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Astronomy 6570 Physics of the Planets Outer Planet Interiors

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Page 1: XVI Outer planet interiors 2018 - Cornell Universityhosting.astro.cornell.edu/...planet_interiors_2018.pdf · cNote: Earth has a magnetic field of opposite polarity to those of the

Astronomy6570

PhysicsofthePlanets

OuterPlanetInteriors

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GiantPlanets,CommonFeatures

Mass: 15– 317MRadius: 3.9– 11.2RDensity: 0.69– 1.67gcm-3

Rotationperiod: 9.9– 18hoursObliq.: 3° – 98°Vis.Surf.: clouds;zonallybanded(N?)

decreasingcontrast:Jè Sè UAtmos.Comp.: H2 +He(roughlysolar)

+CH4,NH3,H2O,…(enhanced)Atmos.Struct.: adiabaticbelow~1bar

warmstratospheresEnergyoutput: ~2*solarinput(exc.U)Atmos.Circ’n.: Zonalwindsof100– 400msMag.Field: 0.14– 4.2Gauss

tilt=0– 59°Satellites: inner,regularsats(e~i~0)

outer,irreg.satsRingsystem: increasingmass:Jè Nè Uè S

assoc.withsmallsatellitesephemeralstructures?

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Radio Occultation Temperature Profiles

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CondensationLevels

RadioSpectrum

T(°K)

P(bar)

Jupiter

λ

• Microwave emission originates from 0.5 – 10 bar levels

• NH3 absorption v. strong near 1 cm è minimum in TB.

TB(°K)

• Condensation levels correspond to predicted cloud layers

• Only uppermost clouds observed directly

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Planetary insolation patterns

• small obliquity (J)

• large obliquity (U)

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Emitted infrared flux and equivalent brightness temperatures versus latitude for the four outer planets. The radiation is emitted, on average, from the 0.3 to 0.5 bar pressure levels. The equator-to-pole temperature differences are small. The largest temperature gradients occur at the extrema of the zonal velocity profile. (Ingersoll, 1990)

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Zonalwindprofiles(Voyagerdata)

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Sanchez-Lavega (2005) Science 307, 1223.

System III (Voyager)SKR (Cassini)

Cassini ISS

HST (1994-2004)

Voyager ISS

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Internalcirculationmodels:Saturn

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Magnetic field comparison:

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ComparisonofplanetarymagneticfieldsEarth Jupitera Saturna Uranusa Neptunea

Radius,Rplanet (km) 6,373 71,398 60,330 25,559 24,764SpinPeriod(Hours) 24 9.9 10.7 17.2 16.1MagneticMoment/MEarth 1b 20,000 600 50 25SurfaceMagneticField(Gauss)

DipoleEquator,B0 0.31 4.2 0.22 0.23 0.14Minimum 0.24 3.2 0.18 0.08 0.1Maximum 0.68 14.3 0.84 0.96 0.9

DipoleTiltandSensec +11.3°

-9.6° -0.0° -59° -47°

Distance(A.U.) 1d 5.2 9.5 19 30SolarWindDensity(cm-3) 10 0.4 0.1 0.03 0.005RCF 8RE 30RJ 14RS 18RU 18RNSizeofMagnetosphere 11RE 50-100RJ 16- 22RS 18RU 23-26RNa Magnetic field characteristics from Acuna & Ness (1976), Connerney et al. (1982, 1987, 1991).b MEartth = 7.96 × 1025 Gauss cm3 = 7.906 × 1015 Tesla m3.c Note: Earth has a magnetic field of opposite polarity to those of the giant planets.d 1 A.U. = 1.5 × 108 km.

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PlanetaryInteriorModels(generalconsiderations)

Assume spherical symmetry (for simplicity only!)

1. Hydrostatic equilib.: dPdr = −ρg =

−Gm r( )ρr2

2. Mass conservation: dmdr = 4π r 2ρ

3. Equation of state: P = f ρ,T; composition( )

4. Heat transfer: k dT

dr = F! conduction

dTdr =

∂T∂P( )s dP

dr ! convection

%

&'

('

- in approximate treatments (4) may be dropped and (3) replaced by P = f ρ( )3 first-order D.E.'s ⇒ 3 boundary conditions

1. m 0( ) = 0

2. P R( ) = 0

3.T R( ) =Tsurf (solid surface)Teff (jovian planets)

%&'

('

Adjust model parameters (e.g., composition, Mcore, etc.) to fit observables:

M,R,J2 ~ CMR2( ),J4, etc.

Model ⇒ ρ r( ),P r( ), g r( ),T r( )

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Central pressures : dP

dr = −Gmρ

r 2

⇒ roughly Pc −P0

R ! 4π3

GM2

R5

∴ Pc !GM2

R4

Case I : a uniform-density planet:

m r( ) = 4π3 ρr 3 ⇒

g = 4π3 Gρr ⇒

dPdr = −

4π3( )Gρ2 r

∴ P r( ) = Pc −2π3 Gρ2 r 2

Boundary condition ⇒ Pc =2π3 Gρ2R2 = 3

8πGM2

R4

ρ (gcm-3)

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Case II : P = !ρ2 (n = 1 polytrope ~ Jupiter)

⇒Pc =2π 3

9 Gρ2R2 (see Polytrope notes)

Body ρ(gcm-3) R(km) CaseI CaseII(Mb=1011 Nm-2)

Moon 3.34 1738 0.047 0.155

Earth 5.52 6371 1.73 5.68

Uranus 1.32 25,600 1.60 5.25

Jupiter 1.33 71,400 12.6 41.4

Examples

Detailedmodels:Earth=3.5MbJupiter=70MbUranus=8Mb

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Adiabats

HYDROGEN

H-He

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Cassini gravity model (Iess 2018)

Constraints on heavy element content in Jupiter & Saturn.

(Guillot)

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Saturn

Jupiter

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2 3 4 5 6 7 8 9 10 11 12

DHgUHH

10-8

10-7

10-6

10-5

10-4

10-3

10-2

10-1

8nnoUm

DOizH

d Z

onDO H

DUm

onic

CoHff

iciH

ntV

(Jl)

8nifoUm UotDtion2bVHUvHd 9DOuH8ncHUtDinty

Saturn gravity harmonics (Cassini proximal orbits)

Iess, et al. (2108)

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-80 -60 -40 -20 0 20 40 60 80-200

0

200

400U

(m s

-1)

a

ObservedReconstructed

-80 -60 -40 -20 0 20 40 60 80Latitude

-200

0

200

400

U (m

s-1

)

b

ObservedDifferential RotationReconstructed

Observed and reconstructed zonal wind profiles for Saturn, based on Cassini gravity measurements. Dashed curve indicates a symmetric model with rotation on cylinders (Iess, et al. 2018).

Rotation on cylinders.

Winds decay with depth at ~9000 km.

Winds truncated at 60 deg latitude.

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GiantPlanetModels(Stephenson)

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HubbardandMacFarlane

“rock”

“ice”

gas

Density distribution in Uranus, calculated for a model with solar abundances of “ice”and “rock”. The temperature distribution corresponds to the present epoch.

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HubbardandMacFarlane

“rock”

“ice”

gas

Density distribution in Neptune, calculated for a model with solar abundances of “ice” and “rock”. The temperature distribution corresponds to the present epoch.