Uncertainty parameter

Last updated
The orbits of kilometre class NEAs are generally well known, though a few have been lost. However, large numbers of smaller NEAs have highly uncertain orbits. NEA-sizes-vs-uncertainties-compact.PNG
The orbits of kilometre class NEAs are generally well known, though a few have been lost. However, large numbers of smaller NEAs have highly uncertain orbits.

The uncertainty parameterU is introduced by the Minor Planet Center (MPC) to quantify the uncertainty of a perturbed orbital solution for a minor planet. [2] [3] The parameter is a logarithmic scale from 0 to 9 that measures the anticipated longitudinal uncertainty [4] in the minor planet's mean anomaly after 10 years. [2] [3] [5] The larger the number, the larger the uncertainty. The uncertainty parameter is also known as condition code in JPL's Small-Body Database Browser. [3] [5] [6] The U value should not be used as a predictor for the uncertainty in the future motion of near-Earth objects. [2]

Contents

Orbital uncertainty

Classical Kuiper belt objects 40–50 AU from the Sun
JPL SBDB
Uncertainty
parameter

 
Horizons
January 2018
Uncertainty in
distance from the Sun

(millions of kilometers)
Object
 
Reference
Ephemeris

Location: @sun
Table setting: 39
0±0.01 (134340) Pluto E2022-J69
1±0.04 2013 BL76 JPL
2±0.14 20000 Varuna JPL
3±0.84 19521 Chaos JPL
4±1.4 (15807) 1994 GV9 JPL
5±8.2(160256) 2002 PD149 JPL
6±701999 DH8 JPL
7±1901999 CQ153 JPL
8±5901995 KJ1 JPL
9±1,600 1995 GJ JPL
‘D’ Data insufficient for orbit determination.
‘E’ Eccentricity was guessed instead of determined. [7]
‘F’  Both ‘D’ and ‘E’ apply. [7]

Orbital uncertainty is related to several parameters used in the orbit determination process including the number of observations (measurements), the time spanned by those observations (observation arc), the quality of the observations (e.g. radar vs. optical), and the geometry of the observations. Of these parameters, the time spanned by the observations generally has the greatest effect on the orbital uncertainty. [8]

Occasionally, the Minor Planet Center substitutes a letter-code (‘D’, ‘E’, ‘F’) for the uncertainty parameter.

D   Objects with a ‘D’ have only been observed for a single opposition, and have been assigned two (or more) different designations ("double").
EObjects such as 2003 UU291 with a condition code ‘E’ [9] in the place of a numeric uncertainty parameter denotes orbits for which the listed eccentricity was assumed, rather than determined. [7] Objects with assumed eccentricities are generally considered lost if they have not recently been observed because their orbits are not well constrained.[ citation needed ]
FObjects with an ‘F’ fall in both categories ‘D’ and ‘E’. [7]

Calculation

The U parameter is calculated in two steps. [2] [10] First the in-orbit longitude runoff in seconds of arc per decade is calculated, (i.e. the discrepancy between the observed and calculated position extrapolated over ten years):

with

uncertainty in the perihelion time in days
eccentricity of the determined orbit
orbital period in years
uncertainty in the orbital period in days
, Gaussian gravitational constant, converted to degrees

Then, the obtained in-orbit longitude runoff is converted to the "uncertainty parameter" U, which is an integer between 0 and 9. The calculated number can be less than 0 or more than 9, but in those cases either 0 or 9 is used instead. The formula for cutting off the calculated value of U is

For instance: As of 10 September 2016, Ceres technically has an uncertainty of around 2.6, but is instead displayed as the minimal 0.

The result is the same regardless of the choice of base for the logarithm, so long as the same logarithm is used throughout the formula; e.g. for "log" = log10, loge, ln, or log2 the calculated value of U remains the same if the logarithm is the same in both places in the formula.

Function graph U(r) Mpc-uncertainty-parameter.svg
Function graph U(r)
URunoff
Longitude runoff per decade
0 < 1.0 arc second
1 1.04.4 arc seconds
2 4.419.6 arc seconds
3 19.6 arc seconds 1.4 arc minutes
4 1.46.4 arc minutes
5 6.428 arc minutes
6 28 arc minutes 2.1°
7 2.1°9.2°
8 9.2°41°
9 > 41°

648000 is the number of arc seconds in a half circle, so a value greater than 9 would mean that we would have basically no idea where the object will be in 10 years.

