Showing posts with label Lunar Magnetic Anomalies. Show all posts
Showing posts with label Lunar Magnetic Anomalies. Show all posts

Wednesday, September 14, 2016

Disrupted Terrain at the Antipodes of Young Great Basins

A new study of areas diametrically opposite from the Moon's youngest basins goes beyond crustal magnetic fields and swirl albedo features found at these focal points and proposes examples of highly modified terrain. Animation from preliminary lunar crust thickness maps prepared from GRAIL (2012) data by the Science Visualization Studio. [NASA/GSFC].
Joel Raupe
Lunar Pioneer

Studying the lunar magnetic anomalies and albedo swirls nested near the antipodes, at those points that are absolute opposite on the Moon from its youngest basins, can be a little disorienting. The antipodes of the two most familiar nearside basins Mare Imbrium and Mare Serenitatis, for example, are also near the mountainous northwest and northern border region of the vast (and more ancient) South Pole-Aitken (SPA) basin.

Such simple facts as these, derived during the relatively short history of modern lunar exploration, camouflage a variety of unknowns and complexities, as well as some controversy over the origin of the peculiar features discovered there.

Within ten degrees of the farside coordinates diametrically opposite from the officially designated center of Mare Imbrium, close to the surface, is a fairly well-known local magnetic field. Associated with this crustal magnetism is one of the Moon's most familiar tracings of delicate and bright albedo "swirls," apparently composed of a very thin layer of fine dust of the sort of low optical maturity, a signature of the Moon's youngest features draped over its oldest.

Like some kind of alien graffiti, these swirls really stand out as attributes of Mare Ingenii, the largest lava-flooded plain on the farside, a hemisphere almost as devoid of "seas" as the Moon's Earth-facing side is covered by them.

The Ingenii swirl fields are a highlight of anyone's tour of the Moon. To start considering these giant swirls traced over the surface of Ingenii as integral to Mare Imbrium on the Moon's nearside can sometimes seem like reading through a mirror.

Mare Imbrium is probably the most easily detected 'naked-eye feature' of the tidally-bound Earth-facing hemisphere. Centered officially by the IAU at 34.72°N, 345.09°E, the corresponding, though still preliminary, antipode for the Imbrium basin should be near 34.72°S,165.09°E, on the farside's southern hemisphere.

The antipode of Mare Imbrium (yellow spot) was a foci of conjoining seismic shock and ejecta from the epoch-changing basin-forming impact that hollowed out Mare Imbrium, roughly 3.85 billion years ago. Persistent bright surface markings that have lasted beyond the 800 million to 1 billion years thought to inevitably darken lunar regolith are thought to be the result of a cyclical interaction of charged lunar dust precipitating through the locally intense magnetic field. The white rectangle outlines one of many areas of disrupted terrain, "material of grooves and mounds" identified on the geological map of Stuart-Alexander (1978). LROC Wide Angle Camera (WAC) monochrome mosaic [NASA/GSFC/Arizona State University].
When we think of the clusters of features often found together near these points directly opposite from the Moon's nearside basins it's often easier to label Mare Ingenii as Imbrium Antipode, and the Gerasimovich region as Crisium Antipode, etc.

This unconventional labeling emerges as we study a whole family of, literally, "far-flung phenomena," though most of the species, fortunately, are not yet associated with a local name. Unlike the more easily spotted features at Mare Ingenii, now thought to have originated with Mare Imbrium, such features elsewhere are less easily picked out, overlapping widely differing terrains and a variety of mountain ranges, plains and crater groups.

A very distinctive bifurcated swirl, one of many similar, striking aspects of Mare Ingenii, on the Moon's farside and immediately adjacent to the antipode of Mare Imbrium. From an oblique LROC NAC observation M191830503R, LRO orbit 13304, May 16, 2012 [NASA/GSFC/Arizona State University].
The point on the Moon opposite Mare Serenitatis is not as distinctive (see image below). The coordinates were easy enough to determine, like the Imbrium Antipode it's just inside the circumference of SPA basin, a little north and east the antipode of Imbrium as Serenitatis basin, on the nearside, is a little south and east of Imbrium.

Like most of the farside, however, there is no mare-inundated plain near the Serenitatis antipode to allow for a clear photographic contrast with local differences in albedo. The crustal magnetism (or the granularity of our data) seems more diffuse, with smaller, less intense knots of crust magnetism.

The absence on the Moon of the kind of global magnetic field that affords life so much welcome protection here on Earth was one of the earliest conclusions of modern lunar exploration. As men and machines transited to and from the surface, however, the magnetic picture became more complex. The earliest magnetometers, in orbit and on the surface, were detecting magnetic signatures bound to local features, but their local intensity and apparent close association of with surfaces that seemed to defy aging were only beginning to be grasped.

The Serenitatis Antipode is not as easy for the naked eye to pick out from the background as points opposite the Imbrium basin associated with Mare Ingenii. The antipode of Serenitatis is marked with a cross in frame one (Figure 5 from the study by Hood, et al (2013). In that same frame the authors draw attention to mountains along the rim of SPA basin (white arrows) as possible examples of terrain disrupted by the Serenitatis basin-forming impact here near the opposite point on the Moon. The frame following draws attention to two anomalous optically immature surface areas within Galois Q crater, followed by Clementine color ratio analysis where the older terrain (red) surface areas stand out with characteristics of new (blue) and reflective regolith fines. The twin patches coincide with a local magnetic field strength "bump" measuring 9nT. The final frame shows the same albedo patches at 77 meters resolution in LROC Wide Angle Camera (WAC) observation M160959807C (604 nm), spacecraft orbit 8854, May 25, 2011, angle of incidence 62° from 60 km [NASA/USGS/DOD/GSFC/Arizona State University].
As the Apollo era came to an end it was understood, at least, that the Moon seemed once to have had an internal dynamo like Earth, generating global magnetism fossilized today in its rocks. A higher resolution picture of the Moon's magnetism and its interrelation with the Sun, Earth and its own dust would wait for a second very slowly renewed period of unmanned exploration beginning with vehicles like the DOD remote sensing test platform Clementine (1994).

At the close of the 20th century the remarkable Lunar Prospector (1998-1999) helped add important pieces to the picture. Specifically, the small vehicle returned highly valued data on the Moon's local magnetic fields very close to the surface, as it was gradually lowered toward a planned impact within the permanently shadowed Shoemaker crater, a feature of the far lunar south today baring the name of the celebrated pioneer Gene Shoemaker (1928-1997) who originally planned the impact that inspired the LCROSS mission ten years later.

Investigators have continued to correct and tease valuable information from the sparse Lunar Prospector magnetometer data to this day. The data sometimes allowed identifying lunar features in a manner opposite than before. Reiner Gamma, the most familiar swirl phenomena in Oceanus Procellarum, stands out in low power telescopes. Its associated crustal magnetism was identified later. Elsewhere on the nearside magnetometer data from as few as one to three late mission low orbital passes by Lunar Prospector allowed diffuse albedo patches at Airy and Descartes to be definitively associated with locally intense crustal magnetism and identified as true "swirl phenomena."

