ASTRO - Notes
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California State University, Chico *
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Course
204C
Subject
Astronomy
Date
Oct 30, 2023
Type
Pages
47
Uploaded by lydiafaris17
➔
Jupiter Saturn Conjunction
◆
A constellation is a region of the sky, within official borders set in 1928 by the
IAU.
◆
Most official names of the 88 constellations come from antiquity. Some southern
hemisphere constellations were named by European explorers in the 17th and
18th centuries. The patterns of stars have no physical significance.
➔
Constellations
◆
Most official names of the 88 constellations come from antiquity. The patterns of
the stars have no physical significance! Stars that appear close together may lie
at very different distances.
◆
Modern astronomers use constellations as useful general landmarks, but specify
the exact location of objects by a system of celestial coordinates.
●
North celestial pole, south celestial pole, celestial equator
●
Ecliptic: the annual path of the Sun through the celestial sphere, which is
just a projection of Earth’s orbital plane on the sky
➔
The Celestial Sphere
◆
North and south celestial poles.
◆
The sky above looks like a dome…a hemisphere…
◆
If we imagine the sky around the entire Earth, we have the celestial sphere.
◆
This is a 2-dimensional representation of the sky. There is no physical sphere up
there.
◆
Because it represents our view from Earth, we place Earth in the center of this
sphere
◆
➔
Measuring the Sky
◆
We may use a term like “angular distance,” but we want an angle, not a distance!
◆
We measure the sky in angles, not distances.
◆
Full Circle = 360 degrees
◆
1 degree = 60 arcmin
◆
1 arcmin = 60 arcsec
◆
3600 arcsec = 1 degree
◆
Note: The Moon is about 0.5 degrees, but so is the Sun! A larger object
farther away can have the same angular size as a smaller object closer to
us.
➔
MEASURING ANGLES IN THE SKY
◆
The moon is ½ degree. The Big Dipper is 5 degree. One finger is about 1
degree. A full hand is about 20 degrees. One fist is about 10 degrees.
◆
We say that the angular “distance” between these two stars in the Big
Dipper is 5 degrees.
◆
There are about 9 “fists” between horizon and zenith.
◆
CONVENIENT: Held at arm’s length…
●
Your fingernail is about 1 degree across
●
Your fist is about 10 degrees across
●
Your outstretched hand is about 20 degrees across
➔
Zenith:
The point DIRECTLY ABOVE you
➔
Horizon: ALL POINTS 90 degrees from the zenith.
➔
Elevation: The
angle
above the horizon.
➔
Meridian: A line from the northern horizon point through the zenith and down to the
southern horizon.
➔
To pinpoint a spot in the local sky…
◆
Once you specify elevation, you can use the meridian to identify the direction,
and then you have your coordinates. So if I see a star 60 degrees above the
horizon, then I know that I can use my meridian to determine the relative direction
(let’s say SE), and then I can label this object as “Altitude: 60 degrees,”
“direction: SE.”
◆
Elevation (or altitude) angle and direction along the horizon (or azimuth)
➔
Right Ascension and Declination
◆
Like latitude and longitude on the Earth
◆
Declination
is the angle (above or below) the Celestial Equator - the projection
of Earth’s equator onto the sky.
◆
Right Ascension
: is measured
along
the Celestial Equator (increasing
Eastward) from a
reference point
in the sky called the First Point of Aries
◆
Advantage
: these coordinates don’t change as a star rises and sets.
◆
Disadvantage:
You need to know your latitude and the local sidereal time.
➔
The Daily (diurnal) Motion
◆
As Earth rotates (W→E), the sky appears to us to rotate in the opposite direction
(E→W).
◆
The sky appears to rotate around the N (or S) celestial poles.
◆
If you are standing at the poles, nothing rises or sets.
◆
If you are standing at the equator everything rises and sets 90 degrees to the
horizon.
➔
Elevation angle of the celestial pole = your latitude
◆
All stars are at an angle LESS THAN your latitude away from:
●
Your celestial pole never set (they are circumpolar) and from
●
The other celestial pole never rise and cannot be seen by you.
◆
Other stars (and sun, moon, planets) rise in the Earth and set in the West at an
angle = [90 degrees - your latitude]
➔
Solar and Sidereal Days
◆
➔
Remember: the angular distance of the sun per hour. The sun is in the sky roughly 12
hours. This means that of the 360 degrees to be covered in those 24 hours, it must be
180 degrees visible/12 hours = 15 degrees one hour. Or… 360 degrees/24 hours = 15
degrees per hour.
➔
The moon is about 0.5, but so is the sun
◆
A larger object farther away can have the same angular size as a smaller object
closer to us.
➔
Definitions: The local sky
◆
Zenith - the point directly above you
◆
Horizon - all points 90 degrees from the zenith
◆
Elevation - the angle above the horizon
◆
The sun travels 15° every hour across our sky. Because 360° / 24 hours
◆
Moon is about 0.5° per hour
◆
To pinpoint a spot in the local sky. Use cardinal direction, specify elevation (or
altitude) and direction along the horizon (or azimuth)
➔
Right Ascension Declination
➔
The Seasons
◆
Our goals for learning:
➔
What is the cause of seasons on Earth?
