Showing posts with label lunar crater. Show all posts
Showing posts with label lunar crater. Show all posts

Wednesday, May 29, 2013

Alien materials found in lunar crater! (Film at Eleven)

Central peaks of Copernicus - covered by fairy dust? -- From oblique LROC Narrow Angle Camera (NAC) mosaic M193025138LR, LRO orbit 13472, May 30, 2012; field of view is a 1350 pixel section from a spectacular LROC mosaic revealing the 90 km-wide interior of the landmark lunar crater, HERE [NASA/GSFC/Arizona State University].
Paul D. Spudis
The Once and Future Moon
Smithsonian Air & Space


Accuracy in scientific reporting (and thus the education of the public) is wholly dependent on a reporter’s understanding of the material they’re covering.  Making a reporter’s job even more challenging is the fact that some research results themselves can be misleading.  
A variant of my post title above appeared recently over a story reporting the results of a paper published in the journal Nature Geoscience.  That study used computer modeling to simulate the effects of a low velocity impact on the Moon.  Computer models of natural phenomena are made in an attempt to understand complex processes that we could otherwise not be able to address.

To briefly set the stage on this new work, we believe that the vast majority of craters on the Moon and planets are formed by the collision of solid objects with these bodies.  These impacts occur at very high speeds; on the Moon, the average velocity of impact is about 20,000 meters per second.  At such speeds, geological materials will vaporize and the mechanics of the formation of a crater are complex.  These results have been painstakingly described through laboratory and field studies of both natural and artificial impact craters of a wide range of sizes.

Because we needed to fully understand the mechanics of impact cratering to understand the record in the Apollo lunar samples, much work was conducted toward characterizing the physical and chemical effects of impact on typical rocks.  Because impact velocities are typically high, there is little preservation of the projectile in impact craters.  Most of the impactor is vaporized and this super-hot silicate vapor is partly lost to space and partly incorporated into the shock melted rocks of the crater interior.
"For every problem there is a solution that is simple, elegant and wrong." - Mencken

The soils returned from the Apollo missions contained a recognizable fraction of material that must have been added by the impacting objects that created its craters.  In most soils, this fraction is on the order of a few weight percent.  Interestingly, this “meteoritic component” tends to be defined chemically and actual fragments of meteorite in the lunar soil are extremely rare.  This observation would seem to support the notion that most of the impacting debris is vaporized at impact and does not occur as fragments on the surface.

However, the speed of impacting projectiles cited above is an average speed, meaning that while some impacts occur at higher velocities, others must occur at lower speeds.  As the encounter velocity decreases, there is an increasing likelihood that some portions of the impacting fragments might be preserved on the surface.  It is this last possibility that the new paper considers.  The authors modeled the effects of the impact of a relatively slow-moving body with the Moon and found that more fragments of the object are preserved than in high velocity impacts.  Moreover, by tracing the paths of impactor particles during cratering flow, they find that much of this preserved material ends up on or near the central peak of the resulting crater.

That last finding is interesting because in remote sensing studies of the lunar surface, it is in the central peaks where we find “unusual” compositions, in the sense that those compositions are different from the average upper lunar surface.  The traditional explanation for this relation is that because central peaks are derived from well below the impact target, they are exposing deep-seated compositions (lower levels of the crust of the Moon contain different rock types than occur on the surface).  The study’s new interpretation suggests instead that the central peaks are covered in debris from the impacting projectile.

One problem with this interpretation is that the “debris covering” of central peaks should occur in a distinct minority of craters (i.e., those created by low velocity impacts).  But the exposure of unusual compositions within central peaks of lunar craters is quite common and occurs globally.  Moreover, there are as many impacts at higher velocity as at lower velocity.  Yet slow impacts would produce less total volume of impact melt and most of the central peak craters on the Moon have abundant melt deposits.

M1098059280LR-NSJ-58ax-33p-2450x3380
Central peaks of the farside landmark crater Tsiolkovskiy, from over 200 km to the west of the highest promontory. The large, mare-inundated impact crater was very unlikely to have been formed by a "low-velocity" collision.  A highly reduced in scale crop from a LROC NAC mosaic, M1098059280, orbit 14176, July 27, 2012; resolution between 4.6 and 5.3 (background) meters, from 87.66 km over 20.44°S, 121.42°E. Enlargement, HERE [NASA/GSFC/Arizona State University].

The most serious flaw in the new study is the assumption that the “unusual minerals,” olivine and spinel (found in many central peaks), are rare on the Moon. They are not rare; although spinel is somewhat sparse on the lunar surface (requiring high pressure for its formation), it has been described as present in lunar rocks from the first sample return and more recently has been found in remote sensing data of impact basin deposits. 

Olivine is a very abundant mineral on the Moon and typically makes up a significant fraction of the dark mare basalts (including some lavas that consist only of olivine and glass.)  Olivine is also not uncommon in highland rocks, usually occurring within the rock type troctolite, a 50-50 mixture of olivine and plagioclase.  The presence of olivine does not indicate either “deep” origins or “lunar mantle” provenance; virtually all olivine in lunar samples has high calcium content, indicating a relatively shallow origin (probably in magmas that crystallized within a few kilometers of the surface). 

In short, there is no compelling reason to believe that the central peaks of many lunar craters are dusted with exotic minerals from asteroids, although such a possibility is certainly not excluded.  The minerals that we see in central peaks are all indigenous to the Moon and in some cases, abundant in the lunar crust.

Computer modeling in science has both value and pitfalls.  An impact event is extremely messy and complicated.  Simultaneously, gigantic shock pressures and temperatures occur, putting billions of particles in motion.  Computers are good at keeping track of these particles and the codes developed to model complex, multi-variable phenomena have been shown to at least partly describe the behavior of crater formation on Earth.  However, the results of computer models must be interpreted cautiously; small changes in input variables or the conditions of the simulation sometimes result in drastic changes in the output of the model.  In addition, there is a tendency in science to believe in numbers, regardless of their provenance.  Because a model holds together does not mean that it describes reality.

In science, it is dangerous to embrace a model because it “works” (i.e., comes to closure).  Much of the current fracas over human-induced climate change comes from those who contend that the results of computer models constitute “settled science” (whatever that is).  Because the computer models say that it may happen, people assume (and some journalists report) that it is happening.  In actual fact, we have no direct observational evidence that human-caused emissions of carbon dioxide are causing the climate to change.  That conclusion comes from computer models that “show” (project) that humanity’s introduction of “excess” carbon dioxide into the atmosphere by industrialization will increase the magnitude of the greenhouse effect and raise the mean global temperature.  But climate (like impact) is a complex, chaotic phenomenon and we still do not fully understand how the Earth’s atmosphere interacts with itself and the cosmos.

In questions of complex natural processes, beware of accepting the results of computer modeling too easily.  Computer models are useful tools, but the old software adage of “garbage in, garbage out” still applies.  Be familiar with whom and from where the information comes, understand how it is processed and then carefully consider the likelihood of reported accounts.

Originally published May 29, 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.

Thursday, May 23, 2013

Layers of Imbrium excavated by Caroline Herschel Crater

Exposed mare basalt layering in the wall of Caroline Herschel crater (34.48°N, 328.71°E). LROC Narrow Angle Camera (NAC) observation M175475137R, spacecraft orbit 10994, November 9, 2011; field of view 350 meters at 45 cm per pixel resolution; angle of incidence 55.93° from 30.15 km [NASA/GSFC/Arizona State University].
Sarah Braden
LROC News System

Outcrops of layered mare basalt are visible in the interior wall of Caroline Herschel crater (located at 34.48°N, 328.71°E, in western Mare Imbrium).

The mare basalt layers were exposed during the excavation phase of the impact which created this 13.7 km diameter crater. Some debris from the crater rim and the wall have fallen over the layers but the structure of the outcrop is still preserved.

The crater is superposed on a north-south trending wrinkle ridge which is visible in the LROC WAC context image below. This crater is named after Caroline Herschel, an astronomer and half of the sister/brother science team with astronomer Sir William Herschel.

Wider angle view of the northwestern rim, wall and interior of C. Herschel. LROC NAC M1106123678L, orbit 15305, October 29,  2012; resolution 1.5 meters per pixel, angle of incidence 53.18° from 150.4 km [NASA/GSFC/Arizona State University].
Caroline discovered several comets, and in 1828 the Royal Astronomical Society awarded her their Gold Medal for her work. She made observations, kept detailed records, performed complex mathematical calculations, and polished her own telescope mirrors. Caroline has multiple comets named after her as well as the lovely lunar crater in today's Featured Image.

