Showing posts with label Copernicus. Show all posts
Showing posts with label Copernicus. Show all posts

Saturday, February 6, 2016

Edgar Mitchell (1930-2016)

Edgar Mitchell, sixth human to visit the lunar surface, takes a live panorama of the close horizon using the first color television camera successfully operated on the Moon; at Fra Mauro, south of Copernicus, February 1971. Photograph by Apollo 14 commander Alan Shepard [NASA/JSC].
Astronaut Edgar Mitchell, lunar module pilot on Apollo 14, passed away Thursday in West Palm Beach, Florida,  and on the eve of the 45th anniversary of his lunar expedition in 1971.

Mitchell joined Apollo 14 commander Alan Shephard, Jr., the first American in space, in the lunar module Antares, which touched down February 5, 1971, in the Fra Mauro highlands. Shepard and Mitchell were assigned to traverse the lunar surface to deploy scientific instruments and perform a communications test on the surface, as well as photograph the lunar surface and any deep space phenomena. It was Mitchell’s only spaceflight.

Mitchell and Shephard set mission records for the time of the longest distance traversed on the lunar surface; the largest payload returned from lunar surface; and the longest lunar stay time (33 hours). They were also the first to transmit color TV from the lunar surface. Mitchell helped collect 94 pounds of lunar rock and soil samples that were distributed across 187 scientific teams in the United States and 14 other countries for analysis.

Read the full NASA release HERE.

Tuesday, April 8, 2014

One in a Million Mounds

Boulders, most 10 to 20 meters across, pepper the flanks of a cratered mound on the northern bifurcated floor of Copernicus crater. LROC NAC observation M1139037292R, field of view roughly 1100 meters across, LRO orbit 19933, November 14, 2013; resolution 1.12 meters per pixel at 67° illumination incidence from 119.38 km [NASA/GSFC/Arizona State University].
J. Stopar
LROC News System

A domical mound protrudes from the floor of Copernicus crater (see 10.332°N, 340.117°E), which is dominated by a solidified sea of impact melt rocks. 

These rocks host a variety of positive- and negative-relief features including collapse features, central peaks, and blocky cratered mounds like the one above. 

Mounds with craters near their peaks can superficially resemble volcanoes, which often have a summit crater. Previously, several examples of cratered mounds, usually located along the mare-highlands boundaries, were suggested as possible newly discovered volcanoes (Volcanoes in Lacus Mortis, Bull's Eye Crater or Volcanic Vent, Another Small Volcano).

Cratered and Boulder dome on northern bifurcated floor of Copernicus (small arrow, above center). The demarcation between the character of the western and eastern floor, north of the landmark twin central peaks of Copernicus are particularly striking in spectral analysis. LROC WAC observation M147109260CE (643 nm), spacecraft orbit 6813, December 16, 2010; angle of incidence 77.97° at 60 meters per pixel resolution from 43.13 km [NASA/GSFC/Arizona State University].
This mound remains unexplored, thus we don't know for sure how it formed. Below is a collection of lunar mounds that are similar in appearance. For each example, try to think about how (or why not) these features might shed light on the formation of the cratered mound in Copernicus.

1. Volcanic Dome?

The summit crater of a volcano is expected to lack a raised rim and is usually less circular than an impact crater. Some small domes at the Compton-Belkovich silicic volcanic complex have craters that are thought to be summit vents (Example 1).

Example 1: A cratered and blocky dome at the Compton-Belkovich silicic volcanic complex, in the farside highlands. 510 meter-wide field of view from LROC NAC mosaic M119198897LR, LRO orbit 2700, January 27, 2010; resolution 60 cm per pixel, incidence angle 76.56° from 54.09 km [NASA/GSFC/Arizona State University].
Low basaltic shield volcanoes like those in the Hortensius region also have summit craters (Example 2). The crater on the Copernicus mound lacks a prominent rim crest, but high-resolution NAC-derived topography would better help us differentiate between a degraded impact crater and a volcanic crater in this case.

Example 2: Mare domes of Hortensius, west by southwest of Copernicus, in Oceanus Procellarum. Low profile, basaltic shield volcanoes, from a dramatic LROC NAC oblique observation, about 16.6 km-wide field of view from a mosaic of the left and right frames from LROC NAC M1108418130, spacecraft and camera slewed 56.7° west of a descending nadir, LRO orbit 15626, November 24, 2012; illumination incidence angle 74.56° at an average resolution of 2.87 meters, from 112 km over 7.28°N, 332.85°E [NASA/GSFC/Arizona State University].
2. Cratered Impact Debris?

