Title: History of the Moon and Mercury
1History of the Moon and Mercury
2In This Lecture
- Moon/Mercury (mostly 4.5 3.0 Ga)
- Formation events
- Basin sequences
- Plains volcanism
- Tectonics
- Atmospheres and polar volatiles
0.27 RE 1.00 AU
Surface activity on the Moon and Mercury mostly
died off about 3 Ga
as opposed to
Surface history of Venus is only available from
1.0 Ga onward
Surface activity and history of Mars spans its
entire existence
0.38 RE 0.39 AU
3Introduction to the Moon
- Moon is in a 11 spin orbit resonance with the
Earth - Two major surface units
- Heavily cratered light toned Terrae
- Less cratered dark toned Maria
- Crater size distribution follows a power law with
an exponent close to -2 - Expected from fragmentation mechanics
- Extensive work on relative ages and stratigraphy
relationships - Apollo and Luna samples allowed that work to be
attached to absolute dates
4Formation of the Moon
- Previous theories
- Co-accretion
- Fission of spinning Earth
- Capture of rogue planetisimal
- Apollo results (and common sense)
- Moon depleted in volatile elements
- Moon depleted in siderophile elements
- Oxygen isotope ratios similar
- Capture of a rouge planet would be a dynamical
miracle - Fission questionable since Moon doesnt orbit in
equatorial plane - Current paradigm is Giant impact
- Earth close to final size
- Mars-sized impactor
- Both bodies already differentiated
- Both bodies formed at 1 AU
From Robin Canup, SWRI Boulder
5Bulk composition and orbital state
- Iron cores of both bodies stay in the Earth.
- About 1 lunar mass of material goes into orbit
outside the Earths Roche limit. - Most of the matter in the Moon is from the
impacting body. - Heat of debris-disk removes volatiles
From Robin Canup, SWRI Boulder
- Earths spin and Moons orbit become locked in
11 Cassini state - Moons orbit expands by a few cm/year
- Earths rotation slows
6Magma Ocean
- Accretion of lunar material into the Moon within
a few years! - High-accretion rates mean surface is molten
- Magma ocean probably a few hundred km thick
- Apollo 11 returned highland fragments, first
suggestion of Magma ocean - Idea since extended to other terrestrial planets
- Different minerals condense at different times
- Pyroxene and Olivine sink
- Plagioclase-feldspar floats
- Moon gains global anorthosetic upper crust
- The leftover stuff sandwiched between these
layers finally condenses - Rich in incompatible elements such as potassium
(K), rare-Earth elements (REE) and phosphorus (P) - Collectively called KREEP 4.3 Ga
- Crust solidifies, sealing in radiogenic heat,
which will become important 0.5 Gyr later
7Final Internal Structure
- Crustal Thickness Asymmetry
- Average crust 54-62km thick (45km at Apollo
sites) - Far-side crust is much (about 15km) thicker
- Crustal asymmetry is one the central questions in
lunar science - Mantle
- Ambiguous seismic results at 500-800km
- Upper 800km very low attenuation
KREEP
8- Core size?
- Remnant magnetism shows there was once a liquid
core - Moment of inertia (0.39) consistent with very
small core (200-450 Km) - Interaction with the solar wind suggests a solid
conducting core of 340 90 km (1-3 of the lunar
mass) - Poor seismic data are consistent with liquid core
(s-wave attenuation) - but Apollo heat flow measurements are very low
- Free oscillation periods consistent with a single
rigid body.
