Title: Radiation from Solar System Objects
1Radiation from Solar System Objects
2Types of observation
- Photometry estimating sizes of unresolved
objects and scattering properties of their
surface material - Thermal radiometry sounding the near-surface
temperature distribution - Spectrophotometry identifying minerals or
chemical compounds via their absorption/emission
features - Radar estimating surface roughness and
composition constructing 3D size/shape models of
visually unresolved objects
3Observing Geometry
- External planet outside the Earths orbit
- - example Mars
- Internal planet inside the Earths orbit
- - example Venus
- Elongation angle S-E-P
- Phase angle angle S-P-E
Sun
Earth
Planet
4Phases
- Opposition E ? (external planets)
- Conjunction E 0 (all planets)
- Quadrature (external planets) E ? ?/2 and
- Max. elongation (internal planets) ? ?/2 and
Phases of Venus
5Elongations Phase Angles
6Bond Albedo
- Albedo whiteness
- R specularly reflected flux
- S scattered flux in all directions
- I? solar energy flux
AB fraction not absorbed 1-ABabsorbed fraction
7Phase Function
- Ratio between the flux scattered at phase angle ?
and the backscattered flux with ?0 - Phase integral
8Geometric Albedo
- Backscattered flux Fb
- Incident solar flux Fsun
- - AB is omnidirectional, Ap is unidirectional
- - AB is frequency averaged, Ap refers to a
photometric passband - - AB is theoretical, Ap is observational
9The Lambert Disk
- Non-absorbing isotropic scatterer with f(?)
cos? - Same surface brightness from all directions
(?lt?/2) - q 1
- Ap AB 1
- Ap is the amount of backscattered sunlight
relative to a Lambert disk with the same area
10Geometric Albedos, Phase Integrals
11Observed Magnitudes
- If S is the solar flux at the Earth in a certain
passband, the flux leaving an object toward the
Earth is - If R is the radius of the object, the flux
observed at the Earth is - In magnitude units
- where and
12Colours
- The magnitudes m are usually measured with
different broadband filters (U, B, V, R, etc.) - The differences, e.g. BV, are called colour
indices - From the magnitude formula for a Solar System
object, we get - Thus the measured colour index depends on
- the solar colour (BV)?
- the albedo ratio Ap(B)/Ap(V)
(true colour) - the phase reddening ?B(?)?V(?)
13Phase Curves
Photometry ? R2Ap Size-albedo ambiguity
- At small ?, a linear formula is often used as
phase curve - Opposition effect spike in brightness at very
small ? for atmosphereless objects
14Opposition Effect in Saturns A Ring
- Cause of the brightness spike at opposition
- - Lack of shadowing
- - Coherent backscatter
Cassini image
15Light scattering from grains (1)
- Examples the zodiacal light, dust tails in
comets, etc. - Observed brightness collective amount of
scattered sunlight from all grains along the line
of sight - The grain size distribution is important for
interpreting the observations - - for grains of radius a, the surface/volume
ratio is ? a-1
16Light scattering from grains (2)
- Large grains or boulders scatter light like
planets without atmospheres backscattering - Very small grains (?) are much more forward
scattering
Jupiters rings seen against the Sun
17Temperature radiometry (1)
- Incident energy flux (insolation) depends on the
distance to the Sun and the solar elevation angle - Insolation Scattering Thermal radiation
Heat conduction - The scattering efficiency is measured by AB
- Thermal emissivity ?IR
- - Is ?IR 1-AB? No, ?IR?0.9 is assumed in
general
18Planetary spectra
- Common planetary minerals have spectral features
in the IR - - e.g. stretching of bonds within molecules
- - local variation of emissivity
- Important for chemical analysis and thermal
modelling
Infrared spectrum of Mercury
Jupiters spectrum
19Temperature radiometry (2)
- Emitted flux of thermal radiation from the
Stefan-Boltzmann radiation law - Assume isothermal, spherical object!
- Absorbed insolation per unit time
- Emitted radiation per unit time
- Equilibrium temperature for thermal balance
20Bond albedos Eq. temperatures
21Radar observations (1)
- Send a radio pulse toward the object receive and
analyze the echo - Two main variables Delay and Doppler shift
- Received intensity I(?t,??)
- Find a model of the objects size, shape and spin
that represents I(?t,??)
22Radar observations (2)
- Echo frequency range
- Noise level for integration time ?t
- Received signal
- Signal/Noise ratio
Toutatis, small near-Earth asteroid
Kleopatra, large main-belt asteroid