Impact debris often appears dome-shaped and sometimes lacks craters (Example 3), although these mounds are frequently cratered.

Example 3: Bouldery Mound in Anaxagoras. 910 meter-wide field of view from LROC NAC M155309869RE, LRO orbit 8022, March 21, 2011; incidence angle 72.1° and resolution 88 cm per pixel from 42.15 km [NASA/GSFC/Arizona State University].
Larger mounds to the north of Today's Featured Image also exhibit craters near their peaks (Example 4). This type of cratered mound is fairly common on the floor of large impact craters.

Example 4: Similar debris and impact melt fallout mounds observed to the north (yellow arrow) of the bouldery mound (blue arrow) on the north floor of Copernicus. Both are comprised of impact debris and wall materials. Image is cropped portion of LROC NAC controlled mosaic COPERNICLOB [NASA/GSFC/Arizona State University].
3. Blocks as Remnants of Impact Melt that Once Draped the Mound?

Lumpy mounds on the floor of Rutherfurd crater (Example 5) are littered with the broken fragments of impact melt rocks. These rocks formed as sheets of impact melt draped over the crater floor. Over time, this sheet of rock slowly breaks up and dis-aggregates.

Example 5: The Lumpy floor of Rutherfurd crater; 1050 meter wide field of view from LROC NAC observation M1123653329R, LRO orbit 17769, May 20, 2013; resolution 1.05 meters, incidence angle 81.13° from 50.43 km [NASA/GSFC/Arizona State University].
A cracked mound on the floor of Anaxagoras crater (Example 6) illustrates what this sheet of melt might look like before dispersion through mass wasting. The boulders on the Copernicus mound could represent degraded bits of draping impact melt rocks; however, there is little evidence for a coherent layer of solidified melt as in the Anaxagoras example.

Example 6: Cracked mound on the floor of Anaxagoras; 600 meter-wide field of view from LROC NAC M122273232L, LRO orbit 3153, March 3, 2010; resolution 49 cm per pixel, incidence 73.78° from 42.18 km [NASA/GSFC/Arizona State University].
4. Squeeze-ups of Impact Melt?

Squeeze-ups of molten rock are one possible form of pseudo-volcanism that might occur in a molten sea of impact melt (Example 7).

Example 7: A possible squeeze-up of impact melt in Tycho crater; field of view 730 meters,  LROC NAC observation M1144856403R, LRO orbit 20751, January 20, 2014; illumination incidence angle 57.92° at 72 cm per pixel resolution, from 59.2 km [NASA/GSFC/Arizona State University]. [NASA/GSFC/Arizona State University].
However, squeeze-ups tend to experience tensional stress across their peak (Example 8), but in the Copernicus example, we do not see any evidence of stress fracturing across the mound. Thus, when all the evidence is considered together, the cratered mound in Copernicus is most consistent with a block of impact debris with a small impact crater near its summit -- not volcanic at all!

Example 8: Fractured mound in Stevinus crater; Structure is roughly 3 km across, LROC NAC observation M1131495601R, LRO orbit 18872, August 18, 2013; resolution 78 cm,  incidence 37.88° from 75.5 km [NASA/GSFC/Arizona State University].
Explore the entire NAC image HERE, and look for evidence of other explanations for this cratered mound.

Some Related Posts:
Shiny Mound, April 3, 2014
Hansteen α, January 15, 2014
Jackson's complexity, January 9, 2014
X marks the spot on the floor of Stevinus, January 7, 2014
Diversity of basaltic volcanism and the Marius Hills, November 5, 2013
Fall Out, October 3, 2013
That's a Relief, October 1, 2013
The Domes of Stevinus Crater, April 23, 2013
The Fourth Marian Dome, April 17, 2013
New oblique views of Gruithuisen Domes, March 4, 2013
Kagami-Mochi on the Moon, February 12, 2012
Morphology of lunar volcanic domes, February 22, 2011
Anomalous Mounds on the King Crater Floor, May 3, 2011
Constellation ROI at Hortensius Domes, April 2, 2010

Tuesday, September 3, 2013

Excavating Dark Deposits

M185955372RE_thumb-580
An approximately 250 meter crater has excavated low reflectance material from beneath the lunar surface, west of Sommering P crater, southeast of Copernicus. LROC Narrow Angle Camera (NAC) frame M185955372R; LRO orbit 12483, March 9, 2012; 9.56° angle of incidence, native resolution 1.11 meters per pixel, from 110.79 km over 1.53°N, 249.3°E, field of view 1.8 kilometers [NASA/GSFC/Arizona State University].
Sarah Braden
LROC News System

Amazing ejecta patterns from small, young craters are always something to look at on the lunar surface. Today's Featured Image displays compositional diversity in fresh ejecta. The broad, low-reflectance streaks of material are likely excavated pyroclastic materials. This approximately 250 m diameter crater is located at 2.162°N, 349.401°E, west of the crater Sommering P.

