Title: Planetsystemets fysik MN1
1Planetsystemets fysik MN1
- General inventory list
- The Sun, heliosphere
- 8 major planets
- Natural satellites, ring systems, magnetospheres
- Minor planets (asteroids, Trojans, NEOs, TNOs,
scattered disk) - Comets
- Meteorides
- Dust
2Relative sizes and colors of the planets
3Planetary physical properties
4Properties of solar system objects
- Quantities derivable from observations (Earth
based or in situ) - Orbit
- Mass
- Size
- Rotation state and direction
- Shape
- Temperature
- Magnetic field
- Surface composition
- Surface structure
- Atmospheric structure and composition
-
- Observations are used to constrain planetary
properties such as bulk composition and interior
structure
5Orbits
- Determined from
- Observations of astrometric positions
- 3 observations required
- In the 2-body problem, the orbit is described by
- Keplers and Newtons laws
- Six orbital elements
- a, semimajor axis
- i, inclination
- e, eccentricity
- ?, longitude of ascending node
- ?, argument of perihelion
- T, time of perihelion passage
Q a(1e)
Q a(1-e)
6Keplers laws
- All planets move along elliptical paths with the
Sun at one focus - The heliocentric distance rs is given by
- rs a(1-e2)/ (1e cos f)
- where a semimajor axis, e eccentricity, f true
anomaly (angle between perihelion and
instantaneous position), - e (1 - bm2/a2)1/2,
where 2bm b - A line segment connecting any given planet and
the Sun sweeps out an area at a constant rate due
to conservation of angular momentum, - dA/dt constant
- The square of a planets orbital period about the
Sun is proportional to the cube of the semimajor
axis - P2 4p2 a3 / G (m1 m2)
- where P period of the orbit, m1 mass of central
object, m2 mass of planet, G gravitational
constant
7Mass
- The mass of an object can be derived from
the gravitational force it exerts on other bodies - Orbits of satellites (Kepler III)
- P2 4p2a3/G(m1m2),
- m1m2 is solved for from observed orbit (P and
a), assuming m1gtgtm2 - Perturbations (for objects without satellites)
- short-term (close encounters)
- long-term (objects locked in stable orbital
resonances) - Spacecraft tracking data
- From Doppler shift of transmitted radio signal
- Resonant action on rings (amplitude of spiral
density waves or wakes) - Non-gravitational forces (comets)
8Rotation
- Movement of markings on resolved disk
- Useful for planets with albedo features
- Atmospheric winds may cause period to vary with
time and latitude - Radio emission of core or magnetosphere
- Particles trapped in magnetic fields are
accelerated and emit radio waves - Periodicity observed is that of the core
- Light curve observations
- Total brightness as a function of time
- Due to variations in albedo or projected area
- Doppler shifts derived from radar or reflectance
spectra - Useful for resolved featureless bodies
- Gives period and direction of rotation axis
Great Red Spot longitude drift chart
Asteroid light curve
9Size
- Measurement of angular diameter (for resolved
objects) - knowledge of the orbit provides the distance
- Occultations (for unresolved objects)
- timing of a number of observed chords within
occultation zone - Radar echoes
- only for nearby objects radar echo signal
strength drops as 1/r4 - Lander and orbiter triangulation
- Radiometric method
- thermal emission spectrum observed
- size and albedo derived F(?)
F(Ap, ?, ?, Teff) - (size/albedo ambiguity in visible)
Occultation coords of asteroid Laetitia
Radar echo image of asteroid Toutatis
10Shape
- Direct imaging
- From ground or spacecraft
- Stellar occultation chords
- Radar echoes
- Light curve models
- Visible observations shape/albedo ambiguity
- Shape of central flash
- Observed when the center of a body with an
atmosphere passes in front of an occulted star
caused by focusing of light rays refracted by the
atmosphere
Asteroid shape model based on visible light curve
observations
11Temperature
- Energy balance between solar insolation and
thermal reradiation Fabsorbed Femitted - Complicated by
- Internal heat sources (e.g., Io, Jupiter)
- Diurnal, latitudinal and seasonal temperature
variations - Greenhouse effect, a temperature increase due to
an atmosphere or surface layer more transparent
at optical than thermal wavelengths - In-situ thermometer on lander
- Shape of thermal infrared spectrum
- Most solid and liquid planetary materials are
nearly perfect blackbody radiators with emission
peak at near to mid infrared wavelengths - Derived temperature may be a function of
wavelength due to - variation of temperatures on surface
(pole-equator variation, volcanic hot spots,
albedo variations, surface material variation of
emissivity) - opacity variations of an atmosphere, allowing
different altitudes to be probed
Infrared spectra and blackbody temperatures of
Mars, quartz, and the Earth
12Surface composition
- Reflectance spectrum
- Optical, IR windows from Earths surface
- UV from spacecraft
- Thermal (difficult to interpret)
- infrared spectra
- radio data
- Microwave radar reflectivity (from surface or
orbiting spacecraft) - electrical and thermal conductivity
- X-ray and ?-ray fluorescence (from orbiter or
lander) - Chemical analysis (in situ or on returned
samples) - Mass spectroscopy (in situ or on returned samples)
Near-infrared spectra of the Moon
Isotope abundance ratios on Mars
13Surface structure
- Large scales (gtcm)
- Imaging (at optical/IR/radio wavelengths)
- Single camera imaging
- Stereoscopic imaging
- Two angle geometry data resolves slope-albedo
ambiguity - Radar imaging
- Laser altimetry (spacecraft)
- Small scales (ltcm)
- Radar echo brightness
- High reflectance for size scales near radar
wavelength - Phase angle intensity observations
- Opposition effect
- Large phase angle brightness
14Atmospheric structure and composition
- Composition and structure (temperature-pressure
profile) may be derived from - spectral reflectance data at visible wavelengths
- thermal spectra and photometry and infrared and
radio wavelengths - Doppler shift of satellite signal during
occultation - phase shift due to atmospheric refraction
- density and temperature profile derived from
refractivity profile - attenuation of radio signals from surface landers
and atmospheric probes - in situ mass spectrometers
Mars temperature profile in S winter
Pressure profiles of the giant planets
atmospheres
15Magnetic fields
- The magnetic fields of the planets may be
approximated by dipoles, with higher order
perturbations to account for irregularities - Types of magnetic field
- generated by internal dynamo operating in a fluid
region (giant planets, Earth, Mercury) - induced by interaction between solar wind and
charged particles in ionosphere/atmosphere
(Venus, comets) - localized crustal magnetic fields due to remnant
ferromagnetism (Mars, Moon) - very small fields caused by interaction between
solar wind and conducting regions within the body
(e.g., asteroids) - Magnetic fields may be detected
- directly using an in situ magnetometer
- indirectly via
- effects of accelerating charges producing radio
emissions - presence of aurorae, caused by charged particle
precipitation in in a plöanets upper atmosphere
Jupiters synchrotron radiation at ? 20 cm
16Planetary interiors
- Interior not directly accessible to study, but
properties may be inferred from observable
parameters, indirect clues and constraints - Bulk composition
- meteorites studied in the laboratory
- observed size and mass, surface composition,
heliocentric distance, cosmogonic abundance
assumptions - material properties from laboratory data and
quantum mechanical calculations - Internal structure
- gravitational field and rotation rate degree of
concentration of mass - velocity and attenuation of seismic waves
measured by in situ seismometric network
density, rigidity and other physical properties,
which in turn depend on composition - surface structure (volcanism, plate tectonics),
energy output - magnetic field structure (dipole fields generated
near core, higher-order fields closer to surface) - free oscillation periods of gaseous planets
(similar to helioseismology)