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Titan: an overview Basic facts • Motivation Radiative transfer • Photochemistry • Dynamics What do we see, and can we explain it? Titan’s possible future

Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

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Page 1: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Titan: an overview• Basic facts

• Motivation

• Radiative transfer

• Photochemistry

• Dynamics

• What do we see, and can we explain it?

• Titan’s possible future

Page 2: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future
Page 3: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Basic Titan facts I• Moon of Saturn, and second largest moon in solar

system (size is between Mercury and Mars)

• Slowly rotating (cf Venus), 1day ~ 16 Earth days

• Is also orbit time since Titan is tidally locked (cf our moon) => always has same side to Saturn

• ~ 674 Titan days per Titan year => ~ 29.5 Earth years per Titan year

• Inclined at 26.7° to the Sun (cf Earth’s ~23°) => Titan experiences seasons

Page 4: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Large moons and small planets Titan is the only one to have a significant atmosphere – probably it was big and cold

enough to retain ammonia when the solar system formed (as ammonia hydrate ices).

Titan is sufficiently cold that the nitrogen released to form the present atmosphere doesn’t suffer rapid Jeans escape.

Page 5: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Basic Titan facts II• ~ 95% N2 (cf Earth)

• Psurf ~ 1.5 Bar (~ 1.5 x Earth)

• Tsurf ~ 90K (Earth ~ 288K)

• ~ 4%CH4 – close to saturation, possibly supersaturated => CH4 ‘hydrological’ cycle (cf H2O on Earth)

• Photochemistry is important (cf Earth, Venus)

• CH4 is a ‘greenhouse gas’ (cf Earth) • Stratospheric haze absorbs solar energy (cf O3 in Earth’s

stratosphere) and creates ‘anti-greenhouse’ effect

Page 6: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Titan’s atmosphere

NB – 1D radiative transfer codes are able to produce matching temperature profiles by including what we know about Titan’s composition

Page 7: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Why the interest?1. All the similarities and

parallels with Earth2. Link into planetary

evolution3. Cassini/Huygens

mission

Cassini should reach Saturn on July 1st 2004, Huygens due to be released December 25th this 2004, entering Titan’s atmosphere January 14th 2005.

Page 8: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Why the interest?

1. All the similarities and parallels with Earth

2. Link into planetary evolution

3. Cassini/Huygens mission

Cassini should reach Saturn on July 1st 2004, Huygens due to be released December 25th this 2004, entering Titan’s atmosphere January 14th 2005.

Page 9: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

The Cassini mission

• Cassini’s Saturn tour involves 44 close flybys of Titan• Instruments used to examine Titan’s atmosphere and

surface include cameras; ir, vis and uv mappers; radio science; and radar

Page 10: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

The Huygens probe

• Huygens will take 2½ hours to descend through atmosphere• Instruments include those to measure atmospheric structure

during descent; surface imagers; spectral radiometers; solar sensors (giving aerosol data); in situ composition analysers; surface science package

Page 11: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Titan’s atmospheric structure

• Present understanding comes largely from Voyager observations

• Cassini’s 4 year + mission will only cover one Titan season, but will still greatly increase temporal and spatial coverage

• Voyager and Earth-based spectra indicate composition, important for explaining atmospheric T structure and past evolution

Page 12: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Radiative transfer on Titan I

• In lower atmosphere, ‘greenhouse’ effect due to collision-induced absorption of thermal radiation (H2-H2, N2-CH4, etc.) and absorption in vibration-rotation bands of gases with permanent dipole moments (e.g. CH4)

• In upper atmosphere, ‘anti-greenhouse’ effect due to absorption of incoming solar radiation by haze particles

• UV (<400nm): Rayleigh scattering plus haze absorption

• VISIBLE (400-700nm): haze absorption (hides surface from human eyes)

Page 13: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Radiative transfer on Titan II

• IR (>750nm; <13,000cm¯¹): haze scattering plus strong CH4 absorption bands with windows to the surface between them

• Also see many emission features (see above) from species present in stratosphere (where T increases with height)

Page 14: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

The Yung et al. photochemical model CH4 = methane C2H2 = acetylene

C2H6 = ethane C2H4 = ethylene

C3H8 = propane C4H2 = diacetylene

CH3C2H = methylacetylene

Page 15: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Photochemistry, Titan’s haze and CH4 loss• Photodissociation products of N2 & CH4 recombine, form larger

molecules which condense to form haze• Sufficiently large particles will fall out• May act as nucleation sites for CH4 condensate

• Some will be ‘refractory’ => oily/solid substances which won’t re-evaporate => net loss of CH4

• Requires mechanism to replace CH4, or total removal estimated in tens of millions of years

• This is significant, as the haze and most trace species are derived from CH4

• Surface oceans of C2H6-CH4 suggested as source and sink of CH4 cycle, but incompatible with high radar reflectivity and evidence of surface features

• Alternatives include outgassing from interior or methane clathrates

Page 16: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

The meridional circulation• A solution with no meridional flow, and radiative equilibrium

surface temperatures everywhere, exists for frictionless flow• However, friction requires a meridional flow (a ‘Hadley’ cell or

cells) to exist within some region about the equator, with the v=0, radiative equilibrium regime allowed at higher latitudes

• Held and Hou’s model gives the latitude at which the solutions intersect (the latitude to which the Hadley cell extends):

φH = (5/3 x g H ΔH)½ / Ωa,

(where H=tropopause height, ΔH=fractional drop in potential temperature between equator and poles, Ω=rotation rate and a=radius)

• => as Ωa decreases, Hadley cells extend further polewards

• => a nearly pole to pole Hadley cell exists around solstice

Page 17: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Equatorial superrotation

EQNP

•(wind speeds faster than surface speed) expected away

from equator when conserving angular momentum (e.g.

zonal jet in winter hemisphere)

•Superrotation at equator requires mechanism to deposit momentum here

•Gierasch mechanism found to be plausible in General

Circulation Models

Page 18: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Limb brightening and the ‘smile’

Page 19: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Titan’s surface

• The bright features (seen in gaps between near IR CH4

absorption bands) are thought to be regions of high IR albedo on the surface

• The dark regions may correspond to hydrocarbon oceans

Page 20: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Features strongly linked to dynamics

1. North-south albedo asymmetry: due to transport of haze to winter hemisphere by Hadley circulation. => darker in UV and visible (more haze absorption), brighter in IR (little absorption; mostly scattering). As expected, is observed to reverse every ~15 years

2. Polar hood: during polar night, chemical species normally destroyed by photolysis build up, and temperatures fall, encouraging these and other species to condense

3. The detached haze layer: this has recently been produced in general circulation models:

Page 21: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

Simulation of the detached haze layer

From Rannou, Hourdin and McKay, Nature 2002

• Haze production occurs at the highest altitudes shown• Away from equinox, the Hadley circulation transports haze

down in altitude over the winter pole (here the north• Haze is then spread out at this altitude and below, producing

the main haze layer

Page 22: Titan: an overview Basic facts Motivation Radiative transfer Photochemistry Dynamics What do we see, and can we explain it? Titan’s possible future

The possible future of Titan• If CH4 did eventually run out, then the ‘greenhouse’

effect would be reduced (=> Tsurf↓)• But CH4 is the basic ingredient required for the haze,

hence the ‘anti-greenhouse’ effect would also be reduced (=> Tsurf↑)

• However, less haze would also mean less heating in the stratosphere (=> Tstrat↓)

• Plus no CH4 would mean no more H2 to balance that escaping to space, and H2 is also an important greenhouse gas (=> Tsurf↓)

• Lower temperatures overall would eventually lead to N2 condensation, => Psurf ↓ => atmospheric collapse