This low-reflectance material is part of a larger area called a Dark Mantle Deposit (DMD). Dark mantle deposits have lower reflectance compared to surrounding mare basalt areas and are also spectrally distinct from mare basalt. In this case, the dark mantle deposit was likely covered by a thin layer of crater ejecta.

Context with Sommering P
The small crater's location marked with a white circle in an LROC Wide Angle Camera (WAC) context image of a field of view 80 km across [NASA/GSFC/Arizona State University].
The opening image has a low incidence angle of 10° which means the Sun is high in the sky (near local noon). High-sun images are good for revealing differences in the reflectance properties of the surface. Low-sun (large incidence angle) images are better at emphasizing morphology due to topographic shading and shadowing. Incidence angle is the angle between the vector of sunlight and the vector normal to the surface. The WAC context image above has a large incidence angle (taken in early morning) which makes visible the topographic high where the crater was formed. This topographic high is a remnant of highland terrain (kipuka) surrounded by younger mare basalt deposits (smooth, flat areas). There are many other craters on the topographic high that excavate low-reflectance material, which suggests that the whole area is different from the surrounding mare basalt deposits. The high-sun WAC mosaic (below) of the same area shows the locations where the dark mantle deposit is visible. You can learn more about dark mantle deposits here!

643nm high sun, high-reflectance WAC context
LROC WAC monochrome (643 nm) high sun, high reflectance view of the same area as seen in the WAC mosaic immediately above, resolution roughly 100 meters per pixel. Note darker material around the area of the topographic high place [NASA/GSFC/Arizona State University].
Explore the full NAC image HERE to see the other craters excavating low-reflectance material.

Related Images:
Hyginus Crater and Pyroclastics
Dark Wisps in Copernicus
Polka-Dot Ejecta
Pyroclastic Excavation

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.

Saturday, April 6, 2013

Do large impacts always erase surface mineralogy?

Our present all-encompassing view of the nearside landmark lunar crater Copernicus seems only a little different than the best photography from Earth. Only 20 degrees west and less than 10 degrees north of the 'center' of the Moon's tidally-locked hemisphere, the round rim appears only slightly oblong from angle seen from our backyards. Its general brightness, both inside and out, wash out much of the detail seen in this LROC Wide Angle Camera (WAC) monochrome (649 nm) montage made up of observations in six orbital passes in January 2010. Long recognized differences can easily be confirmed between the northwest quadrant and the remaining three-quarters of the crater floor may be more extraordinary than previously believed possible [NASA/GSFC/Arizona State University].
EDITORIAL NOTE: One of a handful of features on the Moon's nearside detectible to the naked eye, it's amazing what there is still to be learned about the majestic crater Copernicus. Not as young and bright as Tycho, with rays streaming over an entire hemisphere, it's rays are impressive enough and the larger Copernicus is distinctive enough be the namesake for an entire lunar Age, the "Copernican," the Moon's most modern period, encompassing features less than about 1.1 billion years old.

This has made the Copernican family of excavations very valuable to planetary scientists who utilize Earth's Moon as the Rosetta Stone of the Solar System (and, increasingly, our Earth - the planet with which it has shared precisely the same space in the universe for approximately 4.575 billion years.

Most likely mapped first by Galileo, the 93 kilometer impact crater has since his time been drawn and redrawn with with increasing precision and appreciation. Since the 19th century, and definitely since the latter half of the 20th century, Copernicus may be the lunar crater most individually photographed from Earth. A highly oblique orbital image captured from Lunar Orbiter 2, November 24, 1966, is one of only a handful of images popularly celebrated as a "Photograph of the Century." 

Detail (highly resampled) from Lunar Orbiter 2-162, oblique view from 26 km over the lunar surface south of Copernicus crater, November 24, 1966 [Moonviews].
That delicate telemetry was recovered and reprocessed by the phenomenal Lunar Orbiter Image Recovery Project (LOIRP) in 2009. Without question, we have learned a great deal about the Moon since 1957, but, until recently, not very much more about Copernicus crater than might have been inferred using a decent telescope here on Earth. It's complexity and subtle albedo has defied definitive understanding.

