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EART160 Planetary Sciences. Francis Nimmo. Last Week. Planetary mass and radius give us bulk density Bulk density depends on both composition and size Larger planets have greater bulk densities because materials get denser at high pressures - PowerPoint PPT Presentation
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EART160 Planetary Sciences
Francis Nimmo
Last Week• Planetary mass and radius give us bulk density• Bulk density depends on both composition and size • Larger planets have greater bulk densities because
materials get denser at high pressures• The increase in density of a material is controlled by
its bulk modulus• Planets start out hot (due to accretion) and cool• Cooling is accomplished (usually) by either
conduction or convection• Vigour of convection is controlled by the Rayleigh
number, and increases as viscosity decreases• Viscosity is temperature-dependent, so planetary
temperatures tend to be self-regulating
Talk tomorrow• 4pm in NS101
• Matija Cuk, The lunar cataclysm
This Week - Atmospheres• What determines the surface temperature of a planet?• What determines the temperature and pressure
structure of planetary atmospheres?• What are the atmospheres made of, and where do
they come from?• What determines the wind strengths?• How do planetary atmospheres evolve?
Surface Temperature (1)
22)1( rr
EinEFRAE 2 44radE R T
4/12
4
)1(
AF
r
rT EE
eq
• What determines a planet’s surface temperature?
Incident energy
Reflectedenergy Energy re-radiated
from warm surface
Absorbed energywarms surface
Sun
• Balancing energy in and energy out gives:
R
A is albedo, FE is solar flux at Earth’s surface, rE is distance of Earth to Sun, r is distance of planet to Sun, is emissivity, is Stefan’s constant (5.67x10-8 Wm-2K-4)
Surface Temperature (2)• Solar constant FE=1300 Wm-2
• Earth (Bond) albedo A=0.29, =0.9• Equilibrium temperature = 263 K• How reasonable is this value?
• How to explain the discrepancies?• Has the Sun’s energy stayed constant with time?
4/12
4
)1(
AF
r
rT EE
eq
Body Mercury Venus Earth Mars
A 0.12 0.75 0.29 0.16
Teq 446 238 263 216
Actual T 100-725 733 288 222
is Stefan’s constant5.67x10-8 in SI units
Greenhouse effect• Atmosphere is more or less transparent to radiation
(photons) depending on wavelength – opacity• Opacity is low at visible wavelengths, high at infra-red
wavelengths due to absorbers like water vapour, CO2
• Incoming light (visible) passes through atmosphere with little absorption
• Outgoing light is infra-red (surface temperature is lower) and is absorbed by atmosphere
• So atmosphere heats up• Venus suffered from a runaway greenhouse effect –
surface temperature got so high that carbonates in the crust dissociated to CO2 . . .
Albedo effects• Fraction of energy reflected (not absorbed) by surface
is given by the albedo A (0<A<1)• Coal dust has a low albedo, ice a high one• The albedo can have an important effect on surface
temperature• E.g. ice caps grow, albedo increases, more heat is
reflected, surface temperature drops, ice caps grow further . . . runaway effect!
• This mechanism is thought to have led to the Proterozoic Snowball Earth
• How did the Snowball disappear?• How did life survive?• How might clouds affect planetary albedo?
Atmospheric Structure (1)• Atmosphere is hydrostatic:• Gas law gives us:
• Combining these two (and neglecting latent heat):
)()( zgzdzdP
RT
gP
dz
dP
Here R is the gas constant, is the mass of one mole, and RT/gis the scale height of the (isothermal) atmosphere (~10 km) which tells you how rapidly pressure increases with depth
RT
P
• Result is that pressure decreases exponentially as a function of height (if the temperature stays constant)
Scale Heights• The scale height tells you how far upwards the
atmosphere extends• Scale height H = RT/g. Does this make physical sense?
• Total column mass (per unit area) = 0H=P0/g (where’s this from?)
• It turns out that most planets have similar scale heights:
Venus Earth Mars Jupiter Saturn Uranus Neptune
Tsurf (K) 733 288 215 165* 135* 76* 72*
Albedo 0.75 0.29 0.16 0.34 0.34 0.29 0.31
H (km) 16 8.5 18 18 35 20 19
* Temperature measured at 1bar pressure
Atmospheric Structure (2)• Of course, temperature actually does vary with height• If a packet of gas rises rapidly (adiabatic), then it will
expand and, as a result, cool• Work done in expanding = work done in cooling
pC dT
pdzdT
C
g
VdP dP
• Combining these two equations with hydrostatic equilibrium, we get the dry adiabatic lapse rate:
Cp is the specific heat capacityof the gas at constant pressure
is the mass of one mole, isthe density of the gas
• On Earth, the lapse rate is about 10 K/km• What happens if the air is wet?
Atmospheric Structure (3)
Temperature (schematic)
tropopause
troposphere
stratosphere
mesosphereradiation
adiabat
clouds
Measured Martian temperature profiles
Lapse rateappx. 1.6 K/km – why?