9Large Basins Form
- Bombardment of the Earth-Moon system continues
- Heavily cratered lunar highlands form
- Saturation equilibrium reached i.e. new impacts
remove previous craters - Several large basins form, which divide lunar
stratigraphy into different epochs - Fracture lithosphere to great depths
- Excavate lower crustal material e.g. KREEP
10The Moon at 3.8 Ga
- Crater saturation
- Lithosphere homogenized to depths of 20km
- Regolith generated to depths of 10s of meters
- Cratering rate declining dramatically
- Several large basins formed Aitken basin 2200
Km - Whole Moon has highland appearance
- Small amounts of mare material have appeared but
were eliminated by basin impacts - Radiogenic heat starting to produce large
quantities of magma
11Formation of the Maria
- Mare material originates deep in the crust
- Maria lava fill pre-existing depressions (impact
basins) - High levels of pyroxene and olivine relative to
the upper crust - Very similar to terrestrial basalt
- Except that it is completely devolatilized
- Also abnormally high in titanium
- Darker color due to higher Fe content
- Amounts are small
- Most Maria 1-2km thick
- 5km in Imbrium, 0.6km in Orientale
- Individual flows 10-40m thick
- VERY low viscosity
- Some maria material interacts chemically with the
KREEP layer as it rises - Known as KREEPy maria
- Maria erupt mostly during the Imbrian period
(3.8-3.1 Ga) - A little late Mare formation into the
Eratosthenian period but not much
12Evolution of the Maria
- Maria lava fill pre-existing depressions (impact
basins) - Maria does not reach surface on the far-side due
to the thicker crust. - Cryptomaria some maria can be buried
- Very smooth on scales of 100s of meters
- Weight of maria material causes subsidence
- Compression (wrinkle ridges) in the center
- Extension (graben) at the edges
- Edges of the Maria remain sharp
- Little lateral mixing from impacts
13Lunar Chronology
- Maria start forming as the heavy bombardment era
ends. - Maria crater density is much lower than the
highlands - Regolith is shallower than highlands probably a
few meters deep - Craters continue to accrue at a relatively slow
rate until present day
14Lunar Timeline
Pre-Nectarian 4.6 3.92 Ga
- Giant impact between Earth and Mars sized body
forms Moon - Magma ocean
- Olivine rich rocks crystallize (sinks)
- Anorthosetic highland formation (floats)
- KREEP formation
- Heavy bombardment
- Homogenizes regolith up to 20 km
- Large basins form
- First maria destroyed by bombardment
- Impact rate declines significantly
- Maria erupt onto surface
- Mare material fills in preexisting basins
- Lighter cratering continues
- Recent craters still have bright rays
- Polar volatiles accumulate
Nectarian 3.92 3.85 Ga
Imbrian 3.85 3.15 Ga
Eratosthenian 3.15 1.0 Ga
Copernican 1.0 0 Ga
15Mercury
16Introduction to Mercury
- Orbital period 88 days is 3/2 times the
rotational period - Orbit is eccentric (e0.21)
- Leads to hot and cold poles on the equator
- Surface is lunar-like but with important
differences - Surface units
- Intercrater plains
- Smooth plains
- Caloris basin
- Global tectonic features
17Data acquired
- Mariner 10 had three fly-bys in 1974/5
- Equatorial pass _at_ 700 km (on dark side)
- South polar pass _at_ 50,000 km
- North polar pass _at_ 400 km
- Ironically the mission was not really designed
for photogeology
- 45 photographic coverage of variable resolution
and illumination - Discovery of a dipole magnetic field
18Mercurys Abnormal Interior
- Mercurys uncompressed density (5.3 g cm-3) is
much higher than any other terrestrial planet. - For a fully differentiated core and mantle
- Core radius 75 of the planet
- Core mass 60 of the planet
- Larger values are possible if the core is not
pure iron
- 3 possibilities
- Differences in aerodynamic drag between metal and
silicate particles in the solar nebula. - Differentiation and then boil-off of a silicate
mantle from strong disk heating and vapor removal
by the solar wind. - Differentiation followed by a giant impact which
can strip away most of the mantle. - Geochemistry of mantle materials can distinguish
between these hypothesis - Lunar formation example shows there might be a
better and more-surprising answer out there.
19- Core still liquid?
- Cooling models say probably not
- Unless theres a lot of (unexpected) sulfur
- Dipole field observed by Mariner 10 spacecraft
says yes - but that could be a remnant crustal field.