We have known for some, for example, it has at least two (or three) central peaks, and mulled over tantalizing indications of a twin set of widespread rays - hinting at a near simultaneous double impact. High-resolution analysis of its wide interior achieved greatest progress in study of the continued arrival of unambiguously remote sensing from India's Chandrayaan-1 and the U.S. Lunar Reconnaissance Orbiter (LRO) after beginning its on-going mission in close polar orbit in 2009. 

Hints that the northwest quadrant of its interior floor is very distinct from the remaining three-fourths slowly have finally come into focus, hopefully to stay.

The demarcation between the character of the western and eastern north floor of Copernicus has just become more obvious as images from LRO continued to improve. Those differences are particularly striking in spectral analysis, by the Clementine orbiter in 1994, for example. LROC WAC observation M147109260CE (643 nm), spacecraft orbit 6813, December 16, 2010; angle of incidence 77.97° at 60 meters per pixel resolution, from 43.13 km [NASA/GSFC/Arizona State University].
Now the distinguished lunar and planetary scientist Carle Pieters and a team at Brown University have added another set of clues to sharp lines from remote sensing of the northwest quarter of the floor of Copernicus that might have everyone refining or completely revising set theories about what happens in those fantastic and brief hours immediately following a highly energetic crater-forming impact.

Pre-existing mineral deposits on the Moon (sinuous melt, above) have survived impacts powerful enough to melt rock. Not detectable in the crater image (inset), deposits are visible only in light at certain wavelengths [NASA/Deepak Dhingra].
Brown University — April 2 — Despite the unimaginable energy produced during large impacts on the Moon, those impacts may not wipe the mineralogical slate clean, according to new research led by Brown University geoscientists.

The researchers have discovered a rock body with a distinct mineralogy snaking for (28.9 km) across the floor of Copernicus crater, a 60-mile-wide hole on the Moon’s near side. The sinuous feature appears to bear the mineralogical signature of rocks that were present before the impact that made the crater.

The deposit is interesting because it is part of a sheet of impact melt, the cooled remains of rocks melted during an impact. Geologists had long assumed that melt deposits would retain little pre-impact mineralogical diversity.

Large impacts produce giant cauldrons of impact melt that eventually cool and reform into solid rock. The assumption was that the impact energy would stir that cauldron thoroughly during the liquid phase, mixing all the rock types together into an indistinguishable mass. Identifying any pre-impact mineral variation would be a bit like dumping four-course meal into a blender and then trying to pick out the potatoes.

But this distinct feature found at Copernicus suggests that pre-existing mineralogy isn’t always blended away by the impact process.

“The takeaway here is that impact melt deposits aren’t bland,” said Deepak Dhingra, a Brown graduate student who led the research. “The implication is that we don’t understand the impact cratering process quite as well as we thought.”

Close up view of the feature marked with light green, designated "Surrounding Melt (Fe-Ca rich Pyroxene)" in the study illustration immediately above. LROC Narrow Angle Camera (NAC) observation M175408129R, spacecraft orbit 10984, November 8, 2011; resolution 41 cm per pixel from 26.06 kilometers [NASA/GSFC/Arizona State University].
The findings are published in online early view in the journal Geophysical Research Letters .

Copernicus is one of the best-studied craters on the Moon, yet this deposit went unnoticed for decades. It was imaging in 83 wavelengths of light in the visible and near-infrared region by the Moon Mineralogy Mapper — M3 — that made the deposit stand out like a sore thumb.

M3 orbited the Moon for 10 months during 2008-09 aboard India’s Chandrayaan-1 spacecraft and mapped nearly the whole lunar surface. Different minerals reflect light in different wavelengths at variable intensities. So by looking at the variation at those wavelengths, it’s possible to identify minerals.

In the M3 imaging of Copernicus, the new feature appeared as an area that reflects less light at wavelengths around 900 and 2,000 nanometers, an indicator of minerals rich in magnesium pyroxenes. In the rest of the crater floor, there was a dominant dip beyond 950 nm and 2400 nm, indicating minerals rich in iron and calcium pyroxenes. “That means there are at least two different mineral compositions within the impact melt, something previously not known for impact melt on the Moon,” Dhingra said.

It is not clear exactly how or why this feature formed the way it did, the researchers say. That’s an area for future study. But the fact that impact melt isn’t always homogenous changes the way geologists look at lunar impact craters.

“These features have preserved signatures of the original target material, providing ‘pointers’ that lead back to the source region inside the crater,” said James W. Head III, the Scherck Distinguished Professor of Geological Sciences and one of the authors of the study. “Deepak’s findings have provided new insight into the fundamentals of how the cratering process works. These results will now permit a more rigorous reconstruction of the cratering process to be undertaken.”

Carle Pieters, a professor of geological sciences at Brown and the principal investigator of the M3 experiment, was one of the co-authors on the paper, with Peter Isaacson of the University of Hawaii.

Tuesday, March 5, 2013

Copernicus collapse pit

Collapse feature in the impact melt on the floor of Copernicus, field of view 430 meters, from LROC Narrow Angle Camera (NAC) observation M168333206L, LRO orbit 9941, August 18, 2011; resolution 40 cm per pixel from 25.4 kilometers. Originally posted to illustrate "Failed Skylights of Copernicus," January 24, 2012 [NASA/GSFC/Arizona State University].
Sarah Braden
LROC News System

A fresh collapse feature within the impact melt floor of Copernicus crater is 330 meters across (that's about 3 American football fields wide!). At one point the impact melt in this area was flat, but then the area collapsed forming the feature here (located at 10.204°N, 339.998°E). The rim of the depression is still very fresh with outcrops and boulders.

An estimate of the feature's depth is approximately 50 meters, based on shadows from another NAC image of the same area. There are a few possible causes for the collapse.

A subsurface void may have formed as the impact melt flowed and cooled. Subsurface voids occur when melt emplaced shortly after the impact drains away deeper into the impact cavity. Perhaps a small bolide impacted the surface and instigated the collapse of the structurally weak void. Alternatively, the collapse might be due to seismic shaking from moonquakes disturbing the weak section of the melt deposit.

Oblique view of the featured collapse pit, from well to the east of Copernicus; a montage of the left and right frames of LROC NAC observation M193025138 (thumbnail at bottom), orbit 13472, May 30, 2012. Spacecraft slewed from 63.11° from nadir [NASA/GSFC/Arizona State University].
This collapse feature is much larger in diameter than the mare pits: the Mare Ingenii pit is about 130 meters in diameter, the Marius Hills pit is about 65 meters and the Mare Tranquillitatis pit is around 100 meter across.

Pits in mare basalt may have formed when a portion of a lava tube collapsed. The subsequent pit is a skylight that leads into the intact lava tube. Impact melt pits are common within impact melt deposits like the one here in Copernicus, however the depression in the Feature Image is larger in diameter than average impact melt pit. Perhaps in this case the subsurface void was larger, or the surface layer of impact melt was structurally weaker, resulting in a larger collapse area.

Arrow marks location of the featured collapse pit, near an north-south contact between distinct impact melt types, easier to visualize, perhaps, in color and other images highlighting lunar surface albedo. LROC Wide Angle Camera (WAC) monochrome mosaic M147109260C, orbit 6813, December 16, 2010; resolution 60 meters from 43 km, angle of incidence 78°
A previous Featured Image, "Copernicus Seen Looking Straight Down," featured a mosaic of Copernicus's floor (9.62°N, 339.92°E, 93 km in diameter), but today's Featured Image offers much higher resolution.

Explore the entire NAC frame for more high resolution impact melt deposits, HERE

Related Images:
Copernicus Seen Looking Straight Down
Copernicus Central Peak
Natural Bridge on the Moon!
Impact Melt Pit
Failed Skylights of Copernicus

Wednesday, February 20, 2013

Dark Mantle Deposit (DMD) Excavations

Thin Skin? A patch of Dark Mantle Deposits, prominent albedo features of west and east Sinus Aestuum (southeast of Copernicus) have been over-turned by relatively recent impact, uncovering much brighter material not far below the surface. From LROC Narrow Angle Camera (NAC) observation M1103666930R, orbit 14961, September 30, 2012; resolution 94 cm per pixel. LROC Featured Image center 4.591°N, 344.348°E, field of view above is 545 meters across [NASA/GSFC/Arizona State University].
Hiroyuki Sato
LROC News System

Dark Mantle Deposits (DMDs) are diffuse deposits with a very low albedo, which are the remnants of pyroclastic eruptions. Sinus Aestuum is a DMD near Copernicus crater.

Today's Featured Image (covers) a portion of one of the lowest-reflectance areas in this DMD (see next WAC context images below), about 150 km southeast from Copernicus.

In the opening image, the lowest-reflectance materials are located at the rims and the ejecta of the multiple small craters (less than 20 meters in diameter), indicating that these dark materials are in the shallow subsurface.

Context view of western Sinus Aestuum and surrounding areas in a LROC Wide Angle Camera (WAC) monochrome mosaic centered on 4.60°N, 344.38°E. The NAC footprint (blue box) and the location of opening image field of view (yellow arrow) are indicated [NASA/GSFC/Arizona State University].
On the other hand, the two craters near the middle of this image display relatively high reflectance materials and do not expose any dark deposits from beneath the surface. That means that the lateral extent of these low-reflectance pyroclastic materials is somewhat discontinuous.  Looking at the ejecta blankets of craters within lunar DMDs is one of the best ways to estimate the extent and thickness of lunar pyroclastic deposits.  In the case of regional DMDs like Sinus Aestuum, the pyroclastic glasses that comprise these deposits represent one of the most accessible lunar resources that could be used by future human explorers to enable extended lunar surface operations.