Related Research Articles

In astronomy, absolute magnitude is a measure of the luminosity of a celestial object on an inverse logarithmic astronomical magnitude scale. An object's absolute magnitude is defined to be equal to the apparent magnitude that the object would have if it were viewed from a distance of exactly 10 parsecs, without extinction of its light due to absorption by interstellar matter and cosmic dust. By hypothetically placing all objects at a standard reference distance from the observer, their luminosities can be directly compared among each other on a magnitude scale. For Solar System bodies that shine in reflected light, a different definition of absolute magnitude (H) is used, based on a standard reference distance of one astronomical unit.

(35396) 1997 XF11 (provisional designation 1997 XF11) is a kilometer-sized asteroid, classified as a near-Earth object, Mars-crosser and potentially hazardous asteroid of the Apollo group.

4486 Mithra, is an eccentric asteroid and suspected contact-binary, classified as near-Earth object and potentially hazardous asteroid, approximately 2 kilometers in diameter. It belongs to the Apollo group of asteroids and is a relatively slow rotator.

<span class="mw-page-title-main">Orbital eccentricity</span> Amount by which an orbit deviates from a perfect circle

In astrodynamics, the orbital eccentricity of an astronomical object is a dimensionless parameter that determines the amount by which its orbit around another body deviates from a perfect circle. A value of 0 is a circular orbit, values between 0 and 1 form an elliptic orbit, 1 is a parabolic escape orbit, and greater than 1 is a hyperbola. The term derives its name from the parameters of conic sections, as every Kepler orbit is a conic section. It is normally used for the isolated two-body problem, but extensions exist for objects following a rosette orbit through the Galaxy.

For most numbered asteroids, almost nothing is known apart from a few physical parameters and orbital elements. Some physical characteristics can only be estimated. The physical data is determined by making certain standard assumptions.

(292220) 2006 SU49, provisional designation 2006 SU49, is a sub-kilometer asteroid, classified as near-Earth object and potentially hazardous asteroid of the Apollo group that had a small chance of impacting Earth in 2029.

(179806) 2002 TD66 (also written 2002 TD66) is a sub-kilometer asteroid, classified as near-Earth object of the Apollo group. It was discovered on 5 October 2002, by the LINEAR project at Lincoln Laboratory's ETS in Socorro, New Mexico. It was announced on 7 October 2002 and appeared later that day on the JPL current risk page.

<span class="mw-page-title-main">Lost minor planet</span> Asteroids whose orbits are not known accurately enough to find them again

A minor planet is "lost" when today's observers cannot find it, because its location is too uncertain to target observations. This happens if the orbital elements of a minor planet are not known accurately enough, typically because the observation arc for the object is too short, or too few observations were made before the object became unobservable.

(5496) 1973 NA, is a very eccentric and heavily tilted asteroid, classified as near-Earth object of the Apollo group, approximately 2 kilometers in diameter. It was discovered on 4 July 1973, by American astronomer Eleanor Helin at the U.S. Palomar Observatory in California. At the time of its discovery, it was the most highly inclined minor planet known to exist. It may be the parent body of the Quadrantids.

(153814) 2001 WN5 is a sub-kilometer asteroid, classified as near-Earth object and potentially hazardous asteroid of the Apollo group.

(467336) 2002 LT38, is a sub-kilometer asteroid and suspected tumbler, classified as a near-Earth object and potentially hazardous asteroid of the Aten group, approximately 240 meters (790 ft) in diameter. It was discovered on 12 June 2002, by astronomers of the Lincoln Near-Earth Asteroid Research at the Lincoln Laboratory's Experimental Test Site near Socorro, New Mexico, in the United States.

<span class="nowrap">(367789) 2011 AG<sub>5</sub></span> Near-Earth asteroid in 2040

(367789) 2011 AG5, provisional designation 2011 AG5, 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 meters (460 ft). 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 2011 AG5 is 0.0004 AU (60,000 km; 0.16 LD)

<span class="mw-page-title-main">367943 Duende</span> Near-Earth object

367943 Duende (provisional designation 2012 DA14) is a micro-asteroid and a near-Earth object of the Aten and Atira group, approximately 30 meters (98 ft) in diameter. It was discovered by astronomers of the Astronomical Observatory of Mallorca at its robotic La Sagra Observatory in 2012, and named for the duende, a goblin-like creature from Iberian and Filipino mythology and folklore. Duende is likely an uncommon L-type asteroid and significantly elongated. For an asteroid of its size, it has a relatively long rotation period of 9.485 hours.

(471240) 2011 BT15, provisional designation 2011 BT15, is a stony, sub-kilometer sized asteroid and fast rotator, classified as a near-Earth object and potentially hazardous asteroid of the Apollo group. It had been one of the objects with the highest impact threat on the Palermo Technical Impact Hazard Scale.

