Torino scale explained

The Torino scale is a method for categorizing the impact hazard associated with near-Earth objects (NEOs) such as asteroids and comets.It is intended as a communication tool for astronomers and the public to assess the seriousness of collision predictions, by combining probability statistics and known kinetic damage potentials into a single threat value. The Palermo Technical Impact Hazard Scale is a similar, but more complex scale.

Near-Earth objects with a Torino scale of 1 are discovered several times a year, and may last a few weeks until they have a longer observation arc that eliminates any possibility of a collision. The only two objects on the Torino Scale that have ever ranked higher are asteroids 99942 Apophis, which had a rating of 4 for four days in late 2004, the highest recorded rating, and, with a historical rating of 2 from February to May 2006.

Overview

The Torino Scale uses an integer scale from 0 to 10. A 0 indicates an object has a negligibly small chance of collision with the Earth, compared with the usual "background noise" of collision events, or is too small to penetrate Earth's atmosphere intact. A 10 indicates that a collision is certain, and the impacting object is large enough to precipitate a global disaster.

An object is assigned a 0 to 10 value based on its collision probability and the kinetic energy (expressed in megatons of TNT) of the possible collision.

The Torino Scale is defined only for potential impacts less than 100 years in the future.

"For an object with multiple potential collisions on a set of dates, a Torino Scale value should be determined for each date. It may be convenient to summarize such an object by the greatest Torino Scale value within the set."[1]

History and naming

The Torino Scale was created by Professor Richard P. Binzel in the Department of Earth, Atmospheric, and Planetary Sciences, at the Massachusetts Institute of Technology (MIT). The first version, called "A Near-Earth Object Hazard Index", was presented at a United Nations conference in 1995 and was published by Binzel in the subsequent conference proceedings (Annals of the New York Academy of Sciences, volume 822, 1997.)

A revised version of the "Hazard Index" was presented at a June 1999 international conference on NEOs held in Torino (Turin), Italy. The conference participants voted to adopt the revised version, where the bestowed name "Torino Scale" recognizes the spirit of international cooperation displayed at that conference toward research efforts to understand the hazards posed by NEOs. ("Torino Scale" is the proper usage, not "Turin Scale.")[1]

Due to exaggerated press coverage of Level 1 asteroids, a rewording of the Torino Scale was published in 2005, adding more details and renaming the categories: in particular, Level 1 was changed from "Events meriting careful monitoring" to "Normal".

The Torino Scale has served as the model for the Rio scale, which quantifies the validity and societal impact of SETI data.[2]

Current Torino scale

The Torino Scale also uses a color code scale: white, green, yellow, orange, red. Each color code has an overall meaning:

No hazard (white)
0The likelihood of a collision is zero, or is so low as to be effectively zero. Also applies to small objects such as meteors and bodies that burn up in the atmosphere as well as infrequent meteorite falls that rarely cause damage.
Normal (green)
1A routine discovery in which a pass near Earth is predicted that poses no unusual level of danger. Current calculations show a collision is extremely unlikely with no cause for public attention or public concern. New telescopic observations very likely will lead to reassignment to Level 0.
Meriting attention by astronomers (yellow)
2A discovery, which may become routine with expanded searches, of an object making a somewhat close but not highly unusual pass near Earth. While meriting attention by astronomers, there is no cause for public attention or public concern as an actual collision is still very unlikely. New telescopic observations very likely will lead to reassignment to Level 0.
3A close encounter, meriting attention by astronomers. Current calculations give a 1% or greater chance of collision capable of localized destruction. Most likely, new telescopic observations will lead to reassignment to Level 0. Attention by public and by public officials is merited if the encounter is less than a decade away.
4A close encounter, meriting attention by astronomers. Current calculations give a 1% or greater chance of collision capable of regional devastation. Most likely, new telescopic observations will lead to reassignment to Level 0. Attention by public and by public officials is merited if the encounter is less than a decade away.
Threatening (orange)
5A close encounter posing a serious, but still uncertain threat of regional devastation. Even though most objects of this level will be lowered to Level 0, critical attention by astronomers is still needed to determine conclusively whether a collision will occur. If the encounter is less than a decade away, governmental contingency planning may be warranted.
6A close encounter by a large object posing a serious but still uncertain threat of a global catastrophe. Critical attention by astronomers is needed to determine conclusively whether a collision will occur. If the encounter is less than three decades away, governmental contingency planning may be warranted. Some objects of this level may be lowered to Level 1 or 2, if the chances of collision decrease.
7A very close encounter by a large object, which if occurring this century, poses an unprecedented but still uncertain threat of a global catastrophe. For such a threat in the next 100 years, international contingency planning is warranted, especially to determine urgently and conclusively whether a collision will occur.
Certain Collisions (red)
8A collision is certain, capable of causing localized destruction for an impact over land or possibly a tsunami if close offshore. Such events occur on average between once per 50 years and once per several thousand years.
9A collision is certain, capable of causing unprecedented regional devastation for a land impact or the threat of a major tsunami for an ocean impact. Such events occur on average between once per 10,000 years and once per 100,000 years.
10A collision is certain, capable of causing global climatic catastrophe that may threaten the future of life as we know it, whether impacting land or ocean. Such events occur on average once per 100,000 years, or less often.

No incoming object has ever been rated above level 4, though over all of Earth's history impacts have spanned the full range of damage described by the scale.

Actual impacts and impact energy comparisons

The Chicxulub impact, believed by most scientists to have been a significant factor in the extinction of the non-avian dinosaurs, has been estimated at 100 million (108) megatons, or Torino Scale 10. The impacts that created the Barringer Crater and the 1908 Tunguska event are both estimated to be in the 3–10 megaton range,[3] corresponding to Torino Scale 8. The 2013 Chelyabinsk meteor had a total kinetic energy prior to impact of about 0.5 megatons, corresponding to Torino Scale 0. Between 2000 and 2013, 26 asteroid impacts with an energy of 1–600 kilotons were detected.[4]

The biggest hydrogen bomb ever exploded, the Tsar Bomba, was around 50 megatons.The 1883 eruption of Krakatoa was the equivalent of roughly 200 megatons.

The comet C/2013 A1, which passed close to Mars in 2014, was originally estimated to have a potential impact energy of 5 million to 24 billion megatons, and in March 2013 was estimated to have a Mars impact probability of ~1:1250, corresponding to the Martian equivalent of Torino Scale 6.[5] The impact probability was reduced to ~1:120000 in April 2013, corresponding to Torino Scale 1 or 2.[6]

Objects with non-zero Torino ratings

Currently non-zero

Last updated: -08-18

Downgraded to zero

This is a partial list of near-Earth asteroids that have been listed with a Torino Scale rating of 1+ and been lowered to 0 or been removed from the Sentry Risk Table altogether. Most objects that reach a Torino Scale of 1 have a short observation arc of less than 2 weeks and are quickly removed as the observation arc gets longer and more accurate.

