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53 Cards in this Set

  • Front
  • Back
Definition of Planet
Orbits around the sun



Enough Mass to Assume Hydrostatic Equilibrium (nearly round shape)




Clear the neighborhood (no other surrounding bodies same size except satellites or those under gravitational force of planet)

Definition of Dwarf Planet
Orbits around the sun



Enough Mass for Hydrostatic Equilibrium




DOES NOT clear he neighborhood

Possible Origins of Moons
1) Conformation: Formed along with the planet and out of the same material as the planet



Example: Jupiter's inner satellite




2) Fission/Collisional Ejection: Moon Breaks off from the original parent body. Can only happen if there is a collision with a very large object.




Example: earth's moon which came from a collision




3) Capture: gravitational field captures orbiting debris. Collide or missed collision with third party within gravitational reach of planet




Example: Captured Asteroids

Synchronous Orbits
the rotation of a body with a period equal to its orbital period; also called 1 to 1 spin orbit coupling



LOOK UP MORE ON TIDAL EFFECTS

Orbital Resonance
The resonance that occurs whenever the orbital periods of two objects are related by a ratio of small integers



Rhythmic gravitational interactions in an orbital resonance can have stabilizing or destabilizing effect

The Roche Limit
The smallest distance from a planet or other object at which a second object can be held together by purely gravitational force



Example: Ring particles

Asteroids (what they are made of)
Small objects with various mixtures of ice, rock and metal
Asteroids (where they are found)
Orbit the sun between Mars and Jupiter



Between 2 and 3.5 AU

Typical Size of Asteroids
Majority of asteroids are smaller than 1km across



700,000 to 1.7 Million are greater than 1km




200 are bigger than 100km




Pallas and Vesta are 500km




Ceres is 975km

Number of Asteroids
100,000
Kirkwood Gaps
Gaps in the spacing of asteroid orbits



MORE

Plutinos
100 objects in the Kuiper belt that orbit the Sun with nearly the same semimajor axis as Pluto
Edgeworthe-Kuiper Belt



(Location - Layout - Typical Objects)

30 to 50 AU




Orbits in or fairly close to the ecliptic plane. Objects tend to be larger




some are dwarf planets




70,000 objects greater than 100km



Oort Cloud



(Location - Layout - Typical Objects)

extends in 3 dimensions from the sun in a total distance of 50,000 AU



composed of chunks of ices with a total mass of about 40 ties that of Earth




Largest objects are only a few km across

What becomes of meteroids?
They burn up in the atmosphere or enter in the form of a meteorite
Comets
a small body of ice and dust in orbit around the sun. While passing near the sun, a comet's vaporized ices give rise to a coma and a tail
Comet tails
The gases burning off as the frozen ice moves closer to the sun
Photosphere
Thin Layer (300-500 km thick)



Surface from which visible light escapes




Temperature is 5800K but varies dropping to nearly 4400K near top




Continuous spectrum emission, but with some absorption near upper layers




Granulated (convection cells)




Periodic sunspot activity

Chromosphere
Thin layer, but several times thicker than photosphere (2000 km thick)



Temperature varies: 4500K-25000K




Very low density, Hot thin gas.




Red/Pink colored layer due to strong H emission line spectrum




Spicules - short lived spikes or jets of gas shooting up a few thousand km

Corona
Very diffuse and very large, outermost layer of sun



3000 to 10000km above photosphere




Irregular shape determined to some extent by solar magnetic field




Extremely high temperature (a few million degrees K)




Source of sun's UV and XRay emission




Sporadic holes that are believed to be corridors for the solar wind

Thermal Equilibrium
Temperature at each depth in sun's interior remains constant even though each depth has different temperature from the others
Hydrostatic Equilibrium
the balance between the weight of a layer in a star and the pressure that supports it



Forms spherical design

Helioseismology



And how that determines sun's composition

By measuring the oscillations of the sound waves generated through the sun, a better understanding of the interior's composition is created
Sunspots
Dark, irregular-shaped region on the photosphere of the sun



It only appears dark because of the contrast with the surrounding photosphere




Photosphere - Temperature of 5800 K and Sunspot is 4300K




They occur where photosphere's magnetic field is significantly stronger than that of surrounding photosphere