In observational astronomy, the observation arc of a Solar System body is the time period between its earliest and latest observations, used for tracing the body's path. It is usually given in days or years. The term is mostly used in the discovery and tracking of asteroids and comets. Arc length has the greatest influence on the accuracy of an orbit. The number, spacing of intermediate observations, and timestamps have a lesser effect.

<span class="nowrap">(66063) 1998 RO<sub>1</sub></span> Stony near-Earth object of the Aten group

(66063) 1998 RO1 is a stony near-Earth object of the Aten group on a highly-eccentric orbit. The synchronous binary system measures approximately 800 meters (0.50 miles) in diameter. It was discovered by astronomers of the Lincoln Near-Earth Asteroid Research at the Lincoln Laboratory's Experimental Test Site near Socorro, New Mexico, on 14 September 1998.

2010 GZ60 was originally estimated by JPL to be a near-Earth asteroid approximately 2 kilometers (1.2 miles) in diameter. But is now known to be an asteroid from the inner region of the asteroid belt that does not get closer than 1.5 AU (220 million km) to Earth.

2013 GM3 is a micro-asteroid, classified as near-Earth object of the Aten group, approximately 20 meters in diameter. It was first observed on 3 April 2013, by astronomers of the Mount Lemmon Survey conducted at the Mount Lemmon Observatory near Tucson, Arizona, United States.

(385343) 2002 LV, provisional designation 2002 LV, is a stony asteroid on a highly eccentric orbit, classified as near-Earth object and potentially hazardous asteroid of the Apollo group, approximately 1.5 kilometers in diameter. It was discovered on 1 June 2002, by astronomers with the Lincoln Near-Earth Asteroid Research at the Lincoln Laboratory's Experimental Test Site near Socorro, New Mexico, in the United States. The Sr-type asteroid has a rotation period of 6.2 hours and is likely elongated.

2021 PH27 is a near-Earth asteroid of the Atira group. It was discovered by Scott Sheppard using the Dark Energy Survey's DECam imager at NOIRLab's Cerro Tololo Inter-American Observatory on 13 August 2021. 2021 PH27 has the smallest semi-major axis and shortest orbital period among all known asteroids as of 2021, with a velocity at perihelion of 106 km/s (240,000 mph). It also has the largest relativistic perihelion shift of any object orbiting the Sun, 1.6 times that of Mercury. With an absolute magnitude of 17.7, the asteroid is estimated to be larger than 1 kilometer (0.6 miles) in diameter.

References

  1. "Orbits for Near Earth Asteroids (NEAs)". Minor Planet Center. International Astronomical Union . Retrieved 25 June 2020. via "M.P. Orbit Format". Minor Planet Center. International Astronomical Union.
  2. 1 2 3 4 "Uncertainty parameter 'U'". Minor Planet Center. International Astronomical Union . Retrieved 15 November 2011.
  3. 1 2 3 "Trajectory Browser User Guide". Ames Research Center. Mission Design Center Trajectory Browser. NASA . Retrieved 3 March 2016.
  4. Editorial Notice (PDF) (Report). The Minor Planet Circulars / Minor Planets and Comets. 1995-02-15. p. 24597. MPC 24597–24780. Retrieved 3 March 2016.
  5. 1 2 Drake, Bret G. (2011). Strategic implications of human exploration of near-Earth asteroids (Report). NASA Technical Reports. NASA. 2011-0020788. Retrieved 3 March 2016.
  6. "Definition / description for SBDB parameter / field: condition code". JPL Solar System Dynamics. Retrieved 15 November 2011.
  7. 1 2 3 4 "Export format for minor-planet orbits". Minor Planet Center. International Astronomical Union . Retrieved 3 March 2016.
  8. "Near-Earth objects close-approach uncertainties". JPL Near-Earth Object Program Office. NASA / JPL. 31 August 2005. Archived from the original on 24 March 2004. Retrieved 15 November 2011.
  9. "2003 UU291". Minor Planet Center. International Astronomical Union.
  10. Desmars, Josselin; Bancelin, David; Hestroffer, Daniel; Thuillot, William (Jun 2011). Alecian, G.; Belkacem, K.; Samadi, R.; Valls-Gabaud, D. (eds.). "Statistical analysis on the uncertainty of asteroid ephemerides". SF2A 2011: Annual Meeting of the French Society of Astronomy and Astrophysics. Paris, France: 639–642. Bibcode:2011sf2a.conf..639D . Retrieved 3 March 2016.