A higher (sunrise) illumination angle normally emphasizes terrain relief over albedo, and vice versa, though in this full resolution crop from the LROC WAC mosaic (below) the contrast in local albedo are still quite evident [NASA/GSFC/Arizona State University].
The full WAC mosaic covers the western dark mantle deposit field of western Sinus Aestuum, an approximately 150 kilometers wide field of view captured over four sequential orbital passes in December 2011 [NASA/GSFC/Arizona State University].
Explore the DMDs at Sinus Aestuum in full NAC frame yourself, HERE.

Related Posts:
Pyroclastic Trails
Pyroclastics and Vent
Hyginus Crater and Pyroclastics
Pyroclastic Excavation
Rima Bode: Constellation Region of Interest

Unrelated visually, both Lunar Prospector (1998-99) and Japan's SELENE-1 (Kaguya) detected perhaps the highest rates of radioactivity stretching from Fra Mauro to west of Copernicus, represented above in a signature of Thorium. Remote sensing shows a similar, only slightly less prominent detection of Uranium, also.

Thursday, September 6, 2012

LROC: Pyroclastic Trails

Northeastern rim of unnamed crater 340 km southeast of Copernicus, among the Schröter and Gambart crater groups in Southern Sinus Aestuum (5.65°N, 8.71°W). A 612 meter-wide field of view from LROC Narrow Angle Camera (NAC) observation M144680787R, spacecraft orbit 6455, November 18, 2010; angle of incidence 49.39° at an original 50 cm per pixel resolution from 46.42 km. Downslope is to the bottom-right, view the original 1200 x 1200 LROC Featured Image HERE [NASA/GSFC/Arizona State University]
Hiroyuki Sato
LROC News System

The pyroclastic Southern Sinus Aestuum (5.42°N, 351.36°E) is famous for extensive dark mantle deposits (DMD), materials which have the lowest albedo (or highest optical maturity, or 'OMAT') on the Moon.

The DMD were likely formed as explosive eruptions threw out a blanket of small particles (pyroclasts).

Today's Featured Image shows a portion of unnamed crater rim located inside this DMD unit, about 2.4 km in diameter, with 4 or 5 dark streaks on its slope (see the crater's full profile in the NAC mosaic below).

The opening image highlights one of the sources for a dark streak. The right half of the image is the crater wall, and the left half is the surrounding flat area. The streak originates at nearly the top portion of the crater wall and extends down the slope. Notice that the streak is darker than the surrounding flat area some buried low reflectance materials were exposed on the middle of the slope and slid downhill.

Zoom out view of a mosaic of both the right and left frames of LROC NAC observation M144680787 (M144680787R and M144680787L). About a 3.93 km-wide field of view, sunlight from the east. Blue box indicates the location of the area shown in the LROC Featured Image released September 6, 2012. View the full size context image HERE [NASA/GSFC/Arizona State University].
Actually, the albedo around this unnamed crater is not as low as the main DMD area. The contrast is very, small but you can see a slightly higher albedo halo around the crater in the WAC context image. The dark streaks inside this crater all originate from almost the same level of the crater wall. Probably this unnamed crater excavated higher reflectance bedrock under the DMD, and spread it around the crater. Then the pyroclastic materials exposed in the wall (sandwiched between the bedrock and the ejecta) slumped down the crater wall leaving the dark streaks.

Careful investigations of the craters in the DMD by NAC images are quite useful to understand the thickness, the volume, and formation process of DMD. More and more NAC observations of DMD are expected. 

Southern Sinus Aestuum in context with Copernicus, 340 km away. Note dark streaks from rim to floor are also a feature of nearby Schröter D crater. LROC WAC monochrome mosaic (100 m/pix) centered on the subject unnamed crater (arrow), draped over LOLA altimetry data using the NASA LMMP ILIADS application  [NASA/LMMP/GSFC/Arizona State University].

Explore this pyroclastic slides by full NAC frame yourself, HERE.

Related Posts:
Dark streaks in Diophantus crater
Dark Craters on a Bright Ejecta Blanket
Alphonsus crater mantled floor fracture
Dark-haloed crater in Mare Humorum
Pyroclastic Excavation

Pyroclastic Southern Sinus Aestuum, including the unnamed crater of interest at center, as seen from Earth. 4100 x 5000 pixel Mosaic of the Moon captured by Astronominsk, August 8, 2012.

Tuesday, September 4, 2012

LROC: Dark Ejecta

Southwestern rim of crater Copernicus H (6.88°N, 341.68°E). A 930 meter-wide field of view from LROC Narrow Angle Camera observation NAC M186005514L, spacecraft orbit 12940, March 10, 2010; incidence angle is 10° at 0.93 meters per pixel resolution. View the 1000 px original LROC Featured Image HERE [NASA/GSFC/Arizona State University].
Hiroyuki Sato
LROC News System

Copernicus H (about 4.4 km in diameter, latitude 6.88°N, longitude 341.71°E) , a satellite crater of Copernicus crater, is located 56 km southeast of Copernicus (93 km diameter crater located in eastern Oceanus Procellarum). The opening image highlights a part of the Copernicus H crater rim (see blue square in the next image). The upper right portion of the image with bright/dark streaks corresponds to the crater wall, and the bottom left low reflectance part is the surrounding flat area. The low reflectance materials extend from the rim down the slope into the crater. What is the origin of these dark materials? Is the material mature soil? Impact melts? Pyroclastic deposits?

Zoomed out view of NAC M186005514L. Field of view about 5.7 km. Blue box indicates the location of today's Featured Image [NASA/GSFC/Arizona State University].
As seen in the subsampled NAC image (above) and WAC context image (below), the ejecta blanket of Copernicus H shows relatively lower reflectance than the surrounding area. Normally crater ejecta has a higher reflectance because the newly-exposed material is "immature" in a space-weathered sense. Notice that the crater floor is largely filled by lower reflectance impact melt, and the high reflectance materials extend radially from the floor to the crater rim. These brighter materials are the debris on the slope of the crater wall that are mass-wasting gravitationally toward the crater center.

Looking at the WAC context image below, it is likely that Copernicus H excavated some low reflectance materials underlying the ejecta of Copernicus. Several craters located at least 45 km away from the Copernicus rim also show similar dark ejecta. Therefore, the underlying dark material must be widely distributed. What might these materials be? Pyroclastic deposits at Southern Sinus Aestuum are located at about 90 km southeast of Copernicus H, and are underlying the Copernicus ejecta. If this layer is extensively distributed under the Copernicus ejecta, subsequent impacts with sufficient energy could have excavated the dark materials.

To unravel these complicated stratigraphic relations from orbit, accurate spectral data and an understanding of the effects of space weathering are necessary. New measurements from LRO, SELENE-1 (Kaguya), and Chandrayaan-1 are providing lunar scientists with the needed information!

Copernicus H and surrounding area in WAC monochrome mosaic (100 m/pix). Image center is 6.88°N, 341.73°E. The blue box indicates the footprint of full NAC frame [NASA/GSFC/Arizona State University].

Explore this dark ejecta in full LROC NAC image yourself, HERE.

Related Posts:
Dark Craters on a Bright Ejecta Blanket
Dark halo crater
Just Another Crater?
Dark Impact Melt Sheet
A Beautiful Impact
Pyroclastic Excavation

NASA ILIADS (LMMP) simulated mid-day point of view 40 km over the lunar surface southeast of Copernicus. Copernicus H and it's floor are at upper center in this compilation from LROC Global 100 meter resolution WAC mosaic with LOLA altimetry at 128 meters per pixel. The darker surface further southeast from Copernicus past Copernicus H is identified as a radioactive hotspot, with signatures of thorium and uranium in Lunar Prospector, SELENE and other surveys [NASA/GSFC/LMMP/Arizona State University].

Wednesday, August 22, 2012

LROC: Looking over a four-leaf clover..

Several shallow depressions, secondary craters, dot the surface of Mare Imbrium, in this case near a rocky ext Mons la Hire (near Euler and Lambert), and giving the impression of a four leaf clover. LROC Narrow Angle Camera (NAC) M190780929RE, spacecraft orbit 13158, May 4, 2012; resolution 1.5 meters and field of view 1500 meter across. View a larger cropped image HERE.  [NASA/GSFC/Arizona State University].
Drew Enns
LROC News System

These large, ~500 m diameter, depressions are characteristic of secondary impacts on the Moon. When a bolide (asteroid or comet) hits the surface of the Moon a crater forms at the impact site. To create a secondary crater material is ejected from the impact site at about a 45° angle. If the ejecta travels less than the escape velocity, it falls back down to the Moon. Since the escape velocity on the Moon (~2.4 km/s) is much lower than that at which bolides typically impact the Moon (10-20 km/s) secondary craters often have a distinctive appearance. These lower velocity impacts result in irregularly shaped craters. Sometimes secondaries land in clumps and create distinctive patterns, such as the "four leaf clover" whimsically identified in today's Featured Image.


