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Astronomy 340 Astronomy 340

Astronomy 340 - PowerPoint Presentation

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Astronomy 340 - PPT Presentation

Fall 2007 4 October 2007 Class 10 Review Venus resurfacing events 300500 Myr ago Just how do you determine the age of a planetary surface Impacts Mars Martian Crustal Magnetization ID: 591946

impact abundant surface silicates abundant impact silicates surface craters velocity minerals shock metals rocks solid earth common sio crust

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Slide1

Astronomy 340Fall 2007

4 October

2007

Class

#10Slide2

Review

Venus resurfacing event(s) 300-500

Myr

ago

Just how do you determine the age of a planetary surface?

Impacts

MarsSlide3

Martian Crustal Magnetization

Working model

Collection of strips 200 km wide, 30 km deep

Variation in polarization every few 100 km

3-5 reversals every 10

6

years (like seafloor spreading on Earth)

Some evidence for plate tectonics…but crust is rigid

Earth’s crust appears to be the only one that participates in convectionSlide4

Formation of Impact Craters

Impactor unperturbed by atmosphere

Impact velocity ~ escape velocity (11 km s

-1

)

 tens of meters in diameter

Impact velocity > speed of sound in rocks

 impact forms a shock

Pressures ~100 times stress levels of rock

 impact vaporizes rocks

Shock velocity ~10 km s

-1

 much faster than local sound speed so shock imparts kinetic energy into vaporized rockSlide5

Contact/Compression

Projectile stops 1-2 diameters into surface

 kinetic energy goes into shock wave  tremendous pressures  P ~ (1/2)

ρ

0

v

2

Peak shock pressures ~1000 kbar; pressure of vaporization ~600 kbar

Shock loses energy

Radial dilution (1/r

2

)

Heating/deformation of surface layer

Velocity drops to local sound speed – seismic wave transmitted through surface

Can get melting at impact point

Shock wave reflected back through projectile and it also gets vaporized

Total time ~ few secondsSlide6

Excavation

Shock wave imparts kinetic energy into vaporized debris

 excavation of both projectile and impact zone (defined as radius at which shock

velocty

~ sound speed (meters per second)

Timescale is just a dynamical/crossing time (t = (D/g)

1/2

Crater size? D goes as E

1/3

 empirically, it looks like ~ 10

times

diameter of projectile (but see equation 5.26b).

Can get secondary craters from debris blown out by initial impact

Large impacts

multiring

basins (Mars, Mercury, Moon)Slide7

Craters

35m

2m

4yr

Small Earthquake

1km

50m

1600yr

Barringer Meteor Crater

7km

350m

51,000yr

9.6 mag earthquake

10km

500m

10

5

yr

Sweden

200km

10km

150 Myr

Largest craters/KT impactorSlide8

Crater Density

See Figure 5.31 in your book

 number of craters km

-2

vs diameter

Saturation equilibrium – so many craters you just can’t tell….

Much of the lunar surface

Almost all of Mercury

Only Martian uplands

Venus, Earth not even close  note cut-off on Venus’ distribution

Calibrate with lunar surface rocks

10

7

times more small craters (100m) as there are large craters (500-1000 km)Slide9

Mercury South PoleSlide10

Lavinia Planum Impact Craters

Note ejecta surrounding craterSlide11
Slide12

“It’s the size of Texas, Mr. President” - from yet another bad movie

Comets – small,rocky/icy things

 10s of km

Asteroids – small, rocky things

 a few to 10s of km  the largest is the size of Texas (1000 km)

100-300 NEAs known

Close encounters….

Tunguska River in Siberia  30-50m meteroid exploded above ground  flattened huge swath of forestSlide13

You make the catastrophe…

Need high velocity

max velocity ~ 70 km s

-1

(combine Earth’s orbital velocity plus solar system escape velocity)

Earth-asteroid encounters

 25 km s

-1

Eart-comet encounters  60 km s

-1

Make it big….