• Lower atmosphere (opaque) is dominantly heated from below and will be conductive or convective (adiabatic)
• Upper atmosphere intercepts solar radiation and re-radiates it
• There will be a temperature minimum where radiative cooling is most efficient (the tropopause)
Giant planet atmospheric structure
• Note position and order of cloud decks
Atmospheric dynamics• Coriolis effect – objects moving on a
rotating planet get deflected (e.g. cyclones)• Why? Angular momentum – as an object
moves further away from the pole, r increases, so to conserve angular momentum decreases (it moves backwards relative to the rotation rate)
• Coriolis acceleration = 2v sin()• How important is the Coriolis effect?
is latitude
v
L sin2 is a measure of its importance (Rossby number)
e.g. Jupiter v~100 m/s, L~10,000km we get ~30 so important
Deflection to rightin N hemisphere
Hadley Cells• Coriolis effect is complicated by fact that parcels of
atmosphere rise and fall due to buoyancy (equator is hotter than the poles)High altitude winds
Surface winds • The result is that the atmosphere is broken up into several Hadley cells (see diagram)
• How many cells depends on the Rossby number (i.e. rotation rate)
Slow rotator e.g. Venus Medium rotator e.g. Earth Fast rotator e.g. Jupiter
Ro~30Ro~4Ro~0.02(assumes v=100 m/s)
Zonal Winds
• The reason Jupiter, Saturn, Uranus and Neptune have bands is because of rapid rotations (periods ~ 10 hrs)
• The winds in each band can be measured by following individual objects (e.g. clouds)
• Winds alternate between prograde (eastwards) and retrograde (westwards)
Geostrophic balance• In some situations, the only significant forces acting are
due to the Coriolis effect and due to pressure gradients
• The acceleration due to pressure gradients is
• The Coriolis acceleration is 2 v sin(Which direction?)
• In steady-state these balance, giving:
x
P
1
Why?
x
Pv
sin2
1
Does this make sense?
• The result is that winds flow along isobars and will form cyclones or anti-cyclones
• What are wind speeds on Earth?
L L
Hisobars
pressure
Coriolis
wind
Where do planetary atmospheres come from?
• Three primary sources– Primordial (solar nebula)– Outgassing (trapped gases)– Later delivery (mostly comets)
• How can we distinguish these?– Solar nebula composition well known– Noble gases are useful because they don’t react– Isotopic ratios are useful because they may
indicate gas loss or source regions (e.g. D/H)– 40Ar (40K decay product) is a tracer of outgassing
Atmospheric Compositions
Isotopes are useful for inferring outgassing and atmos. loss
Earth Venus Mars TitanPressure 1 bar 92 bar 0.006 bar 1.5 barN2 77% 3.5% 2.7% 98.4%
O2 21% - - -
H2O 1% 0.01% 0.006% -
Ar 0.93% 0.007% 1.6% 0.004%
CO2 0.035% 96% 95% ~1ppb
CH4 1.7ppm - ? 1.6%40Ar 6.6x1016 kg 1.4x1016 kg 4.5x1014 kg 3.5x1014 kg
H/D 3000 63 1100 360014N/15N 272 273 170 183
Not primordial!• Terrestrial planet atmospheres are not primordial
(How do we know?)• Why not?
– Gas loss (due to impacts, rock reactions or Jeans escape)
– Chemical processing (e.g. photolysis, rock reactions)
– Later additions (e.g. comets, asteroids)
• Giant planet atmospheres are close to primordial:
Solar Jupiter Saturn Uranus Neptune
H2 84 86.4 97 83 79
He 16 13.6 3 15 18
CH4 0.07 0.2 0.2 2 3
Valuesare by number of molecules
Why is the H/He ratio not constant?
Atmospheric Loss• Atmospheres can lose atoms from stratosphere,
especially low-mass ones, because they exceed the escape velocity (Jeans escape)
• Escape velocity ve= (2 g R)1/2 (where’s this from?)• Mean molecular velocity vm= (2kT/m)1/2
• Boltzmann distribution – negligible numbers of atoms with velocities > 3 x vm
• Molecular hydrogen, 900 K, 3 x vm= 11.8 km/s• Jupiter ve=60 km/s, Earth ve=11 km/s• H cannot escape gas giants like Jupiter, but is easily
lost from lower-mass bodies like Earth or Mars• A consequence of Jeans escape is isotopic fractionation
– heavier isotopes will be preferentially enriched
Atmospheric Evolution• Earth atmosphere originally CO2-rich, oxygen-free
• How do we know?
• CO2 was progressively transferred into rocks by the Urey reaction (takes place in presence of water):
3 2 3 2MgSiO CO MgCO SiO • Rise of oxygen began ~2 Gyr ago (photosynthesis &
photodissociation)• Venus never underwent similar evolution because no
free water present (greenhouse effect, too hot)
• Venus and Earth have ~ same total CO2 abundance
• Urey reaction may have occurred on Mars (water present early on), but very little carbonate detected
Summary• Surface temperature depends on solar distance,
albedo, atmosphere (greenhouse effect)• Scale height and lapse rate are controlled by bulk
properties of atmosphere (and gravity)• Terrestrial planetary atmospheres are not primordial –
affected by loss and outgassing• Coriolis effect organizes circulation into “cells” and
is responsible for bands seen on giant planets• Isotopic fractionation is a good signal of atmospheric
loss due to Jeans escape• Significant volatile quantities may be present in the
interiors of terrestrial planets
Key Concepts• Albedo and opacity• Greenhouse effect• Snowball Earth• Scale height• Lapse rate• Tropopause• Coriolis effect• Hadley cell• Geostrophic balance• Jeans escape• Urey reaction• Outgassing
H = RT/g
2 v sin()
Thermal tides• These are winds which can blow from the hot (sunlit)
to the cold (shadowed) side of a planet
Extrasolar planet (“hot Jupiter”)
Solar energy added =
Atmospheric heat capacity =Where’s this from?
So the temp. change relative to background temperature
t=rotation period, R=planet radius, r=distance (AU)
Small for Venus (0.4%), large for Mars (38%)
tr
FAR E
22 )1(
4R2CpP/g
trPTC
gFA
T
T
p
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