Figure 9 from Hood, et al (2013) - Superposition of the two-dimensionally filtered magnetic field magnitude at approximately 25 km altitude (Lunar Prospector), contour interval 1 nano-Tesla, onto LROC WAC mosaic of the nearside, in the south-central highlands vicinity of the Apollo 16 landing site.
Simulated oblique view over ancient Descartes crater (29 km - 11.74°S, 15.66°E), from the Cayley Formation plains explored by Young and Duke on the Apollo 16 expedition (1972) in the northwest around 80 km southeast over the "disrupted terrain" of the Descartes Formation, highlighting its anomalous albedo, not coincidentally at the heart of one of the Moon's most intense crustal magnetic fields. LROC WAC mosaic, from observations collected in three sequential orbital passes December 3, 2011, averaging 52 meters resolution from 38 km - Figure 5 from "Boulder 668 at Descartes C," July 17, 2012 [NASA/GSFC/Arizona State University].
At Orientale Antipode, opposite from what is the Moon's unequivocally youngest basin, the swirl field is very widespread, associated with more than a few peaks in local crustal magnetism. The largest affected feature on the opposite side of the Moon from Mare Orientale is Mare Marginis, characterized by what is likely the Moon's largest and most complex field of swirls at the surface, overlapping every kind of terrain, but also closely identified with the Goddard and Goddard A crater. Still, the actual boundaries of this field of 'persistent albedo patterns' are difficult to trace.

Adding to this complexity, the swirl field near Orientale Antipode has been affected by relatively recent impacts, some with brightly reflective rays. The field is spread far enough east, extending over the farside's mid-latitudes, it's difficult to say with certainty whether an unnamed, tightly wound spectacular swirl field east of Firsov crater belongs to the group.

The Orientale Antipode (near Goddard A) is characterized by very widespread swirls. The greater manifestation (large oval) extends far from the pronounced magnetic field lines of peak strength near Hubble, Goddard and Goddard A craters east nearly to a distant and weaker peak field strength associated with the spectacular field of swirls seemingly spilling out from a bright unnamed Copernican crater east of Firsov (4.204°N, 112.697°E). LROC WAC global 100 meter mosaic [NASA/GSFC/Arizona State University].
Three investigators with established planetary science resumes which include (among many other things) peer-reviewed study of these bright swirl 'patterns' and associated lunar magnetic anomalies, have recently authored a new study building on continued fine-tuning of Lunar Prospector (1998-1999) magnetometer data and the more recent Lunar Reconnaissance Orbiter (LRO) Wide Angle Camera (WAC) surveys.

The new paper, published in the Journal of Geophysical Research, “Origin of Strong Lunar Magnetic Anomalies: More Detailed Mapping and Examination of LROC Imagery in Regions Antipodal to Young Large Basins,” demonstrates further the recent end to a long controversy, helping answer the Space Age mystery posed by the Moon’s delicate, bright, often sinuous surface albedo patterns.

A crew member on-board Apollo 10 almost managed to capture the full length of the magnificent but unnamed surficial albedo swirl field now associated with a measurable peak in crustal magnetism east of Firsov crater. AS10-30-4365 [NASA].
As with most controversies on the long climb of science, a quiet resolution drew upon bits and pieces collected in pursuit of answers to many, often unrelated, questions.

Launched in early 1998, Lunar Prospector spent 19 months in a low polar orbit and became notorious for a remarkably low budget and high return of valued data as much as for improved mapping of the scattered neutron absorption strongly hinting at the presence of volatiles, specifically hydrogen, prematurely ruled out following early analysis of Apollo samples in 1969.

In 2013 terms, for the amount of money the federal government collects, borrows and spends every eight and a half minutes Lunar Prospector gained a well-deserved reputation and confirmed still skeptically-received indications of the presence of hydrogen, both inside and outside the permanently shadowed regions of the Moon’s polar latitudes.
“Will your grace command me any service to the world's end?  I will go on the slightest errand now, to the Antipodes that you can devise to send me on…”
- Much Ado About Nothing, (Act II, scene 2)
The planned mission-ending impact of Lunar Prospector on the permanently shadowed floor of Shoemaker crater, near the Moon’s South Pole, July 30, 1999 (a long-shot, ultimately unsuccessful attempt to send up a plume of volatiles detectable from Earth), inspired the very successful LCROSS mission, launched together with LRO, a decade later.

With its neutron spectrometer, mapping the absence, the absorption, of scattered neutrons indicative of hydrogen, possibly water ices, near the lunar poles, Lunar Prospector also deployed a sensitive magnetometer.

The Moon’s lack of an Earth-like global magnetic field was well known, though Apollo and Luna surface samples clearly indicated the Moon may once have had the kind of molten internal dynamo at its core we take for granted on Earth, a now-dormant generator sufficient for global magnetism, its signature locked into the lineup direction of certain materials as volcanic rock cooled in its earliest ages, some of these as much as a billion years apart. The magnetic fields detected at the surface and from orbit, speculation held, were likely fossilized remnants, surviving islands – though the presence of “lunar magnetic anomalies” on the Moon’s Farside, in concentrations near opposite on the Moon (antipodal) from the Nearside’s large basins was seen as an unlikely coincidence very early in post-Apollo studies.

Along with anomalous local crustal magnetism detected near the Moon’s most famous “swirl,” the alluring Reiner Gamma, bright against the darker background of Oceans Procellarum, and the presence of swirls, some of them spectacular, in vicinity of these islands of knotted magnetic field lines - at the antipodes of Mare Imbrium and Serenitatis - was impossible to ignore.

Very near the Antipodes of Mare Imbrium in particular, the earliest photographs of the Moon’s Farside unveiled a spectacular swirl “field,” seeming almost intelligent in origin, Minimalist butterflies or spiders, strange forms seemed lightly painted in white on the darker floor of the melt-inundated basin floor of Mare Ingenii, by some inscrutable giant almost evoking the walls and ceilings of the cave of Lascaux, or the Nazca Lines.

“Swirls” seem immune from “optical maturity,” an inevitable darkening (really reddening) by solar and cosmic radiation. Incessant bombardment should inevitably weather fade such contrast to match its surroundings, on a timescale between 800 million to 1 billion years.

Had there had been any indication the bright patterns were composed of rough, fresh and reflectively bright small ejecta, like the rays of young 109 million year old Tycho, for example, a predictable cycle of meteorite and micro-meteorite “gardening” turns over the upper 3 centimeters of the entire lunar surface each two million years. Space weather, therefore, should have contributed to their erasure. It was a strong argument for direct, or lacking any difference in the crater counts inside and outside the swirls, indirect encounters with comets.

