Astronomy 405 Solar System and ISM Lecture 8 The Moon February 1, 2013.

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Presentation transcript:

Astronomy 405 Solar System and ISM Lecture 8 The Moon February 1, 2013

The Moon Highland (lighter) littered with craters Maria (darker) lava-filled craters Lunation

The Moon Small gravity => lost atmosphere => no weather => craters and footprints are preserved Take only memory, leave only footprints. - NPS BUT Apollo astronauts took rocks and soil from the Moon, and left seismometers on the Moon !!!

Caught in Action!!! But…

The Moon’s Internal Structure Moonquakes were recorded. to determine the internal structure of the Moon. No tectonic activity. Moonquakes originate from tidal strains caused by the Earth’s gravitational pulls. The Moon’s ringing caused by meteorite hits were also detected. Solid Lithosphere Plastic Asthenosphere

The Moon’s Internal Structure Moonquakes were recorded. to determine the internal structure of the Moon. Solid Lithosphere Plastic Asthenosphere The crust on the near side is thinner than the far side. - only 1 mare on the far side. - tidal forces caused the heavy side to permanently hang down toward Earth

The Moon The Moon has no measurable global magnetic field. Slow rotation, solid core => no magnetic dynamo Apollo ( s) brought back 382 kg of surface rocks and soil. Luna (Russian) brought back 0.3 kg of material. Rocks are volcanic in origin. Basalts similar to those on Earth, rich in iron and magnesium and containing glassy structures characteristic of rapid cooling. However, lunar basalts contain no water and a lower percentage of volatiles relative to refractories.

Radioactive Dating When rocks solidified, all isotopes were trapped inside. Radioactive isotopes decay into stable isotopes. Half-life of the slowest decay determined the decay rate. 235 U Pb x10 8 yr 3.28x10 4 yr  -particle = He nucleus  -particle = electron

Radioactive Dating

Isotope A decays into isotope B A  B The total number of atoms of A changes from N A,i to N A,f after some time t : N A,f = N A,i e - t N A,f = 1/2 = e - 1/2 N A,i ln 2  =  1/2  1/2 is the half-life, and is the decay constant

Radioactive Dating Isotope A decays into isotope B A  B The total number of atoms of A and B remain the same. N A,i + N B,i = N A,f + N B,f N A,f = N A,i e - t N B,f = ( e t - 1 ) N A,f + N B,i We can measure N A,f and N B,f but not N B,i We also do not know if N A,i was uniform in the rock. Therefore, measure stable isotope C that is chemically identical to B, and work with isotope ratios. N C,f = N C,i = N C

Ra dioactive Dating N B,f / N C = ( e t - 1 ) ( N A,f / N C ) + ( N B,i / N C ) Example: A = 87 Rb, B = 87 Sr, C = 86 Sr Half-life = 47.5 Gyr = ln 2 / 47.5  10 9 =  yr -1 Slope = = e t - 1 => t = 4.39  10 9 yr

The Formation of the Moon Fission model (daughter model) Earth was spinning too fast and part of it was torn off to form the Moon. BUT, spin axes are not aligned, no water on the Moon. Co-creation model (sister model) Moon formed at the same time, in an accretion disk around the Earth. BUT, lunar rocks had different compositions. Capture model (wife model) Moon was formed elsewhere, but was captured by Earth. BUT, compositions are too similar, and needs a third body to brake the Moon’s motion.

Collision Model (proposed by Hartmann and Davis, simulated by Cameron and Benz) An intruder ~ twice the mass of the present-day Mars collided with the Earth 4.6 Gyr ago. Explains: Moon’s lack of Fe, Similar O-isotope ratios Earth’s uncompressed mantle