See also

External links

Notes and References

  1. Web site: Torino Impact Scale . 2007-03-11 . dead . https://web.archive.org/web/20070224184143/http://impact.arc.nasa.gov/torino.cfm . 2007-02-24 . Torino Impact Scale (NASA Ames)
  2. Web site: The Rio Scale . International Academy of Astronautics . 2016-08-29 . 2016-09-02 . https://web.archive.org/web/20160902040412/http://avsport.org/IAA/riocalc.htm . dead .
  3. Web site: Sandia supercomputers offer new explanation of Tunguska disaster. Sandia National Laboratories. December 17, 2007. February 21, 2021. June 8, 2021. https://web.archive.org/web/20210608194615/https://www.eurekalert.org/pub_releases/2007-12/dnl-sso121807.php. live.
  4. Web site: Archived copy . 2014-09-05 . dead . https://web.archive.org/web/20140905214015/http://sentinelmission.org/wp-content/uploads/2014/04/B612_PR_042214.pdf . 2014-09-05 .
  5. Web site: 3 March 2013. Close approach to Mars. Up-to-date analysis. SpaceObs.org blog (ISON-NM). Leonid. Elenin. 2013-03-03. 2013-03-07. https://web.archive.org/web/20130307081417/http://spaceobs.org/en/2013/03/03/probability-of-collision-with-mars/. dead.
  6. Web site: News - Comet to Make Close Flyby of Red Planet in October 2014. NASA/JPL. 2013-06-05. 2013-03-08. https://web.archive.org/web/20130308140413/http://www.jpl.nasa.gov/news/news.php?release=2013-081. live.
  7. Web site: Sentry: 2023 JE5 . 2023-05-18 . 2013-05-11 . https://web.archive.org/web/20130511010048/http://neo.jpl.nasa.gov/risk/a99942.html#?des=2023%20JE5 . live .
  8. Web site: JPL Horizons: 2023 JE5 geocentric distance and uncertainty on 4 October 2071 . https://web.archive.org/web/20230518192929/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272023+JE5%27&START_TIME=%272071-10-04%2020:24%27&STOP_TIME=%272071-10-05%27&STEP_SIZE=%272%20day%27&QUANTITIES=%2720,39%27 . 2023-05-18 . live.
  9. Web site: Sentry: 2023 GQ2 . 2023-04-19 . 2013-05-11 . https://web.archive.org/web/20130511010048/http://neo.jpl.nasa.gov/risk/a99942.html#?des=2023%20GQ2 . live .
  10. Web site: JPL Horizons: 2023 GQ2 geocentric distance and uncertainty on 16 November 2028 . 2023-04-19 . 2023-04-20 . https://web.archive.org/web/20230420144523/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272023+GQ2%27&START_TIME=%272028-11-16%2000:58%27&STOP_TIME=%272028-11-17%27&STEP_SIZE=%272%20day%27&QUANTITIES=%2720,39%27 . live .
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  13. https://archive.today/20230316171038/https://cneos.jpl.nasa.gov/sentry/details.html%23?des=2023%20DW Sentry: 2023 DW
  14. Web site: JPL Horizons: 2023 DW geocentric distance and uncertainty on 14 February 2046 . JPL Horizons . https://web.archive.org/web/20230304160813/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272023+DW%27&START_TIME=%272046-02-14%2021:36%27&STOP_TIME=%272046-02-15%27&STEP_SIZE=%272%20day%27&QUANTITIES=%2720,39%27 . 2023-03-04 . live . 2023-03-21 . Risk Corridor Calculations: Piero_Sicoli and StevearenoBR
  15. https://archive.today/20230201094029/https://cneos.jpl.nasa.gov/sentry/details.html%23?des=2023%20AJ1 Archive Sentry: 2023 AJ1
  16. Web site: JPL Horizons: 2023 AJ1 geocentric distance and uncertainty on 10 January 2096 . JPL Horizons . 2023-01-26 . 2023-01-27 . https://web.archive.org/web/20230127062319/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272023+AJ1%27&START_TIME=%272096-01-10%27&STOP_TIME=%272096-01-11%27&STEP_SIZE=%272%20day%27&QUANTITIES=%2720,39%27 . live .
  17. Web site: Sentry: 2023 TL4 . 2023-12-03 . 2013-05-11 . https://web.archive.org/web/20130511010048/http://neo.jpl.nasa.gov/risk/a99942.html#?des=2023%20TL4 . live .
