ASTRONOMY 340FALL 200725 September 2007Class #6-#7

Review Physical basis of spectroscopy

Einstein A,B coefficients probabilities of transistions

Absorption/emission coefficients are functions of ρ, N, quantum mechanical factors, temperature

Molecular spectroscopy More available quantum states – rotational,

vibrational Low energy transitions IR, radio part of the

spectrum (hν << kT) Examples

CaI in the atmosphere of Mercury linewidth = Δλ = Δv (1/2)mv2 = (3/2)nkT

Quantum mechanics Principle quantum # (n) energy Angular momentum, l Spin, s Multi-electron atoms have many filled

orbitals (constrained by exclusion principle) e.g. electron with n=2 could have l=1 or l=0, and if its l=1 it could have s=1/2 or -1/2 many orbitals, many transitions, many spectral lines http://physlab2.nist.gov/PhysRefData/ASD/

lines_form.html

Molecules Nuclei act as single nucleus with

common potential Multiple nuclei generate other quantum

states Electronic Rotational Vibrational low energy radio/NIR part of

the spectrum Most surface and atmospheric

components are molecular

CO Main product of stellar evolution Transitions easily excited rotational

modes J = 1 0 (2.7mm, 115.3 GHz) J = 2 1 (1.3mm)

Observations radiotelescopes Measure “brightness temperature”, Tb Optically thick vs optically thin

Mars – non thermal CO

Example: Mercury What does the spectrum of Mercury look

like? Planetary reflectance spectrum Terrestrial emission and absorption Narrow source emission lines wavelength

shifted via Doppler Process

What do you actually measure? Linewidths? Wavelength?

Spencer et al. 2000Science 288, 1208

Io is the most geological activity of anything in solar system volcanoes discovered during Voyager flyby in ’79

What’s coming out of that volcano?

Spencer et al. 2000Science 288 1208 Use transit of Io across Jupiter to observe plumes from

volcanoes why? Scattered light dust scatters photons effectively so you

get a “non-thermal” continuum effect is to fill in absorption line

Identify S2 and SO2 lines in 240.0-300.0nm range -> fit linewidths T ~ 300 K N(SO2) ~ 7 x 1016 cm-2

N(S2) ~ 1 x 1016 cm-2

Pure SO2 suggests a lack of Fe since Fe will bind with SO2 if available

CO molecule C,O main products of stellar evolution,

particularly intermediate mass stars 3He 12C or 12C + 4He 16O On terrestrial planets CO comes from CO2 + uv

photons CO + O Transitions

J = principle rotational quantum number J=10 (2.7mm, 115.3 GHz) J=21 (1.3mm), J=32 (0.87mm) J=0 is ground state, but get to J=1 if there’s

ambient thermal bath with T~5.5K it’ll get excited to J=1 level

CO molecule Photons too dang weak for CCDs, so you

need a radio telescope Characterize intensity with a “brightness

temperature” if line is optically thick the observed brightness temperature really is the thermal temperature Tb = (λ2/2k)Bλ Rewrite radiative transfer as:

(dTb(s)/dτλ) = Tb(s) – T(s) Tb(s) = Tb(0)e-τ(s) + T(1-e-τ(s)) Tb = τT (τ << 1) Tb = T (τ >> 1)

Venus Images in J=1-0 Line Observations

2.7mm continuum, J=1-0 CO line 3-element interferometer

Continuum results 10% increase in Tb from day side to night side a

change in atmospheric conditions? CO line results

Line shape varies broad, shallow lines on dayside; deep, narrow lines on night side

Note on Conductivity Specific heat units are J mole-1 K-1

function of temperature for most minerals

Example: feldspar (KAlSi3O8)

Transition Slide…. Radiative transfer tells us how radiation

is affected travelling through some substance (gas)

In Rayleigh-Jeans approximation we can substitute a temperature (Tb) for the radiation intensity

Now onto some fun stuff – planetary surfaces….

Relevant reading: Chapter 5

Processes at Work Impact cratering Weathering/erosion Conditions of the atmosphere Geological activity

Volcanic activity Tectonics

Geological activity - Earth Volcanism

Shield volcanoes Formed via a single plume Hawaii – crustal plate moving over a hot spot

“cone” volcanoes Formed over subduction zones Cascade mountains, Mount Etna

Earthquakes At plate boundaries

Plate tectonics Mid-ocean ridges, mountain chains, moving

continents, earthquakes, “ring of fire”, global resurfacing

Apollo 17 View of Earth

Earth Topographic Map

Mercury Heavily cratered No volcanoes, no mountain chains, no

plate boundaries, no continents no recent tectonics

Shrinking? Weak magnetic field Conclusion: one plate planet with no

activity over the past several billion years; surface is shaped by impacts

Mercury, Mariner 10 3/74, 9/74, 3/75

Mercury South Pole

Mercury, Scarp displacement

Luna, near sideLUNA

Earth Facing Side The far side

Moon from Galileo Spacecraft

Apollo 14

Apollo 12

Apollo 15

Apollo 17

Apollo 11

Apollo 16

Lunar Highlands

Lunar Mare

Venus Lots of volcanic activity in the recent past

Characteristic feature is a “coronae” which is a circular structure like the caldera of a volcano but without the mountain to go with it

Global resurfacing about 300 Myr ago Crater density (number per km2) We call this a “young” surface

A couple of continent-like features No obvious plate boundaries

Venus Clouds Mariner 10

Venus Topography identified

Venus Surface, Venera 13

Sapas Mons

Maat Mons

Terrestrial Planet Surface Morphology (4)

• Mars

• Massive Shield Volcanoes• Huge Erosion Channels• Much Cratering, much eroded• Polar Caps

Mars Hubble

Mars Orbiter Laser Altimeter Topographic Map

Sojourner at Yogi Seeds Fig 23-15)

Vallis Marineris (Seeds Fig 23-17

Olympus Mons Viking 1

MOLA Generated Perspective of O.Mons

Vallis Marinaris

Fig 23-22a

Fig 23-23a

Fig 23-23b

Water in Newton Crater, Context

“Evidence” for recent liquid flow

Fig 23-24a

Famous Viking 1 Face

MGS view of the “Face”

Let’s put it all together…. Calculate the surface area to mass ratio

(km2 g-1) Moon: 5.16 10-19

Mercury: 2.26 10-19

Mars: 2.25 10-19

Venus: 9.46 10-20

Earth: 8.55 10-20