Traps solar plasma and keeps it cooler/darker




Come in groups/pairs with opposite polarity

Solar Cycle
Periodic change in sun's activity and appearance. Duration of 11 years
Sun's Source of Energy
Hydrogen Fusion into Helium



Thermonuclear Fusion

How long will sun shine
6 million more years
Thermonuclear Fusion
Requires very fast atoms, therefore very hot temperatures



Also requires very high density, which means high pressures




Can only occur in the interior core of sun and has been mimicked in thermonuclear weapons and for brief instants in plasma fusion rings

The solar neutrino problem
Discrepancy between theoretical predictions of Sun's neutrino output and actual measured value



Recent experiments shows that solar neutrinos change species while in flight between Earth and Sun (neutrino oscillation). These neutrinos were previously undetected due to technology

Why fusion is hard to start and maintain
Temperature is too hot
How distances to stars are measured
d = 1/parcsec



1 parc sec = 3.26 ly

parallax
the apparent displacement of an object due to the motion of an observer
parcsec
3.26 lightyears
light year (distance)
distance light travels in a year



MORE

Luminosity
the rate at which electromagnetic radiation is emitted from a star or other object
Luminosity connection to temperature and surface area



And thus to Sun's radius

brightness = Luminosity / 4 pi (d^2)
Inverse Square Law
the apparent brightness of a light source varies inversely with the square of the distance from the source




Principal Spectral Classes



Color, Temperature, Spectral Lines

O - Blue Violet - 30,000-50,000K - Ionized Atoms, helium



B - Blue Violet - 11,000-30,000K - Neutral helium, some hydrogen




A - White - 7500-11,000K - Strong hydrogen, some ionized metals




F - Yellow White - 5900-7500K - Hydrogen and ionized metals




G - Yellow - 5200-5900K - Both neutral and ionized metals, especially calcium




K - Orange - 3900-5200K - Neutral Metals




M - Red Orange - 2500-3900K - Strong titanium oxide and some neutral calcium




L - Red - 1300-2500K - Neutral potassium, rubidium, cesium and metal hydrides




T - Red - 700-1300K - Methane, strong neutral potassium and some water




Y - Red - Below 600K - Possibly ammonia

Spectroscopic Parallax
distance to a star derived by comparing its apparent brightness to a luminosity inferred from the star's spectrum
Role of binary stars in determining masses
Mass = Semimajor axis (AU) ^3 / Period (in years) ^2
Mass-Luminosity Relation
There is a precisely known mathematical relation between luminosity and mass.
Birth of stars from interstellar clouds
Gravitational force prevents hydrogen and helium atoms from flying away



The cloud begins to contract if cloud is big enough




Cloud heats up




Cloud falls into itself to compensate from energy radiated away due to being a black body




Contracts more and more and gets hotter and hotter

How low mass stars live and die
The whole star becomes depleted in hydrogen all at once



It will get hotter but no further fusion will occur




Becomes black dwarf

origin of planetary nebulae
The ejected outer envelope left over after helium shell burns and white dwarf formed
origin of white dwarfs
small but intense white-hot ember that is left over after the helium shell burns off
How high mass stars die
Core Collapse


Type 2 Super Novae


Synthesis of Elements
elements heavier than iron. Only phenomena in the universe that can create them.



Stable nuceli will stay and unstable will decay

origin of neutron stars
continued contraction and shrinks past the white dwarf region.



Carbon to Silicon and then Iron. But no energy can be gained from Iron.

Degeneracy Pressure
physical force that can withstand gravity



of electrons

Chandrasekhar Limits
Any white dwarf with mass less than 1.4 AU will stay white dwarf
What happens if Chandrasekhar Limits are exceeded
Type 1a super novae



Carbon detonation super novae

Difference between Type 1a Super Nova and Type 2



(Both in spectrum and mechanism)

Type 1a: no hydrogen emission lines

Carbon Detonation (carbon and oxygen)


Little or no material around core





Type 2: strong hydrogen emission lines


Core Collapse within a star that has much of its outer layers

Pulsars
a pulsating radio source thought to be associated with a rapidly rotating neutron star