The comet encounter theory for the origin of lunar swirls died hard. Proponents pointed to the optical immaturity, the undeniably fresh material of the brighter surface, and claimed this to be evidence that outweighed other factors.

The predominance of Farside swirls gathered near places opposite from the Nearside basins and in the presence of coincident local crustal magnetism, they wrote, pointed perhaps to relatively recent and oblique encounters with comets interacting electro-chemically with these unusual conditions. The still-interesting fact that Reiner Gamma, and two lesser known magnetic anomalies with accompanying bright albedo patches on the Nearside seemed to lack any identified basins at their opposing antipodes on the Farside, they claimed, was also exceptional.

As the recorded readings measured from the Lunar Prospector magnetometer were gradually corrected, properly matched with time, the pressures of sunlight, etc., over many years following the end of that mission in 1999, researchers began discovering, or confirming, the existence of swirls after first deciphering the location of smaller, though sometimes intense, magnetic fields.

Ironically, the most intense magnetic field detected by any of the Apollo surface expeditions, that of Apollo 16, was measured only 80 km northwest of possibly the most intense crustal magnetism on the Moon, together with the amorphous small brighter surface material of the Descartes Formation. John Young and Charlie Duke walked on the northwestern edge of this feature when sampling the Cinco craters on “Stone Mountain,” overlooking South Ray crater, in April 1972.

The Lunar Prospector magnetometer survey of the Moon made for an improvement on earlier maps, but the mission was not comprehensive. Its advantage, at the time, was an unprecedented low orbit, an orbital altitude gradually lowering more and more as the vehicle approached its demise. The data had an inherent high degree of accuracy because of improvements in electronics and hardened electronics since the Apollo era, and a value-added accuracy due to the patience and hard work of investigators properly pegging the to geography and time, in filtering out the noise long after Lunar Prospector was gone.

Much of what is now known about the lunar magnetic anomaly on the Descartes highland hugging the northern edge of ancient Descartes crater, was teased from its measurements taken through three late mission orbits, when Lunar Prospector orbited some 32 km first over the east, and in the next orbit passing directly over Descartes, and last over the west.

Hood and Richmond, authors of this latest study, published their examination of the Lunar Prospector encounter with Descartes in 2003, determining the intensity of the very local magnetic field sufficient to refract the solar wind, dubbing it a “mini-magnetosphere.”

At nearly the same time, similarly strong local magnetic anomalies, though slightly less intense and localized, were shown embedded on the Farside at Gerasimovich, and perhaps elsewhere.

Some were quick to speculate, if a crustal magnetism centered on the Descartes formation were strong enough to refract the solar wind, perhaps such protection prevented the dusty surface of the bright “swirl” on the southern half of “Stone Mountain” from becoming “optically mature.”

The authors were quick to point out in their introductory paper even such an obviously intense local magnetic field offered no protections from heavier cosmic radiation. The depth of the cavity in the solar wind formed by Descartes magnetic anomaly was insufficient to stop highly energetic, and heavy, nucleons traveling – unlike the particles of a solar wind – close to the speed of light. They estimated such a purpose would require a magnetic field 2,000 km across just to begin deflecting highly energetic cosmic rays away from the surface within the fields. Naturally, such a field would have no effect on the patient and steady rain of micro-meteorites adding to the surface maturity.

Ignoring, for the moment, most magnetic anomalies with their attendant swirls are not sufficiently intense to carve out a transitory cavity in the solar wind, the authors demonstrated the most astonishingly enduring, and intense magnetic field ever detected near the lunar surface was no protection from space weathering.

By all rights, the surfaces within their influence should be darkening at or close to the same rate as the lunar surface elsewhere.

Enter Kaguya, Chandrayaan, LRO…

Toppography.

For decades the nature and the origin or the swirl patterns stirred very minor controversy, in planetary science communities. Those who insisted lunar swirls originated from comet encounters

Early in the Space Age investigators concluded our Moon, unlike Earth,

One place suggested as a possible location for samples of the SPA basin is northeast of Plato, where, between that famous crater and the long northern edge of Mare Frigoris, probability points toward the possible existence of a debris pile, the antipodes of the South Pole-Aitken basin.

In this latest study, Hood, Richmond and Spudis add granularity to our understanding the relationship between basin forming impacts and how they modify the landscape at the most remote points possible, as far away from Ground Zero as anyone can get, and remain on the Moon.

Anyone can meditate on Mare Imbrium, for example, and see how energetic the pressure wave, racing away from the center of the impact, scoured out mountains and channels and hurled away and dumped unimaginable masses of melt and solid debris many hundreds of kilometers away. The scar has not been erased, and a significant amount of debris must have been ejected at escape velocity. Much of that material eventually returned or settled elsewhere in the Solar System.

On February 15, 2013, as many in the far-flung world’s astronomy community were preparing to observe an exceptionally close fly-by of asteroid 2012 DA14, out of the glare of the pre-dawn over Central Asia a 7,000 ton, 15 meter-wide rock encountered Earth’s atmosphere at a relative speed of 18 km per second. Immediately flaring bright, it quickly exploded 20 km overhead. The event produced a shockwave into the atmosphere over Chelyabinsk that immediately imparted ten times the energy of the fission bomb exploded over Hiroshima in 1945. The sound of that smaller asteroid’s explosion traveled around the entire planet several times before seismic stations of the world could detect it no longer.

The pressure wave from the Chelyabinsk Event propagated in every direction away from the explosion until all points on the wave converged west-southwest of South America, where the far South Pacific borders the Great Southern Ocean encircling Antarctica. The momentum of the wave through the atmosphere carried past this convergence point, the Antipode of the Chelyabinsk Event, and continued racing away until a second convergence occurred many hours later, back over Russia, where the energy continued on toward the antipode a second time, and so on, like ripples in a pond – only the pond, in this case, was a planet, and its shoreline a single point on the opposite side of the world.


Related Posts:
Bubble, Bubble – Swirl and Trouble (July 19, 2012)
Boulder 668 at Descartes C (July 16, 2012)
LROC: The Swirls of Mare Ingenii (June 22, 2012)
Remnant magnetism hints at once-active lunar core (January 27, 2012)
Grand lunar swirls yielding to LRO Mini-RF (October 4, 2010)
Another look at Reiner Gamma (June 30, 2010)
LOLA: Goddard (June 26, 2010)
Depths of Mare Ingenii (June 16, 2010)
LROC: Ingenii Swirls at Constellation Region of Interest (May 26, 2010)
Local topography and Reiner Gamma (May 22, 2010)
Lunar swirl phenomena from LRO (May 17, 2010)
The still-mysterious Descartes formation (May 11, 2010)
Dust transport and its importance in the origin of lunar swirls (February 21, 2010)
The Heart of Reiner Gamma (November 17, 2009)
Moon’s mini-magnetospheres are old news (November 16, 2009)
MIT claim of solving ‘lunar mystery’ unfounded (January 15, 2009)

Wednesday, June 19, 2013

The Moon's antipodal magnetism mystery

A new study of areas on the Moon opposite (at the antipodes) of the Moon's youngest basins goes beyond long-studied crustal magnetic anomalies and the albedo "swirls" at those opposite coordinates to demonstrate "highly modified terrain" at these opposing points. Animation from preliminary lunar crust thickness maps derived from GRAIL (2012) data by the Science Visualization Studio. [NASA/GSFC].
Paul D. Spudis
The Once and Future Moon
Smithsonian Air & Space


Although the Moon has no global magnetic field like the Earth, small areas on its surface are magnetized.  These fields are not systematically distributed and in general are very weak.  In trying to explain their mysterious presence and origin, several ideas have been advanced.

