Jump to content

Mass concentration (astronomy)

From Wikipedia, the free encyclopedia

This is an old revision of this page, as edited by 67.71.37.102 (talk) at 20:54, 20 July 2016. The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

For mass concentration in chemistry, see Mass concentration (chemistry).
Topography (top) and corresponding gravity (bottom) signal of lunar Mare Smythii containing a significant mascon.

In astronomy and astrophysics, a mass concentration (or mascon) is a region of a planet or moon's crust that contains a large positive gravitational anomaly. In general, the word "mascon" can be used as a noun to describe an excess distribution of mass on or beneath the surface of an astronomical body (with respect to some suitable average), such as is found around Hawaii on Earth.[1] However, this term is most often used to describe a geologic structure that has a positive gravitational anomaly associated with a feature (e.g. depressed basin) that might otherwise have been expected to have a negative anomaly, such as the "mascon basins" on the Moon.

Typical examples of mascon basins on the Moon are the Imbrium, Serenitatis, Crisium and Orientale impact basins, all of which exhibit significant topographic depressions and positive gravitational anomalies. Examples of mascon basins on Mars include the Argyre, Isidis, and Utopia basins. Theoretical considerations imply that a topographic low in isostatic equilibrium would exhibit a slight negative gravitational anomaly. Thus, the positive gravitational anomalies associated with these impact basins indicate that some form of positive density anomaly must exist within the crust or upper mantle that is currently supported by the lithosphere. One possibility is that these anomalies are due to dense mare basaltic lavas, which might reach up to 6 kilometers in thickness for the Moon. While these lavas certainly contribute to the observed gravitational anomalies, uplift of the crust-mantle interface is also required to account for their magnitude. Indeed, some mascon basins on the Moon do not appear to be associated with any signs of volcanic activity. Theoretical considerations in either case indicate that all the lunar mascons are super-isostatic (that is, supported above their isostatic positions). The huge expanse of mare basaltic volcanism associated with Oceanus Procellarum does not possess a positive gravitational anomaly.

Because of its mascons, the Moon has only four "frozen orbit" inclination zones where a lunar satellite can stay in a low orbit indefinitely. Lunar subsatellites were released on the last three Apollo manned lunar landing missions in 1971 and 1972; the subsatellite PFS-2 released from Apollo 16 was expected to stay in orbit for one and a half years, but lasted only 35 days before crashing into the lunar surface. It was only in 2001 that the mascons were mapped and the frozen orbits were discovered.[2]

Effect of lunar mascons on satellite orbits

Lunar mascons alter the local gravity above and around them sufficiently that low and uncorrected satellite orbits around the Moon are unstable on a timescale of months or years. The small perturbations in the orbits from passes through these regions accumulate and eventually distort the orbit enough that it destabilizes and the satellite impacts the surface.

The Luna-10 orbiter was the first artificial object to orbit the moon and it returned tracking data indicating that the lunar gravitational field caused larger than expected perturbations presumably due to 'roughness' of the lunar gravitational field.[3] The Lunar mascons were discovered by Paul M Muller and William L Sjogren of the NASA Jet Propulsion Laboratory (JPL) in 1968[4] from a new analytic method applied to the highly precise navigation data from the unmanned pre-Apollo Lunar Orbiter spacecraft. This discovery observed the consistent 1:1 correlation between very large positive gravity anomalies and depressed circular basins on the moon. This fact places key limits on models attempting to follow the history of the moon's geological development and explain the current lunar internal structures.

At that time, one of NASA's highest priority "tiger team" projects was to explain why the Lunar Orbiter spacecraft being used to test the accuracy of Project Apollo navigation were experiencing errors in predicted position of ten times the mission specification (2 kilometers instead of 200 meters). This meant that the predicted landing areas were 100 times as large as those being carefully defined for reasons of safety. Lunar orbital effects principally resulting from the strong gravitational perturbations of the MASCONS were ultimately revealed as the cause. William Wollenhaupt and Emil Schiesser of the NASA Manned Spacecraft Center in Houston then worked out the "fix" [5][6][7] that was first applied to Apollo 12 and permitted its landing within 163 meters of the target, the previously-landed Surveyor 3 spacecraft.[8]

In May 2013 a NASA study was published with results from the twin GRAIL probes, that mapped mass concentrations on Earth's moon.[9]

See also

References

Cited references

  1. ^ Richard Allen. "Gravitational Constraints (Lecture 17)" (PDF). Berkeley course: Physics of the Earth and Planetary Interiors. p. 9. Retrieved 2009-12-25.
  2. ^ "Bizarre Lunar Orbits". NASA Science: Science News. NASA. 2006-11-06. Retrieved 2012-12-09.
  3. ^ "Luna 10 (NASA)".
  4. ^ Paul Muller; William Sjogren (1968). "Mascons: lunar mass concentrations". Science. 161 (3842): 680–684. Bibcode:1968Sci...161..680M. doi:10.1126/science.161.3842.680. PMID 17801458. {{cite journal}}: Unknown parameter |lastauthoramp= ignored (|name-list-style= suggested) (help)
  5. ^ Jennifer Ross-Nazzal (2 November 2006). "NASA JOHNSON SPACE CENTER ORAL HISTORY PROJECT Oral History Transcript" (PDF). http://www.jsc.nasa.gov. Retrieved 12 November 2015. Bill [Wilbur R.] Wollenhaupt from JPL joined my group. He and I and Bill [William] Boyce and some others traveled to Langley, and met with the Langley people over the weekend, we spent the whole time reprocessing Langley Lunar Orbiter data day and night. {{cite web}}: External link in |website= (help)
  6. ^ Jennifer Ross-Nazzal (7 December 2006). "NASA JOHNSON SPACE CENTER ORAL HISTORY PROJECT Oral History 2 Transcript" (PDF). http://www.jsc.nasa.gov. Retrieved 12 November 2015. Somewhere about this time Wilbur R. Wollenhaupt, who went by Bill, joined our group. He had extensive background in ground-based navigation at JPL. He was pretty familiar with the JPL Deep Space Network (DSN) Trackers after which the Apollo trackers were patterned. {{cite web}}: External link in |website= (help)
  7. ^ Malcolm Johnston; Howard Tindall (31 May 1996). "Tindallgrams" (PDF). http://www.collectspace.com. Retrieved 12 November 2015. If this determination, using the LM data, disagrees substantially with the other data sources, we must consider the possibility that it's due to gravity anomalies. The sort of differences we are willing to tolerate is 0.3° in longitude, which is more or less equivalent to 0.3° pitch misalignment in the platform. True alignment errors in excess of that could present ascent guidance problems. Since 0.3° is equivalent of about five miles, you'd expect the crew's estimate of position could probably be useful in determining the true situation. All they'd have to do is tell us they are short or over-shot the target point a great deal. {{cite web}}: External link in |website= (help)
  8. ^ "Encyclopedia Astronautica : Apollo 12".
  9. ^ Chow, Denise. "Mystery of Moon's Lumpy Gravity Explained". SPACE.com. Retrieved 31 May 2013.

General references

Retrieved from "https://en.wikipedia.org/w/index.php?title=Mass_concentration_(astronomy)&oldid=730727731"