- New Earth-based radar observations of
longitudinal librations core is still partly
molten
- Core freezes into a solid inner core over time
- Slowed by sulfur
- Causes planetary contraction
20Mercurys Surface Almost Lunar
- Radar returns indicate regolith-like surface i.e.
rough terrain composed of unconsolidated
fragments - Spectrally very similar to the lunar highlands
- Similar albedo and morphologies i.e. craters and
basins everywhere
- Old surfaces (craters very degraded) not heavily
cratered - Smooth plains that look volcanic but have no
basalt signature no maria - Global sets of tectonic features preserved
- Global grid of aligned very old faults
- Global grid of unaligned compressional faults
21Geologic epochs on Mercury
- Mercurys history is divided into periods similar
to the lunar examples - Pre-Tolstojan
- Tolstojan
- Calorian
- Mansurian
- Kuiperian
- No absolute dates attached as there are no
samples but crater counts yield some clues
22Spindown into a Cassini State
- Mercury likely started with a faster spin.
- Solar tides de-spun the planet to its current (59
days) spin rate - Ancient global lineament system observed
- Planet bulges less at the equator when spinning
slowly - Stresses created when rigid lithosphere readjusts
to new shape - Orientations of lineaments are a good match to
model predictions
23Pre-Tolstojan Period
- Covers events occurring before the Tolstoj impact
basin (500 km) was formed - Mercury looks very much like the lunar highlands
- Similar number of large basins (gt500 km)
- Inter-crater plains are deposited
- Removes any basins lt 500 Km
- Plains material likely volcanic although theres
no proof of this. - A handful of other large basins accumulate after
plains deposition.
24Tolstojan period
- Begins with formation of Tolstoj basin (500 km)
- Several more basins form
- Impact rate starting to significantly decline
- Smooth plains start to be emplaced
- Period ends with Caloris impact
Tolstoj impact basin
Smooth plains
25Global Contraction
- Extensive set of lobate scarps exist.
- No preferred azimuth
- Global distribution
- Sinuous or arcuate in plan
- Interpreted as thrust faults
- Evidence for an episode of global compression
- Planetary shrinkage of 1-2 Km
- Scarps are dated as Tolstoj through Calorian
periods - Probably formed over a few 100 Myr
Discovery Rupes
26Calorian Period
- Caloris impact was a major event for Mercury
- 3.9 Ga
- Impact structure is 1300 Km across
- Six concentric rings 630-3700 Km across
- Smooth plains material erupts after some delay
- Followed by compression (subsidence)
- Followed by extension (rebound)
Extensional Fractures
Compressional Ridges
27The Caloris Antipode
- Seismic waves from the Caloris impact all meet at
the antipode at the same time. - Modeling suggests vertical motions of up to 1km
- Terrain broken up into 1km sized blocks
- Official name is Hilly and furrowed terrain.
- Mariner 10 team called it weird terrain.
28Mercury Winds Down
- All the geological action for Mercury is now over
- Other geologic periods are relatively quiescent
- The rest of the Calorian sees last lobate scarps
form - Mansurian cratering rate similar to today
- Kuiperian period covers the most recent (freshest
looking) craters (1.0 Ga to present) - Ice accumulates in polar craters
29Mercurys Timeline
- Mercury forms, perhaps with a large core or
suffers a giant impact - Lithosphere forms
- Despinning results in shape change and global
tectonism - Heavy bombardment
- Homogenizes regolith up to 20 km
- Large basins form
- Volcanic flooding inter-crater plains
- Basins lt500km removed
- Core shrinks 1-2 km
- Global system of thrust faults forms lobate
scarps - Caloris impact structure forms
- Antipodal weird terrain
- Smooth plains form
- Subsidence and rebound in Caloris basin
- Lighter cratering continues
- Bright rayed craters
Pre-Tolstojan
Tolstojan
Calorian
Mansurian
Kuiperian
30Summing up
- The Moon and Mercury superficially have a lot in
common - Dominated by impacts with regolith surfaces
- Similar surface materials
- Both in a Cassini state
- Both geologically dead for Gyr
- Both currently have surface-bounded exospheres
- Both have permanent shadowing in their polar
regions probably containing water ice - But their histories and internal structure are
different
LRO Fall 2008
Messenger Spring 2008