E ~ mv

2

 something 1000 km would wipe out the entire western hemisphere, but let’s be realistic and go for ~10m (10

21

J) or ~1 km (10

23

J)

One impact imparts more energy in a few seconds than the Earth releases in a year via volcanism etc.Slide14

Surface Composition

Reflection

spectroscopy

. (remember

radiative

transfer!)

What is the surface made of? Rocks, mostly igneous

Minerals = solid chemical compounds with specific atomic structureSlide15

Common Minerals

Silicates

Si is produced via He-burning in stellar interiors, released via SNe.

O is produced in massive and intermediate mass stars

Si, O bind easily

 SiO

4

, SiO

3

bind with lots of other things (Mg, Al, Fe) and form a solid at high temperature

SiO

2

= quartz

(Fe,Mg)

2

SiO

4

= olivine (most common)

CaAl

2

Si

2

O

8

= feldspar

 60% of surface rocks on Earth

Various Oxides

Fe

2

O

3

= hematite

 generally formed from a reaction between Fe, O, and H

2

O  has been found in Martian samplesSlide16

Common Minerals

Silicon

3

rd

most abundant element (after O, Fe)

Cosmically as abundant as Fe, Mg

Less abundant than C,N,O

Chemically between metals and non-metals

Can survive as solid in interstellar/circumstellar environmentSlide17

Common Minerals

Silicon

3

rd

most abundant element (after O, Fe)

Cosmically as abundant as Fe, Mg

Less abundant than C,N,O

Chemically between metals and non-metals

Can survive as solid in interstellar/

circumstellar

environment

Silicates

lithophiles

” = silicates and things that tend to attach themselves to silicates

 low density minerals, reside in the crustSlide18

Common Minerals

Silicon

3

rd

most abundant element (after O, Fe)

Cosmically as abundant as Fe, Mg

Less abundant than C,N,O

Chemically between metals and non-metals

Can survive as solid in interstellar/

circumstellar

environment

Silicates

lithophiles

” = silicates and things that tend to attach themselves to silicates

 low density minerals, reside in the crust

Igneous rocks

40-75% SiO

2

O:Si ratio is high at high temperature crystallization and you get more olivine; low at low T and you get more quartzSlide19

Common Minerals

Silicon

3

rd

most abundant element (after O, Fe)

Cosmically as abundant as Fe, Mg

Less abundant than C,N,O

Chemically between metals and non-metals

Can survive as solid in interstellar/

circumstellar

environment

Silicates

lithophiles

” = silicates and things that tend to attach themselves to silicates

 low density minerals, reside in the crust

Igneous rocks

40-75% SiO

2

O:Si ratio is high at high temperature crystallization and you get more olivine; low at low T and you get more quartz

Differentiation

 absence of “

siderophiles

” in crust is evidence of differentiationSlide20

Tectonics  What Separates the Earth from Others

Convection

 means of transporting heat  driven by internal heat (radioactive decay?)

Crustal plates are cold upper lid on convective cells  “subsolidus” convection in mantle (3000 km thick)

Consequences

Volcanic activity, mountain chains

Mid-ocean ridges

Continental drift, earthquakesSlide21

Tectonics

1

st

evidence

 mapping magnetic field in Indian Ocean floor  detection of distinct linear features interpreted as “sea-floor spreading”

Puzzle-piece like nature of continents

Youngest rocks near mid-ocean ridgesSlide22

Earth Topographic MapSlide23

Dating: Radionuclide Chronometry

Processes (

Most Important Cases

)

40

K

40

Ar

t

½

= 1.4 x 10

9

yrs

87

Rb 

87

Sr

t

½

= 6 x10

10

yrs

238

U 

206

Pb

t

½

= 5 x 10

9

yrs

Lunar Results

Oldest Highland Anorthosite

t

solid.

= 4.2 x 10

9

yrs

Youngest Mare Basalts

t

solid.

= 3.1 x 10

9

yrs

Terrestrial ResultsSlide24

Radioactive Decay

Consider a number density, n, of atoms

Which decays at an average rate,

l

The solution to which is:

Now n = ½ n

0

at time t =

t

1/2

so

Or,

And finally: