Showing posts with label GSFC. Arizona State University. Show all posts
Showing posts with label GSFC. Arizona State University. Show all posts

Monday, October 17, 2011

LROC Quickmap improvements dazzle

Roof top of the Moon (10,786 meters (35,387 feet) above global mean elevation), as determined by LRO investigators a year ago, is high on the lopsided eastern rim of Engel'gardt crater (5.7°N, 159.0°E), in the farside highlands; 44 km-wide and seen here immediately left of center in a field of view roughly 325 km wide and includes the northern Korolev basin (below). All these features are difficult to spot in cameras, not least of the reasons being in an area criss-crossed with superimposed bright rays. After this past weekend, however LROC premiered an overlay with a variable opacity showing their Global Wide Angle Camera (WAC) digital terrain model (DTM) in false color (here seen at the default 30% over the hybrid LROC NAC and WAC Global mosaic) is now an integral part of the ACT-REACT LROC Quickmap feature on their popular website, improving the map's usefulness when searching through LROC's vast data contribution to the Planetary Data System immeasurably [NASA/GSFC/Arizona State University].
An hour "playing" with the 'new and improved' LROC Quickmap enabled us to assemble this exploration of the tenuous connection between the Marius Hills and the Reiner Gamma albedo feature (with it's attendant crustal magnetic anomaly), both familiar features in Oceanus Procellarum. It's a place to begin digging deeper into the three dimensions of data from LROC already available to the public, especially with the new addition of the LROC DTM. Is Reiner Gamma's long swirl and it's intense local magnetism a result of a sub-surface flash flood of volcanic material? With the new LROC DTM overlay, it's much easier to demonstrate those features with little to no corresponding topographic expression and others nearly invisible except at very high sun angles [NASA/GSFC/Arizona State University].
Not very far from the Moon's highest point is what appears to be it's lowest, within the South Pole-Aitken basin, at the bottom of the large crater on the southern floor of Antoniadi (or, near 70.38°S, 187.2°E, over 9,000 meters below global mean elevation). This mix of LROC WAC imagery overlaid with the false-color WAC DTM adds more than just a feeling of depth of field. Most camera views of the floor of Antoniadi, and mare-filled features everywhere else on the Moon, the surface looks misleadingly flat. Even at 500 meter per pixel resolution, the wide deep flat floor of Antoniadi shows an uneven, almost "dune-like" roughness, lost in surveys based on albedo alone [NASA/GSFC/Arizona State University].
Another instant study increases the opacity of the LROC WAC DTM overlay from the base WAC optical mosaic of a nearside portion of the lunar south pole environs, offering an informative look at one of the Moon's last terra incognitas [NASA/GSFC/Arizona State University].
Related Post: LROC Quickmap

Wednesday, October 12, 2011

LROC: Perched Boulders

The crest of a linear floor fracture wall is intermittently covered by boulders and smoothed terrain. The largest boulders (lower part of image) are around 30 meters across. LROC Narrow Angle Camera (NAC) M159065590R, LRO orbit 8575, May 3, 2011; from top to bottom (north is to the right) field of view is 960 meters. See the full size LROC Featured Image HERE [NASA/GSFC/Arizona State University].

Lillian Ostrach
LROC News System

Boulders are found nearly everywhere on the Moon, and LROC NAC images allow scientists to study boulder populations. Why would anyone want to spend their time looking for boulders? Boulders represent erosional products on the Moon and can be used to help interpret geologic features and derive a geologic history for a region. Presently, erosion on the Moon largely occurs as a result of micrometeorite bombardment (for a short discussion, check out the Relative Age Relationships Featured Image). For example, the presence of boulders surrounding a 100 meter diameter crater in the mare suggests that when the crater formed, the impactor punched through the layer of regolith and excavated bedrock. Similarly, the boulders perched on wrinkle ridge crests and on the walls of sinuous rilles represent bedrock that is eroding out of these features over time. Perhaps the density or frequency of boulders on wrinkle ridge crests may be used to determine relative ages between features within a region. However, because erosion can be controlled by rock type and how fractured or deformed the rocks are, scientists need to carefully interpret their observations of boulder populations.

Today's Featured Image highlights boulders perched on the crest of a linear floor fracture wall within the central peak ring of Schrödinger basin (73.22°S, 133.82°E).Many of the boulders are around 5 to 10 meters across (although some are smaller), but near the lower edge of the image above the boulders are much larger, around 20to- 30 meters across. There are also more large boulders exposed downslope of the 20 - 30 m boulders compared to other boulder clusters. Why is there an apparent discrepancy?

To answer, we should consider several things. First, we must determine whether the boulders originate from the crest (in-situ) or are impact-derived (that is, they deposited by a nearby impact). Taking a look in the full Narrow Angle Camera frame, there is an approximately 7 kilometer in diameter Eratosthenian-Age crater about 30 kilometers north of the fractures. However, while there are boulders around 30 meters in size located in clusters surrounding the crater the continuous ejecta blanket (for a crater generally) is confined to one crater diameter. Since the fractures are much farther than 7 km from the crater the boulders on the fracture wall crest are probably not derived from that crater.

What about other nearby craters? While there are several craters nearby (check out the LROC WAC context below), none of them are particularly fresh nor bouldery. Based on these observations, the boulders probably orignated in-situ as a result of erosion. Thus, the apparent discrepancy in boulder sizes along the crest may be related to the deformation of the rock during fracture formation and mare flooding of Schrödinger. Right now, though, we do not have a definitive answer; however, to examine this topic further, we would need to complete a survey of boulder sizes and distributions along the length of the fractures. Even then, we may not be able to explain why some boulder groupings contain larger sized boulders.

LROC Wide Angle Camera (WAC) monochrome mosaic showing and area located slightly north of the center of Schrödinger basin with the northern portion of the central peak ring near the top of the image. (Asterisk notes the location of today's Featured Image image.) View the full size LROC WAC context mosaic showing the deep interior of Schrödinger basin HERE [NASA/GSFC/Arizona State University].
Now that we found evidence to suggest that the boulders are probably related to the erosion of the crest of the fracture wall we need to try to explain the smoothed portions of the crest.

In the opening image, there are boulder clusters separated by smoothed areas. What is this smooth stuff? Regolith, the lunar soil, is generated by impacts - big and small - and over time accumulates on the lunar surface. When a surface is covered entirely by regolith, it looks smooth and sometimes has a textured appearance. So, these smooth regions are accumulations of regolith on the wall crest and also along the fracture walls. But then why isn't the crest all smooth, or all bouldery? The illumination and where the shadows lie across the ridge crest may be a clue; these smooth areas have shadows that are not in-line with the bouldery portions of the crest and look like they may be lower topographically than the bouldery parts or may be less steeply sloped than the parts of the crest where boulders are. Again, taking a look at the full NAC frame may help, too, because in the full image there are other smooth regions that are associated with obvious changes in topography and slope along the crest. If we then assume that the smoother regions have a shallower slope at the crest, we may have an answer: boulders are more likely to form along steep slopes of crests where the slope break is steepest (here along the fracture wall crest, or along wrinkle ridges). This is only one explanation based on visual explanation, but we really should take some time to measure slopes in a NAC-derived Digital Terrain Model (DTM) to be certain that we are on the right track.