Elemental and topographic mapping of lava flow structures in Mare Serenitatis on the Moon

2018 ◽  
pp. 207-224 ◽  
Author(s):  
A. Grumpe ◽  
C. Wöhler ◽  
D. Rommel ◽  
M. Bhatt ◽  
U. Mall
Author(s):  
C. Wöhler ◽  
A. Grumpe ◽  
D. Rommel ◽  
M. Bhatt ◽  
U. Mall

The detection of lunar lava flows based on local morphology highly depends on the available images. The thickness of lava flows, however, has been studied by many researchers and lunar lava flows are shown to be as thick as 200 m. Lunar lava flows are supposed to be concentrated on the northwestern lunar nearside. In this study we present elemental abundance maps, a petrological map and a digital terrain model (DTM) of a lava flow structure in northern Mare Serenitatis at (18.0° E, 32.4° N) and two possible volcanic vents at (11.2° E, 24.6° N) and (13.5° E, 37.5° N), respectively. Our abundance maps of the refractory elements Ca, Mg and our petrological map were obtained based on hyperspectral image data of the Moon Mineralogy Mapper (M3) instrument. Our DTM was constructed using GLD100 data in combination with a shape from shading based method to M3 and Lunar Reconnaissance Orbiter (LRO) Narrow Angle Camera (NAC) image data. The obtained NAC-based DEM has a very high effective resolution of about 1–2 m which comes close to the resolution of the utilized NAC images without requiring intricate processing of NAC stereo image pairs. As revealed by our elemental maps and DEM, the examined lava flow structure occurs on a boundary between basalts consisting of low-Ca/high-Mg pyroxene and high-Ca/low-Mg pyroxene, respectively. The total thickness of the lava flow is about 100 m, which is a relatively large value, but according to our DEM the lava flow may also be composed of two or more layers.


The unaided eye can see roundish dark spots on the Moon set in a brighter back­ground. Telescopic observation of these dark spots, called maria (plural of mare , sea) reveals that they are nearly level terrain sparsely covered with craters. The brighter surroundings or terrae are from shadow measurements found to be higher, some 1 to 3 km above the maria. The terra elevations scatter widely, reaching several kilometres in the mountain ranges. The most prominent of these ranges occur as peripheral mountain chains around the near-circular maria. Examples are the Apennines, the Alps, the Carpathians, and the Altai Scarp. These arcuate chains surround the maria as the crater walls surround crater floors, an analogy that can be carried further and implies, apart from scale, a similar origin. This origin is almost certainly impact by massive objects. In the case of the impact maria and pre-mare craters, the source of the objects appear to have been a satellite ring around the Earth through which the Moon swept very early in its history, in its outward journey from its position of origin very near the Earth (Kuiper 1954, 1965). The post-mare craters are presumably mostly asteroidal (and partly comet­ary) in origin and related to the craters observed by Mariner IV on Mars. The estimated time dependencies of these two crater-forming processes are shown schematically in figure 1. A fuller discussion of this problem has been given else­where (Kuiper, Strom & Poole 1966; Kuiper 1966). The higher asteroidal impact rate on Mars, by a factor of about 15, as derived from the Mariner IV records, is interpreted as being due to the greater proximity to the asteroid ring. The num­erical factor approximately agrees with theory. Mars apparently lacks the equiva­lent of the initial excessively intense bombardment of the Moon (attributed to impacts by circumterrestrial bodies); unless, of course, the entire Martian surface has been molten and is directly comparable to the lunar maria. This does not seem probable but can at present not be ruled out; if true, the earliest surface history would have been erased. The nature of the mare surface has, during the past decade, been an object of much, perhaps too much, speculation. With the several recent successful lunar reconnaissance missions completed, the older interpretation of the maria as lava beds, based on telescopic observation, has been abundantly confirmed. Four options discussed in recent literature are analysed in Kuiper (1965, §§A, B, pp. 12–39). Among the most potent arguments for the lava cover of the maria are the prominent lava flows observed on Mare Imbrium and Mare Serenitatis, each having a characteristic colour. A map of some Mare Imbrium flows is found in figure 2.


Icarus ◽  
2010 ◽  
Vol 209 (2) ◽  
pp. 323-336 ◽  
Author(s):  
Shoshana Z. Weider ◽  
Ian A. Crawford ◽  
Katherine H. Joy

2009 ◽  
Vol 114 (E11) ◽  
Author(s):  
Lynn M. Carter ◽  
Bruce A. Campbell ◽  
B. Ray Hawke ◽  
Donald B. Campbell ◽  
Michael C. Nolan

The following summarizes certain previously unpublished inferences regarding the lunar surface that were included in a more extensive oral presentation. Infrared (Shorthill & Saari 1961; Murray & Wildey 1964) and radar (Pettengill & Henry 1962) observations of the Moon acquired in 1960–62 demonstrated that, in some cases at least, conspicuously bright craters like Tycho also are characterized by the presence of more consolidated material at or very near the surface and by considerably rougher terrain on the metre scale. Interpreting the bright craters generally as younger—and less aged—than the less conspicuous craters leads to the conclusion that the process of modification operative on the lunar surface not only gradually reduce the visible reflectivity to the average back­ground level but also smooth and insulate the surface materials. Recent observations of the infrared emission during a lunar eclipse (Saari & Shorthill 1965) and during the lunar night time (Murray, Westphal & Wildey 1967) reveal further an unexpected degree of variability in thermal properties geographically. The infrared anomalies observed during lunar light time and eclipses generally correspond and are distributed quite nonuniformly. For instance, Mare Tranquillitatis exhibits a much higher surface density of anomalies than does Mare Serenitatis. Also, Mare Crisium is characterized by a small, but real, enhancement of night time infrared emission throughout; similar enhancements are also apparent on some portions of other maria surfaces during an eclipse. Both the nonuniform distribution of infrared anomalies and the nonuniform low level enhancements imply processes on the lunar surface which in some areas preferentially produce or expose material of lower than average thermal inertia (more consolidated material) and/or in other areas preferentially remove or cover such material. Specifically, either random impact must be more effective in exposing consolidated rock in Mare Tranquillitatis than in Mare Serenitatis because of intrinsic physical differences in the host rocks of the two maria, or there has been a more rapid covering process operative in Mare Serenitatis. The broad, low level enhancements require similar selective formation or removal processes. These inferences would seem to be most compatible with a terrain characterized by a range of lithologies and, possibly, by periodic extrusion of thin blankets of new materials. It may be of importance to search for any correlation between the distribution of non-thermal visible emission and the distribution of infrared and other anomalies because the same differential surface processes may control the magnitude and distribution of both sets of phenomena.


Icarus ◽  
2013 ◽  
Vol 222 (1) ◽  
pp. 137-148 ◽  
Author(s):  
Prabhjot Kaur ◽  
Satadru Bhattacharya ◽  
Prakash Chauhan ◽  
Ajai ◽  
A.S. Kiran Kumar

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