Rocks typically acquire magnetism (called remnant magnetism) by cooling in the presence of a magnetic field.  At temperatures greater than about 570° C (the so-called Curie point), a rock cannot retain a magnetic signature.  But if it cools below the Curie point, it assumes an induced magnetic field oriented in the same direction as the field in which it cooled.  Unfortunately, on the Moon most rocks have been dislodged from their original orientations by impact processes, so we do not know whether a given rock cooled in the presence of a global (presumably uniform strength and direction) or local (randomized) magnetic field.

We knew the Moon had no global magnetic field before the Apollo crews landed, so it was a bit surprising to learn that some of the returned lunar rocks are strongly magnetized.  Because these rocks are all very old (usually much older than 3 billion years), it was thought that they recorded an ancient epoch when the Moon might have had a global magnetic field, now vanished for some reason.

This finding from the lunar samples was complemented by measurements from orbit that show small areas (10s to 100s of kilometers across) of the surface to be magnetized.  These areas occur all over the Moon and are not associated exclusively with either the dark volcanic maria or the bright highlands crust.  However, they do tend to have two peculiar properties.  First, we find strange “grooved” terrain associated with some of the strongest magnetic anomalies.  This terrain is unlike any other lunar landform – it consists of ridges and valleys that cover the walls and sides of craters and mountains.  Second, these magnetic anomalies tend to occur at the antipodes of (180° away on the opposite side of the globe from) the largest and youngest lunar multi-ring impact basins.  These are curious properties indeed.  What might it mean?

For years, many have pondered and worked on this dilemma.  One idea was developed that perhaps these magnetic anomalies are formed during basin impact.  It was proposed that seismic shaking from these enormous impacts created the grooved terrain and induced fractures in the crust at the antipode, into which hot volcanic magma was injected.  After cooling these dikes assumed remnant magnetism from a global dipole field.  Yet another idea contends that the concentration of magnetized material is a result of antipodal convergence of basin ejecta, which arrived hot from basin formation, collected at the antipode and cooled through the Curie point there.  This last model has the advantage that it might also explain the presence of the grooved terrain, which might have formed by the arrival of basin ejecta on the surface from impacts coming from all directions simultaneously.

Though islands of crustal magnetism are strongly associated with points diametrically opposite from basin forming impacts, these magnetic anomalies are also often offset from those antipodal points. Above, the ring of the Moon's youngest basin Schrödinger, in the far lunar south, is mirrored on the area on the direct opposite side of the Moon in the far lunar north. The absolute antipode is in the vicinity of Anaximenes H. The crustal magnetism mapped using Lunar Prospector data seems at its highest near Catena Sylvester. Terrain cited as greatly disrupted seismically is further still from the Schrödinger antipode, at craters Froelich and Lovelace, just beyond this field of view, at upper right [NASA/GSFC/ASU].
My colleague Lon Hood from the University of Arizona has been studying magnetic anomalies for many years and is an advocate of the last model described above.  Hood was studying some previously ignored, smaller magnetic anomalies found around the Moon that had no explanation. He asked me about the geological setting of one particular magnetic anomaly on the Moon that had yet to be described in detail.  This one occurs in highlands near the north pole of the Moon and had not been previously studied in detail.

I have been something of a skeptic for many years about the basin/antipode relation for magnetic anomalies.  Part of the reason for my position is the problem of Reiner Gamma, which is a bright patch on the lunar surface that has one of the highest magnetic field strengths on the Moon.  The problem is that Reiner Gamma is nowhere near the antipode of any basin and shows no evidence for any grooved terrain.  So I thought that this was the exception that disproves the rule.
“Will your grace command me any service to the world's end?  I will go on the slightest errand now, to the Antipodes that you can devise to send me on…”
- Much Ado About Nothing, (Act II, scene 2)

Nonetheless, I was intrigued by Hood’s finding and decided to examine the area.  To my astonishment, I found wall textures very similar to the famous grooved terrain in the walls of the craters Lovelace and Froelich (not exactly coincident with the anomaly, but very close).  I can see no obvious reason for such terrain development; it appears to be highly restricted in its distribution and is not a fresh feature.  Judging from its degraded appearance, it is rather old.

So, is there a basin antipodal to Lovelace and Froelich?  Indeed there is – the fabulous Schrödinger basin, one of the smaller lunar basins at 325 km diameter, located near the south pole of the Moon.  Before our study, I probably would have thought that Schrödinger was too small to create any global-scale effects, but we don’t fully understand the effects of impact with increasing size and there is no good alternative explanation for the wall textures of these two craters.  The presence of a significant magnetic anomaly nearby is unquestionable.

Froelich (l) and Lovelace (r), adjacent to Catena Sylvester (above map) and the region antipodal to Schrödinger basin - showing grooved terrain in walls (green arrows).
From Hood, et al (2013). Along with its spectacular lunar swirls and complex crustal magnetism, grooved terrain along the walls surrounding Mare Ingenii is also a easily identified characteristic of the region adjacent to the antipodes of Mare Imbrium. Less well-known, perhaps, is the region antipodal to Mare Serenitatis, along the north rim of the more ancient South Pole-Aitken basin [NASA/GSFC/ASU].
So have I changed my mind on the origin of lunar magnetic anomalies?  Possibly.  One of the most convincing ways to get a scientist to change his mind is to bludgeon him with an irrefutable fact that contradicts his worldview.  I now realize the Reiner Gamma problem does not “disprove” the basin antipode model – it merely indicates that it may be incomplete.  That distinction is subtle but significant.  In science, we always look for “rules,” generalities that help us organize observations and suggest possible explanations.  However, these rules sometimes have exceptions and we must carefully distinguish which actually have the force of a rule versus those that merely indicate some general tendencies.

To me, this discovery was surprising.  The new finding still does not fully address exactly how these magnetic anomalies are formed at the antipodes, but the concept that magnetic anomalies and basin-forming impacts are intimately associated has been strengthened and extended.  We will continue to work on this vexing problem.

Originally published June 19, 2013 at his Smithsonian Air & Space blog The Once and Future Moon, Dr. Spudis is a senior staff scientist at the Lunar and Planetary Institute. The opinions expressed are those of the author but are better informed than average.