  18. Web site: ESA Risk List . 2023-11-04 . NEO . en-GB . 2023-03-05 . https://web.archive.org/web/20230305210103/https://neo.ssa.esa.int/risk-list . live .
  19. Web site: JPL Horizons: 2023 TL4 geocentric distance and uncertainty on 10 October 2119 . 2023-12-03 . 2023-12-04 . https://web.archive.org/web/20231204142430/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272023+TL4%27&START_TIME=%272119-10-10%27&STOP_TIME=%272119-10-11%27&STEP_SIZE=%272%20day%27&QUANTITIES=%2720,39%27 . live .
  20. https://archive.today/20221112201640/https://cneos.jpl.nasa.gov/sentry/details.html%23?des=2022%20UE28 Archive Sentry: 2022 UE28
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  22. https://web.archive.org/web/20220904080653/https://neo.ssa.esa.int/risk-list Archive of ESA Risk List
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  24. Web site: Sentry Archive: 2022 BX1 . 2022-01-29 . 2022-01-29 . https://archive.today/20220129200548/https://cneos.jpl.nasa.gov/sentry/details.html%23?des=2022%20BX1 . live .
  25. Web site: JPL Horizons: 2022 BX1 geocentric distance and uncertainty on 11 July 2061 . JPL Horizons . 2022-01-29 . 2022-01-29 . https://web.archive.org/web/20220129213837/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272022+BX1%27&START_TIME=%272061-07-11+21%3A22%27&STOP_TIME=%272061-07-12%27&STEP_SIZE=%271+day%27&QUANTITIES=%2720%2C39%27 . live .
  26. Web site: Archive esa Risk List with 2022 AE1. https://web.archive.org/web/20220111175710/https://neo.ssa.esa.int/risk-list. 2022-01-11.
  27. Web site: Archive esa Risk List with 2021 TP21. https://web.archive.org/web/20211031094029/https://neo.ssa.esa.int/risk-list. 2021-10-31.
  28. Web site: JPL Horizons Archive: 2021 TP21 geocentric distance and uncertainty on 27 March 2081 . JPL Horizons . https://web.archive.org/web/20211031005214/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272021+TP21%27&START_TIME=%272081-03-26%27&STOP_TIME=%272081-03-28%27&STEP_SIZE=%271+day%27&QUANTITIES=%2720%2C39%27 . 2021-10-31 .
  29. Web site: Archive esa Risk List with 2021 TA8. https://web.archive.org/web/20211012143624/https://neo.ssa.esa.int/risk-list. 2021-10-12.
  30. Web site: Archive JPL Horizons: 2021 TA8 geocentric distance and uncertainty on 3 May 2034 . 2021-10-12 . https://web.archive.org/web/20211012075513/https://ssd.jpl.nasa.gov/horizons_batch.cgi?batch=1&COMMAND=%272021+TA8%27&START_TIME=%272034-05-02%27&STOP_TIME=%272034-05-04%27&STEP_SIZE=%271+day%27&QUANTITIES=%2720%2C39%27. 2021-10-12.
  31. Web site: hohmanntransfer: 2020 XR (10 Dec 2020). 12 December 2020. 28 February 2021. https://web.archive.org/web/20210228012834/http://www.hohmanntransfer.com/mn/20/20345_1210.htm#2020XR. live.
  32. Web site: Sentry: 2020 NK1. 2020-07-22. 2013-05-11. https://web.archive.org/web/20130511010048/http://neo.jpl.nasa.gov/risk/a99942.html#?des=2020%20NK1. live.
  33. https://cneos.jpl.nasa.gov/sentry/details.html#?des=2020%20DR2 Sentry: Earth Impact Monitoring 2020 DR2 -- Earth Impact Risk Summary
  34. Web site: Archive.is of Sentry: 2020 BW14 . https://archive.today/20200207192115/https://cneos.jpl.nasa.gov/sentry/details.html%23?des=2020%20BW14 . 7 February 2020 . dead.
  35. Web site: MPEC 2020-C125 : 2020 BW14. 2020-02-10. 2021-03-08. https://web.archive.org/web/20210308172653/https://minorplanetcenter.net/mpec/K20/K20CC5.html. live.
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  52. archive is/Wx0I3
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