LROC Wide Angle Camera (WAC) context for Caroline Hershel. The white asterisk marks the area of basalt layering in the Featured Image. Field of view is 48 kilometers [NASA/GSFC/Arizona State University].
Explore the entire NAC frame to see the beauty of the Moon, HERE.

Related Images:
Galilaei's Layered Wall
Pytheas
Dawes
Lava Flows Exposed in Bessel Crater

Wednesday, November 30, 2011

LROC: Layered basalt on the wall of Marius A

Layered basalt on the wall of Marius A crater partially covered by debris flow. The crater rim is to the right and the crater floor is to the left. LROC Narrow Angle Camera (NAC) observation M137848463R, LRO orbit 5448, August 30, 2010; field of view of the original LROC Featured Image (HERE) 460 meters, at an illumination incidence angle of 33° from an altitude of 44.37 kilometers [NASA/GSFC/Arizona State University].
Sarah Braden
LROC News System

Marius A (12.58°N, 46.05°W) is an approximately 15 kilometer crater located in Mare Insularum. The Featured Image shows basalt layering partially covered by streaks of granular material that slid down from higher up on the wall. Craters with visible basalt layers like Marius A are windows to the history of basalt deposition. 

Each thin layer seen in the wall of Marius A is probably a single flow or flow lobe, each spreading out across the lunar surface due to the low viscosity of mare basalt (basalt has a viscosity similar to that of ketchup). How much time passed between each layer is still an unanswered question. By studying many craters with visible basalt flows, however, scientists may be able to piece together a more detailed, local history for the various mare on the lunar surface. Not all craters in the mare have visible mare basalt layering, though. Additionally, over time post-impact processes like the debris in today's Featured Image and slumping of the crater walls reduce the visibility of basalt layers.

Marius A at 62 meters resolution from LROC Wide Angle Camera (WAC) observation M135493956C, orbit 5101, August 3, 2010 in a field of view roughly 42 km across; incidence angle 57.09° from 44.1 km above. The much small field of view shown in detail in the Featured Image released November 29, 2011 is located at just shy of "3 o'clock" on the east crater rim wall [NASA/GSFC/Arizona State University].
LROC WAC context image of Marius A crater. The image is 59 km across and the rectangle indicates the area of the whole NAC frame from which the Featured Image is taken. View the full size and original LROC WAC context image HERE [NASA/GSFC/Arizona State University].

There are many craters with visible basalt layers and LROC has given us our first look at these incredible details of the lunar surface. Check out the NAC frame of Marius A and then explore the rest of the lunar maria!

Related Posts:
Layering in Euler Crater
Lava Flows Exposed in Bessel Crater
New Views of Lunar Pits

Marius A in a wider oblique context view from a virtual point 254 kilometers over the bright landmark crater Kepler, showing some of the more famous landmarks also nearby. One of the wispy rays of material and reflective secondary craters, superimposed upon Marius A by the Kepler impact event crosses directly upon Marius A and beyond, a distance of 280 kilometers from crater center to crater center [NASA/LMMP/GSFC/ARC/ASU].

Thursday, October 20, 2011

LROC: Lucian's Layers

Layers of material are exposed forming small cliffs just within the south rim of Lucian, perhaps exposing the volcanic strategraphy and geologic history of Mare Tranquillitatis. LROC Narrow Angle Camera (NAC) observation M170321251R, LRO orbit 10234, September 10, 2011; field of view above is 290 meters. View the full resolution field of view in the LROC Featured Image HERE [NASA/GSFC/Arizona State University].
Drew Enns
LROC News System

Lucian crater, located in Mare Tranquillitatis at 14.3°N, 36.7° E, is a small (~7 km in diameter), relatively fresh crater. Because Lucian is still young, rock is freshly exposed in its wall, and the rocks are layered! But how do these layers relate to Mare Tranquillitatis? Scientists think that the maria were formed as the product of large scale flood volcanism.

Billions of years ago large volumes of lava were erupted from fissures in the lunar crust to cover 17% of the Moon's surface. But this process occurred over a period of time with a very low viscosity lava. This model of mare formation predicts that the mare are made up of many distinct layers. Prior to LROC some scientists argued that the layers were thin, and some scientists argued that the layers were thick. LROC data shows Lucian and other craters have thin layers that are a few meters thick. LROC has again helped scientists understand more about the nature of the Moon!