Smaller scale context image shows the relationship of the out-cropping above with the larger Mons La Hires 30 km to the southeast.  Image width is 650 km, LROC WAC mosaic [NASA/GSFC/Arizona State University].
If the secondaries featured today were formed in another impact, which impact created them? The number of craters in our secondary group is fairly large, so the parent crater cannot be small. In the context image covering a slightly broader field of view below, other secondary chains (red arrows) appear to point to the southeast. Maybe zooming out further will reveal the mystery parent crater!

A quick look over the 605 kilometers from the southwestern tip of  the northwest Mons La Hire outcrop and the center of Copernicus, courtesy of the ILIADS application released by NASA/LMMP. The immediate and long-range legacy of the Copernicus event was lasting.
It looks like Copernicus is the parent crater! That makes sense. Copernicus fits our criteria. These secondary chains have been previously identified, but the fact that they were sourced from Copernicus crater hundreds of kilometers away is remarkable. The impact cratering process really is amazing.

Can you identify other secondary craters in the full LROC NAC frame, HERE?

Related Posts:

Wednesday, July 18, 2012

LROC: Second new oblique of Copernicus central peaks, from the west...

West-to-east view of the Copernicus crater central peak complex. Detail from LROC Narrow Angle Camera (NAC) mosaic of M19666538lL & R, LRO orbit 13,981, July 11, 2012; general resolution is 4 meters.  [NASA/GSFC/Arizona State University].
Mark Robinson
Principal Investigator

Lunar Reconnaissance Orbiter Camera
Arizona State University

LROC captured this spectacular view of the heart of Copernicus crater just before (local) sunset, July, 11 2012. Compare it to the reverse view point snapped from the East near local sunrise, May 5.

LROC can only be slewed large angles while looking away from the Sun, otherwise its radiators are exposed to the hot Moon and the LROC Wide Angle Camera (WAC) optics are exposed to the Sun. So back-to-back obliques are not possible on the same day.

Full 920 pixel-wide LROC Featured Image, released July 18, 2012. The sharp boundary at the base of the 700 meter high peak in the foreground is a now frozen sea of impact melt that flooded the floor of the crater in its final stages of formation. Image field of view is approximately 8 km across [NASA/GSFC/Arizona State University].
Between May and July LRO passed over the terminator (boundary between night and day) and thus the direction to the Sun reversed, in terms of LRO. On that orbit the daylight side switched from one side of the Moon to the other, at least from the perspective of the spacecraft. For example if LROC had just completed mapping the nearside, as it crossed the terminator we skip the farside and start remapping the nearside!


Central peak with bouldery outcrops and streak seen from the east (top), and the west (bottom) [NASA/GSFC/Arizona State University].
Back to Copernicus, what are those dark streaks we see on the peak? In the comparison image above, and if you skip back to the earlier post that shows the other side, that dark streak is seen on both sides of the central peak, showing that it is three dimensional within the peak. Might it be a dark rock intruded as a dike into the light colored crystalline bedrock that was brought up from beneath the deepest part of the transient cavity in the Copernicus target? Or is it simply a dark rock that is eroding and slumping down the sides of the peak?

Reduced resolution view of the entire NAC view of Copernicus crater. View 1600 pixel-wide rendition, HERE [NASA/GSFC/Arizona State University].

Because of their state of preservation (despite being nearly a billion years old) and the identification of scientifically interesting mineralogy from remote sensing spectroscopy, the central peaks of Copernicus have long been coveted by lunar explorers as a prime location for a mission, including sample return. In fact, Copernicus was considered as an Apollo landing site, and was recently proposed as a target for a robotic rover within the Discovery program. To sample the peak you wouldn't need to scale the slopes - in the top image you can see many rocks and boulders that have rolled down from the summit, lying on the relatively flat floor waiting to be picked up.

Subsampled synoptic view of the central peak complex, field of view approximately 18 km across, the tallest peak rises more than 1300 meters above the floor. View the larger 1600 pixel-wide rendition, HERE  [NASA/GSFC/Arizona State University].

When and how will we first visit this fascinating, geologically rich area? Imagine the view astronauts will have as they descend to the floor and then step out at the base of this peak. Explore the full LROC NAC oblique mosaic release, HERE.

Previous LROC Featured Images highlighting Copernicus:

Copernicus - Looking Straight Down (June 28, 2012)