Related Posts:
Bubble, Bubble – Swirl and Trouble (July 19, 2012)
Boulder 668 at Descartes C (July 16, 2012)
LROC: The Swirls of Mare Ingenii (June 22, 2012)
Remnant magnetism hints at once-active lunar core (January 27, 2012)
Grand lunar swirls yielding to LRO Mini-RF (October 4, 2010)
Another look at Reiner Gamma (June 30, 2010)
LOLA: Goddard (June 26, 2010)
Depths of Mare Ingenii (June 16, 2010)
LROC: Ingenii Swirls at Constellation Region of Interest (May 26, 2010)
Local topography and Reiner Gamma (May 22, 2010)
Lunar swirl phenomena from LRO (May 17, 2010)
The still-mysterious Descartes formation (May 11, 2010)
Dust transport and its importance in the origin of lunar swirls (February 21, 2010)
The Heart of Reiner Gamma (November 17, 2009)
Moon’s mini-magnetospheres are old news (November 16, 2009)
MIT claim of solving ‘lunar mystery’ unfounded (January 15, 2009)

Thursday, July 19, 2012

Bubble Bubble - Swirl and Trouble

Swirls in Mare Ingenii, far side of the Moon (LROC: The Swirls of Mare Ingenii, Brett Denevi, June 22, 2012.)  [NASA/GSFC/Arizona State University].
Paul D. Spudis
The Once and Future Moon
Smithsonian Air & Space

  
The Moon, unlike Earth, has no global magnetic field but many surface locales of limited extent (tens of kilometers across) are magnetized.  In many instances, these small areas of high magnetic intensity are associated with unusual patterns of surface brightness (albedo, or degree of reflectance) that occur in curved, blotchy or other strange “swirl-like” shapes.  First observed by telescope, lunar scientists have been puzzled by the possible origin of what they imaginatively named “swirls.”

An example of a lunar swirl is a feature named Reiner γ (pronounced “Reiner gamma”), a bright splotch in southern Oceanus Procellarum, the dark mare region of the western near side.  The name indicates that initially this feature was thought to be an isolated peak of highland material that juts up through the mare (lowercase Greek letters were assigned to such prominences in the old nomenclature.)  However, even at very low sun elevations, close examination shows that this bright patch does not cast a shadow.  It is simply a bright patch on the surface, one with diffuse and nebulous edges, yet clearly more reflective than the surrounding dark mare material.  It does not appear to be associated with any crater or other surface feature.  It’s as though someone smudged a finished painting of the lunar surface.

During later Apollo missions, orbiting vehicles released “sub-satellites” (small spacecraft that continued to orbit the Moon long after the crews had left for home) carrying instruments to measure the Moon’s magnetic field.  Interestingly, they found a very strong magnetic field enhancement around the Reiner γ feature.  Moreover, numerous other swirls were found elsewhere on the Moon, especially on the floor of the huge South Pole-Aitken (SPA) basin in Mare Ingenii on the far side, and on the eastern limb of the Moon near Mare Marginis.  Each newly seen swirl was found to be associated with a magnetic anomaly.  However, the converse statement is not true – not all magnetic anomalies have associated swirls.

Two principal models emerged to explain these relations.  One model held that the swirls and the magnetism were contemporaneous – the swirls were surficial deposits caused by the scouring of the surface during the impact of a comet.  In this model, the cometary coma (i.e., the dense gaseous “atmosphere” surrounding the icy nucleus) struck the Moon at high velocity, scouring the surface and increasing its brightness while at the same time embedding the soil with a strong magnetic field caused by the creation of an impact-generated plasma (high temperature, low density matter).

The other model suggested that the magnetic anomalies pre-dated and were the cause of the swirls.  The lunar surface darkens and becomes redder with time owing to exposure to the solar wind (the stream of energetic particles – mostly protons – from the Sun).  Strong, localized magnetic fields serve as protective “bubbles” that caused the incident solar wind to flow around these tiny areas, darkening the edges of the field bubbles with enhanced flow but preserving the inner zones (which were shielded from the solar wind) as bright patches.  Thus, the bright parts of the swirls are areas that have not undergone “weathering” by the solar wind while the dark parts are zones that have experienced excessive space weathering.

Magnetic bubble created in the laboratory [RAL/Univ. York].
It remained uncertain whether this postulated “magnetic bubble” effect would actually work but recent experiments suggest that these bubbles might well operate on the Moon.  Scientists from the UK’s Rutherford Appleton Laboratory, creating a “solar wind tunnel” to observe the interactions of streaming plasma and confined magnetic bubbles, successfully produced a magnetic bubble under simulated space conditions.  They have compared the flow field around the laboratory magnetic bubble with the observations from orbiting spacecraft of lunar surface magnetism and find that the solar wind would be diverted around these magnetic anomalies on the Moon.  If solar wind darkening is the primary process that darkens the surface, we may have an explanation for the creation of the bright swirls.

70 kilometer-wide field of view LROC Wide Angle Camera (WAC) mosaic swept up from two orbital passes in May 2010. (The yellow box show a roughly 2.5 km-wide LROC Narrow Angle Camera (NAC) field of view in the image below. Something is allowing the radiation-linked maturation of lunar regolith in the dark lanes of Reiner Gamma while continuing to keep dust at the surface of its bright albedo lanes fresh and optically immature. Though the local magnetic field is probably strong enough to refract solar radiation, it's not sufficient for repelling more energetic (and admittedly less frequent) cosmic rays. The latter should have sufficient time to redden (darken) or "mature" the bright regions over about 900 million years [NASA/GSFC/Arizona State University].

The astute reader will note that while this bubble model might account for the origin of the swirls, it begs the question about what caused the magnetic field anomalies in the first place.  That remains a mystery.  It was noted many years ago by my colleague Lon Hood of the University of Arizona that many of the magnetic anomalies on the Moon are at the antipodes (i.e., 180° away from the center) of some of the youngest, large impact basins on the Moon.  The largest concentration of both surface magnetic anomalies and swirls are on the floor of the large SPA basin, near Mare Ingenii on the lunar far side.  This area is directly antipodal to the large, young Imbrium basin on the near side.  Likewise, the Mare Marginis swirls and magnetic fields are antipodal to the Orientale basin on the western limb (the last of the large lunar multi-ring impact basins).  Furthermore, as basins tend to cover the entire Moon, one can find a basin near the antipodes of almost any given feature (note well: the swirl that started all this hubbub, Reiner γ, isn’t antipodal to anything in particular).  But an even more significant issue is that while the basin antipodal association of many swirls is intriguing, it does not explain why we should see a zone of enhanced magnetization at such locations.  Igneous intrusion, concentration of impact-generated plasmas and converging ballistic ejecta have all been proposed but no specific mechanism seems to emerge as the magnetic field creating event.

We are left with a continuing and highly unsatisfactory situation – a possible explanation for the development of surface swirls on the Moon and of their association with magnetic field bubbles, but we still don’t understand the origins of these fields, the cause of their shapes and intensities and how they fit into the continually vexing problem of lunar magnetism in general.  Two steps forward and one step back.   Lunar science marches on.