Full width 2 km-wide view of the layering under the surface of the Sea of Tranquility exposed by the explosive impact that formed Lucian crater probably late in the Eratosthenian era (1.1 - 3.1 billion years ago). The flat floor of the crater formed from pooled impact melt is just out of view above, though it is visible in the full NAC frame HERE, and in the Wide Angle Camera (WAC) view immediately below [NASA/GSFC/Arizona State University].

The layering inside the south rim of Lucian, steep slopes and floor of Lucian are visible in a late afternoon local illuminate here in the context of, from north to south, a roughly 36 km long field of view centered on the crater in north central Tranquillitatis: LROC WAC observation (643 nm) M119612004, LRO orbit 2761, January 31, 2010; resolution 61.7 meters per pixel, phase angle 57.81° from 43.76 kilometers [NASA/GSFC/Arizona State University].
A 132 kilometer wide slice of north central Mare Tranquillitatis when the Sun was less than 10 degrees above the east horizon allows more subtle variations in elevation to stand out in long shadows, and with it the variety of ancient features on one the Moon's oldest lunar mare fills. From a monochrome (604 nm) mosaic of LROC WAC observations gathered in sequential orbital passes (orbits 2237 through 2241) December 21, 2009. Highly reduced crop from an original resolution of about 63 meters, at a 57.8° phase angle, from 43.1 kilometers [NASA/GSFC/Arizona State University].
A quick view from the new and improved LROC QuickMap centered on Lucian composed of a base LROC WAC mosaic of northeast Mare Tranquillitatis with the WAC digital terrain model (DTM) overlay (500 meter resolution) at its default opacity of 30 percent [NASA/GSFC/Arizona State University].

How many layers can you count in the full NAC frame?

Related Posts:
Layers near Apollo 15 landing site
Layering in Messier A
Sublunarean void!

Friday, September 30, 2011

LROC: Farside Impact!

A young, fresh impact into the farside highlands, south of Tsiolkovskiy crater. LROC Narrow Angle Camera (NAC) observation M159073200L, LRO orbit 8576, May 3, 2011; image field of view is roughly 325 meters wide. See the full size LROC Featured Image HERE [NASA/GSFC/Arizona State University].
Lillian Ostrach
LROC News System

Young impacts abound on the Moon, and the LROC NAC images of beautiful crater morphologies, spectacular ejecta blankets, and stunning impact melt deposits are enough to make any lunar geologist jump for joy. Many times, fresh impacts into mare material are featured because these craters punch through the thin layer of regolith and produce boulders. However, impacts into the lunar highlands can be just as spectacular.

Today's Featured Image of an unnamed Copernican-aged crater (~630 m diameter, 29.73°S, 134.07°E) is one such example on the farside. Close-up, the crater is bowl-shaped with a well-defined circular rim. At the crater floor center is a small, bouldery pond of solidified impact melt. Debris from the crater walls have slumped toward the floor center, but whether these slumps happened immediately after crater formation or yesterday is difficult to determine. 

The first in a brief series of reduced views of a relatively small fresh impact crater near the southwestern rim of the far more ancient 61 km-wide crater Subbotin, in the Farside lunar Highlands [NASA/GSFC/Arizona State University].
Take a look at some of the material nearest to the crater floor; in the crater center, some slumps are veneered with impact melt but other debris piles superpose (overlie) these veneered materials. These stratigraphic relationships can be used to interpret the relative ages of the slumps - the impact melt-covered piles formed soon after impact because they are splashed with impact melt, and the overlying debris piles happened after the impact melt solidified (maybe even yesterday!). Furthermore, the ejecta blanket closest to the crater rim is mostly uniform in reflectance but there are scatterings of boulders and lower-reflectance impact melt streamers that were thrown out of the crater during ejecta emplacement. 

What a beauty! 

A further reduced-resolution view from M159073200L, showing a 2.7 km field of view. See the full-size LROC context image HERE [NASA/GSFC/Arizona State University].
LROC WAC monochrome (566nm) mosaic of the Farside west of Subbotin crater swept up over the course of LRO orbits 4924 through 4926, July 20, 2010. The fresh impact crater in the opening image the small "bulls eye" just left of center in the image above. At this illumination incidence angle, ~72.7° from the west north west, the deeper central circular floor of the crater is already deeply shadowed in the coming sunset.  [NASA/GSFC/Arizona State University].
What other exciting geologic features do you observe when you explore the full LROC NAC image?

Related Posts:
Small crater at the southern rim of Menelaus
Smooth floor in Copernicus crater