AI-generated content. Always verify important information from primary sources.
Report