Originally published at his Smithsonian Air & Space blog The Once and Future Moon, Dr. Spudis is a senior staff scientist at the Lunar and Planetary Institute. The opinions expressed are those of the author and are better informed than average

Tuesday, July 17, 2012

"Boulder 668" at Descartes C

Fig. 1. A mere dimple in Apollo-era orbital surveys, this cracked, relatively large (around 53 meters on its long axis) boulder is nested on the north rim of Descartes C crater, lording over steep walls and an interesting strategraphy of the crater's frozen "over spray" of impact melt. It was tossed up from a depth and now sits high over the 4.3 km-wide, 900 meter deep hole from wince it came. LROC Narrow Angle Camera (NAC) observation M175172374R, LRO orbit 10,949, November 4, 2011; angle of incidence 42.42° from the east-northeast, at 40 centimeters resolution and from an altitude of only 23.9 kilometers [NASA/GSFC/Arizona State University].
Fig. 2. Earth's Moon, Waxing Full, April 1, 2012.
The area in yellow is shown at full resolution below,
in Fig. 3; and the full mosaic, by Yuri Goryachko,
Mikhail Abgarian & Konstantin Morozov of Belarus
can be viewed HERE. [Astronominsk].
Joel Raupe
Lunar Pioneer
 
A boulder that seems precariously balanced on the rim of 4.3 kilometer crater Descartes C (11.028°S, 16.273°E) was photographed by the Lunar Reconnaissance Orbiter Camera (LROC) Narrow Angle Camera (NAC), last year, as LRO happened to be maneuvering through a cycle of exceptionally low orbital passes. It was a fortunate happenstance for Larry F. Scott and myself, because we once suggested a spot only a few meters away for a notional unmanned landing target. Though our area of interest in 2008, the Descartes Formation, so far, appears only sporadically in the released LROC NAC catalog, the team at Arizona State, headed by Mark Robinson, could not have picked a better target for us when LRO was "skimming the Moon," last year.

In 2011, after maintaining the LRO primarily in a low,  near-circular polar orbit, between 35 and 65 km high, for nearly three years flight directors began a change-over to their preferred method for extending the record-breaking mission into 2015, to raise LRO's orbit above 100 kilometers, which they accomplished very early in January.

Their plan reduces, but does not eliminate, the demands on LRO's limited supply of propellant needed to maintain a minimally useful near-circular polar orbit. (See, "Skimming the Moon," September 6 2011.)

The Moon is anisotropic, or "lumpy," as Dr. Robinson reminded us, and its notorious mascons and mass-voids put an uneven drag on LRO's baseline altitude, and this requires well-planned periodic maneuvers to prevent the vehicle from crashing after only seventy days or so. But before raising LRO's orbit, twice in 2011 the spacecraft was maneuvered through brief periods when the low point in its orbit brought the spacecraft down to within 25 kilometers from the surface, and this allowed for some really spectacular and detailed surveys, including even more extraordinarily detailed examinations of the Apollo landing sites.

These close passes also presented opportunities to gather other NAC observations to within 40 cm per pixel, and among the smaller NAC footprints delivered up in March was a nearly complete cross section of Descartes C, a typical small crater situated in a familiar, though unusual, location in the Southern Highlands.
Fig. 3. At full resolution, a 550 km field of view marked off with by a yellow rectangle in Fig. 1, up above, directly centered on the bright Descartes albedo 'swirl;' viewed through a better-than-average telescope. Slightly above and to the left (northwest) of the swirl both North and South Ray craters can be seen, making the Apollo 16 landing site one of the easiest to "pick out" with the mind's eye, even with a telescope back on Earth. Again, the really breathtaking full mosaic by Yuri Goryachko, Mikhail Abgarian & Konstantin Morozov of Belarus, can be viewed HERE. [Astronominsk].
Descartes C marks one indefinite extent of the Descartes formation, a small field of furrows and segmented hills stretching to the crater's northwest, topped with a distinct and bright, but small and amorphous "swirl" resembling a fresh snowfall. This 400 sq. km. patch of optically immature surface, nested inside a remarkably intense local magnetic field, rates higher than average scientific interest.

Our 2008 proposal included a teleoperated robotic ground survey beginning at Descartes C, lengthwise, through the heart of the unusual terrain and swirl, and its lunar magnetic anomaly, perhaps eventually emerging near the landing site of Apollo 16. Today we have an additional stop on that 'fantasy tour' a short distance from our originally proposed landing site. 

Fig. 4. LROC QuickMap (250 meter resolution) view, also centered on the 'anomalous' albedo and the Descartes Formation, seen here mixed with the false color of the LROC Wide Angle Camera (WAC)-derived topography. Again, a yellow rectangle marks off the field of view visible in Fig. 7, below. Note the "centipede" chain of half-kilometer long hills, training to the northeast from Descartes C. That feature is the most obvious distinction setting the formation apart from nearly every other spot on the Moon's surface. The age and wear of Descartes crater becomes more obvious as one closes in on the area [NASA/GSFC/DLR/Arizona State University].
Fig. 5. Simulated slightly oblique view over Descartes (29 km), from the Cayley Formation plains explored by Apollo 16 in the northwest, 80-plus kms southeast over the Descartes Formation and its swirl albedo to the highly-eroded main Descartes crater in the south. LROC WAC mosaic, from observations collected in three sequential orbital passes December 3, 2011, averaging 52 meters resolution, from 38 km, 70° angle of incidence [NASA/GSFC/Arizona State University].
Fig. 6. "Figure 2" from "Correlation of a strong lunar magnetic
anomaly with a high-albedo region of the Descartes mountains
,"
by Richmond, Hood & Halekas, et al. (GFL, V. 30, # 7, 2003)
"Contour map of the two-dimensionally filtered magnetic field
magnitude (in nano-Teslas, or nT) at an altitude of 18.6 km in the
vicinity of the Apollo 16 landing site (boxed cross). The photo-
graph is a portion of Apollo 16 mapping camera frame 0161
(AS16-M-0161). Several exposures of the Cayley formation (CF)
and the adjacent Descartes mountains (DM) are indicated"
[Lunar Prospector Magnetometer data, 1999].
Our paper broadly outlined a very notional multipurpose robotic lander-rover mission in support of the proposed International Lunar Network (ILN). We advocated discovery of ground truth about one lunar magnetic anomaly in particular, and its well-known relationship with a bright surface swirl marking. Also, we wanted to add our small voices to the chorus recommending a cautious approach to the scientifically valuable (and remarkably fragile) artifacts of Apollo, "from the ground, and from a distance." Of course, since then, a growing chorus has out-grown much need for small voices. The NASA Human Exploration and Operations Directorate's recommendation "to space-faring entities," released in July 2011 explicitly spells out the agency's similar concern.

Interest in lunar swirl "patterns" appears as strong as ever, and may be growing. It's become difficult to remember that little more than a decade ago the anomalous albedo 'swirls' today associated with features near Descartes and nearby Airy craters (both easily visible from Earth) were still little recognized.

Because the more famous, more aesthetically pleasing swirl fields at Reiner Gamma, Mare Ingenii and Mare Marginis have been properly associated with local crustal magnetism the recognition of anomalous optically immature regolith elsewhere on the Moon was "reverse engineered."

In the case of smaller 'smudges' near both Airy and Descartes craters, for example, acknowledgement as true swirls has depended on the fleeting detection of magnetic fields at both locations late in the Lunar Prospector mission, not long prior to its eventual crash landing in Shoemaker crater, near the Moon's south pole, in 1999.

For many years after the demise of that small spacecraft researchers continued to tease more and more data from a telemetry stream that today seems remarkably sparse when compared with oceans of data continuously relayed back from LRO. Magnetometer readings from only two low altitude fly-over encounters by Lunar Prospector with the Descartes Formation delivered sufficient evidence to demonstrate a tightly wound mini-magnetosphere existed over the bright albedo swirl, upon on the unusual hills between Descartes crater and the landing site of Apollo 16. The relatively small magnetic anomaly may be the most intense crustal magnetism on the Moon (See Fig. 6).

Fig. 7. The swirl painted on the unique contours of the Descartes formation, just beyond the eroded northern rim of the main crater, is not as striking a in photographs taken from orbit, such as the picture taken from Apollo 14 and 16, or the LROC Wide Angle Camera images from close orbit. The estimated strength of the very localized magnetic field, as measured from Lunar Prospector from an altitude of 18.3 km in 1999, is indicated in nano-Teslas (nT).  LROC WAC observation M177535094C (604nm), LRO orbit 11299, December 3, 2011; angle of incidence 69.57° at 52.3 meters resolution from 38.27 km [NASA/GSFC/Arizona State University].
It's difficult to recall any controversy over the origin (and natural sustaining) of optically immature regolith, at Reiner Gamma, for example. Nevertheless, some very respectable researchers still insist the swirl albedo patterns are the result of scant, recent encounters with comets. The most detailed crater counting methods have all but ruled out any swarming impact origin to the Reiner Gamma swirl. The magnetic field strengths associated with many of these fields are, in some cases (e.g., Descartes and Gerasimovich), sufficiently intense to refract solar wind, but these fields are too small in scale to refract their less frequent but cumulative encounters with the most energetic and heaviest cosmic radiation.

Remote sensing of the Descartes swirl indicates the presence, in abundance, of nanophase iron in the surface grains, thought to be at least one of the ingredients of optical maturity, and a strong indicator of the transparency of the local magnetic field to iron nucleons, a big part of the cosmic ray mix. (Unless, of course, lunar micro-grains implanted with nanophase iron arrived at the site by another mechanism.)

Swirl fields and their associated magnetic fields along the north rim of 4 billion year-old South Pole-Aitken basin are each individually, very closely associated with the antipodes of the most easily-recognized nearside impact basins. The lovely swirls of Mare Ingenii, for example, are nearly on the direct opposite side of the Moon from Mare Imbrium, and the jumble of swirls in and around Goddard crater and Mare Marginis are similarly on the opposite side of the Moon from Mare Orientale.

Because these basins are still believed to be between 3.85 and 3.1 billion years old, respectively, the ages of the magnetic fields clustered at their antipodal foci are thought to be at least as old as those impacts. (But, it should be noted here that no basin-forming impact has yet been associated with the antipodes of smaller nearside swirl patches near Airy or Descartes craters, nor, for that matter, with the unique and much more widespread Reiner Gamma swirl within Oceanus Procellarum.)

The persistent mystery of lunar swirl patterns is still the longevity of "optical immaturity," brightness at the lunar surface that constitutes the swirls themselves. As soon as these "patterns" were associated with local crustal magnetism it was quickly suggested that some refraction, even reversal, of the relentless solar wind kept the surface under their influence from being "darkened." Experiments with high-energy radiation bombardment under laboratory conditions, the energetic variety of cosmic rays that can't be steered away by these fields, appears to indicate that, eventually, any lunar regolith will mature, after only 900 million years or so. As the upper few centimeters of the lunar surface is eventually pulverized into abrasive powder, the process of maturation by hard radiation gets underway.

So how is the optically immature regolith of these swirls kept fresh?

It was our suggestion in 2008 that the answer rests in the very slow migration of lunar dust. The supply of fresh, optically immature dust is continuously supplied by the gardening of impacts, both large and very, very small. And then, at the beginning and end of a daily cycle of charging and discharging of these smallest grains, these nested magnetic fields (which are likely to have more than one kind of origin) preferentially lose and accumulate both mature and immature dust, dividing up both the levitation and fallout along opposing polarities, in a very slow process that still manages to out pace the relentless process of "reddening" or "darkening" by hard radiation, admittedly a less frequent kind of radiation than the bulk of solar wind, but just as relentless.

Which brings us to "Boulder 668," on the north rim of Descartes C, a crater that is itself nested on the north rim of a far more ancient crater, Descartes. The number "668," by the way, marks the boulder's elevation, according to a rough reading of the LROC QuickMap website and its WAC-derived digital elevation model. Obviously there's nothing official about the name.

The boulder reminds us of "House Rock," as well, its smaller cousin ejected out from the North Ray crater impact, and at one time closely examined and sampled directly by John Young and Charles Duke in 1972 (and only about 80 km away from Boulder 668 and Descartes C).

Charlie Duke samples a shatter cone formation in Outhouse Rock, a large fragment shed off the southern end of House Rock, at North Ray crater during the third and final EVA of Apollo 16.  AS16-116-18649 [John Young/NASA/JSC/ALSJ].
The choice for the Apollo 16 landing site, the only manned visit to the lunar highlands, and a landing site referred to as "Descartes," was made in the sincere belief that the apparently unique topography of the Descartes Formation strongly indicated the area to be volcanic in origin. Mission planners were disappointed to discover, almost immediately after Apollo 16 landed, however, no obvious sign of volcanism.

On their second EVA, Young and Duke drove up the slopes of "Stone Mountain," the northwest extreme of the Formation, and looked high and low for a sample uncontaminated by ejecta from nearby South Ray crater.

On their departure from the Moon Captain Young remarked about "still mysterious Descartes," unaware then of the tantalizing evidence they had almost inadvertently uncovered. Their haul of samples proved every bit as valuable as any from the Apollo missions to the overall body of lunar research in the decades following Apollo.

Almost as a footnote, their magnetometer readings proved to be the strongest ever detected on the lunar surface.

In the years since Apollo it's become generally accepted that the unique topography of the Descartes Formation, completely apart from its swirl albedo and magnetic personality, "probably" originated with the impact that formed Mare Imbrium, whose influence is so clearly etched into the landscape of the region, so obviously radiant from the center of that basin. Others say the Nectaris impact, before Imbrium and closer by, tossed up what may turn out to have been a very large, semi-coagulated chuck of impact melt that quickly fell back to the Moon more or less intact, immediately settling in and around existing crater remnants.

Also generally recognized as perhaps the oldest, remarkably intact feature of area is old Descartes itself, an apparently very worn and "tortured" crater differs in many ways from worn craters of apparently the same age elsewhere on the Moon. As worn as it is, it's concentric rings have, for the most part, not been erased (again, remarkably) appear more like a sand castle after the first wave of an incoming tide, without the notched rims characteristic of many largely intact older craters. Descartes seems over washed, with an infill of material around it which consists of more than just the convoluted terrain of the Descartes Formation plateau to its north.

In any case, Descartes, by all appearances, hollowed out a place in the ancient Southern Highlands, perhaps prior the supposed late heavy bombardment.

Though Descartes is now mostly "back-filled," today, more likely from a steady bombardment that erased many of its nearby contemporaries, the impact that formed the old crater tossed up its deepest excavated material and deposited this around its smoothed rim. Some time after this, apparently not from volcanic vent, the half-kilometer-scale chains of hills and furrows of the Descartes Formation arrived on the crater's north exterior, forming or deforming a plateau. Under that material, or, more likely, within the material itself is a very intense, very local crustal magnetic field. That field has since interacted with the slow process of lunar dust charging, discharging, preferential accumulation and levitation, dust migration and the forces driving optical maturity, to form the bright swirl within the magnetism's exceptionally strong influence.

Eons pass, and along came the progenitor that excavated Descartes C crater at the crossroads of all this ancient history. In its formation there was tossed up along its rim the long-buried material once tossed up from an even greater depth by Descartes. "Boulder 668" may represent a bulk of older material less shock metamorphosed than the melt splashed over its rim and pooled on its small floor. The boulder poses questions more, perhaps, than it answers.

In 2008 we fancifully suggested approaching the artifacts of Apollo 16 from the ground, and from a distance of 80 kilometers, all starting with a landing less than 100 meters from the north edge of Descartes C and "Boulder 668." Showing great faith in the future of robust teleoperated robotics we suggested being driven to reconnoiter the Descartes Formation to closely examine "still mysterious Descartes," its magnetic field and albedo. Now, thanks to this remarkably close examination of our proposed landing site we have our fantasy rover's first stop picked out for us for us to examine, and a reason to linger around the perimeter of Descartes and Descartes C a little longer than originally planned.

Fig. 8. Descartes C (4.32 kilometers, centered near 11.028°S, 16.273°E), nested on the deeply eroded rim of Descartes proper, has gradually been seen in increasing detail following multiple LROC Narrow Angle Camera (NAC) observations over LRO's three years in lunar orbit. No longer just a bright crater in a bright region, having excavated an unusually complex area, Descartes C is itself richly complex, with impact melt on steep walls and debris flows into a small kilometer-wide melt-flooded floor. The boulder at 668 meters elevation, high on its rim, was excavated from below the melt pond 750 meters below [NASA/GSFC/Arizona State University]

Friday, June 22, 2012

LROC: The Swirls of Mare Ingenii

An oblique view of Mare Ingenii and the swirl that marks its floor. Scene is approximately 15 km across (subsampled from the native resolution); LROC Narrow Angle Camera (NAC) frames M191830503L & R, LRO orbit 13304, May 16, 2012; resolution 2.95 meters per pixel. See the full size LROC Featured Image HERE [NASA/GSFC/Arizona State University].

Brett Denevi
Lunar swirls are among the most beautiful and bizarre features on the Moon. Seen as bright, sinuous regions, swirls are associated with weak magnetic anomalies in the Moon's crust. Images from LROC, and the topographic information extracted from those images, have shown that swirls have no topography associated with them; they are not higher or lower than their surroundings. Instead, it is as if someone has taken a brush and laid down a beautiful swath of bright paint. In the top image is the classic omega-shaped swirl of Mare Ingenii, also seen in this past featured image. The region of higher terrain is the rim of Thompson crater.

The lavas that formed Mare Ingenii flooded Thompson, leaving only the rim as a kipuka of older highland terrain.

A wider (but very reduced-resolution) view of the Ingenii swirls. The rims of Thompson and Thompson M craters are seen in the foreground. View is from east to west, and the full scene is approximately 58 km across [NASA/GSFC/Arizona State University].
The obvious question: how did swirls, like the one shown here, form? The leading hypothesis involves two main components - solar wind and crustal magnetic anomalies. The solar wind is a stream of charged particles coming from the Sun that normally interact with the Moon's surface, darkening it as one portion of a process called space weathering. On the Earth, the magnetic field acts as a shield and usually deflects the solar wind (when it doesn't, the solar wind interacts with the atmosphere, causing the northern lights). The Moon lacks a global magnetic field, but does have small, local magnetized regions within the crust. This is where we see the swirls. So the idea is that these local magnetic fields prevent the solar wind from doing its normal job of space weathering, and the surface stays bright. The stunning swirly pattern of the bright regions is likely due to the complex pattern of the magnetic field lines, which shield some areas and not others.

LROC Wide Angle Camera (WAC) views of Mare Ingenii, for context. The box in the second image outlines the approximate footprint of the LROC Featured Image released June 21, 2012. The bottom animated gif image, generated from separate views of the 282 km wide Mare Ingenii and the 1400 square km surrounding region from the LROC QuickMap. Resolution was set at 500 meters, WAC mosaic draped over the WAC derived elevation model Researchers long suspected true lunar albedo swirls are not related to any topographic feature, including very small secondary craters. The latest high resolution images and crater count studies continue to back that conclusion.  [NASA/GSFC/Arizona State University].
The LROC team is continuing to study the lunar swirls, including their color properties as observed in LROC Wide Angle Camera data, to learn more about how swirls form, the process of space weathering, the rate at which bright, freshly exposed material is darkened by space weathering, and why crustal magnetic fields are where they are.

See the spectacular full-resolution oblique look at the Ingenii swirls HERE.

Read about the Reiner Gamma swirl, HERE.

Mare Ingenii was imaged using the HDTV camera on-board Japan's lunar orbiter Kaguya (SELENE-1) in 2008 [JAXA/NHK/SELENE].
Mare Ingenii Related Posts:
The new Kaguya Terrain Camera tours (May 5, 2012)
A Potpourri of Lunar Results (March 14, 2012)
NASA@Science: “Down the lunar rabbit hole (July 13, 2010)
Grand lunar swirls yielding to LRO Mini-RF (October 4, 2010)
Depths of Mare Ingenii (June 16, 2010)
LROC: Ingenni Swirls at Constellation ROI (May 26, 2010)
More cavern entrances discovered on the Moon (February 26, 2010)
Moon’s mini-magnetospheres are old news (November 16, 2009)