◆
It is the tilt, as the Earth rotates the sun, the axis remains, and the only thing that
changes is the positioning in orbit about the Sun.
◆
Why are the warmest days typically a month after the beginning of summer?
◆
Global warming is like putting a sweater on the Earth
➔
The Ecliptic Tilt
◆
Earth-centric view
: the Sun moves along this titled ecliptic path.
◆
Reality
: The Earth’s
rotation
axis (defines celestial sphere coordinates) is tilted
by 23.5 degrees from its
orbital
plane
➔
Annual Motion
◆
Earth’s axis of rotation is tilted 23.5° from benig perpendicular to the ecliptic (our
orbital) plane.
◆
So, the celestial equator is tilted 23.5 degrees to the ecliptic.
◆
As seen from Earth, the Sun spends 6 months north of the celestial equator and
6 months south of the celestial equator.
◆
Seasons are caused by the tilt of Earth’s axis, not by the distance from
Earth to the Sun!
◆
The axial tilt remains fixed as Earth goes around the Sun, which implies that the
hemisphere tilted toward the Sun receives more light and heat as shown in the
following illustrations.
➔
Why doesn’t distance matter?
◆
The change of the distance between Earth and the Sun is very small - about 3%
(but distance does matter for some other planets, notably Mars and Pluto).
◆
Seasons on Earth are more extreme in the Northern Hemisphere because of the
land/ocean distribution
➔
Precession of the Equinoxes
◆
Earth’s axis actually processes (wobbles like a spinning top) once about every
26,000 years).
◆
Precession changes the position in the sky of the celestial poles and the
equinoxes!
◆
→ Polaris won’t always be the north star!
◆
→ The Spring equinox, seen by ancient Greeks in Aries, moves westward and is
now in Pisces!
➔
Lunar Motion
◆
Phases of the Moon’s 29.5 day cycle
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◆
New, waxing crescent, first quarter, waxing gibbous, full, waning gibbous, last
quarter
◆
The week comes from religion, the Book of Genesis.
➔
Why do we see the same face?
◆
Rotation period = orbital period
◆
Moon not rotating
◆
Moon rotating
➔
Why not eclipses every month?
◆
The Moon’s orbit tilted 5.2 degrees to the ecliptic plane.
◆
Crosses the ecliptic plane only at the two nodes.
◆
Eclipse possible only when full/new moon occur near those nodes - this is rare
◆
The orbital periods (of Earth and Moon) are NOT synchronized in any way.
➔
Review from Last Time
◆
Astronomy in the ancient world
◆
Ancient Greek astronomy, geocentric model of the solar system, parallax.
●
Say there is a star between me and a nearby star. Take your thumb and
move it to your face. Close one eye at a time. Does your thumb appear to
move? What about when it’s further away, does it move as much? This is
parallax. The midterm is for sure online.
◆
The Copernican Revolution and heliocentric model for the solar system.
◆
Copernicus, Tycho, Kepler, Galileo.
◆
Kepler’s Laws.
◆
The role of Galileo.
◆
The scientific method!
◆
We move slightly faster when we are closer to the sun, but it is not something we
really perceive.
➔
Describing Motion
◆
Today we will discuss the laws that govern motion and energy in the universe. By
understanding these laws, you will be able to make sense of the wide range of
phenomena that we will encounter.
●
In a previous lecture we learned that the ancient Greeks thought that it
was natural for everything to be in a state of rest. Galileo’s Galilea
◆
Motion and Force
●
Speed: rate at which object moves
○
Speed = distance/time (units of m/s)
○
Example: speed of 10 m/s
●
Velocity: speed and direction
○
Example: 10 m/s, due east
●
Acceleration: any change in velocity (either rate or direction)
○
Units must be speed/time (m/s^2)
○
Something that has a size and direction is called a
vector
◆
The Acceleration of Gravity (G)
●
All falling objects near the Earth’s surface accelerate (pick up speed) at
the same rate (not counting friction of air resistance).
●
We call this constant acceleration, g. The acceleration due to gravity.
●
On Earth, g = 10 m/s^2. Speed increases 10 m/s^2 each second until
hitting terminal velocity. Technically 9.8 m/s^2
●
Galileo showed that g is the same for falling objects, regardless of their
mass; remember mass is the quantity of matter.
➔
Mass, Momentum, Force
◆
Mass: property of a body which determines its resistance to a change in its
motion. The desire of a body to create gravity. Gravitational attraction is
proportional to the mass of the two bodies. Mass is also the desire of an object to
be moved or not (to be accelerated or not).
◆
Momentum: product of a body’s mass and velocity: M x V.
◆
Force: “push” or “pull”. More formally, a method for changing a body’s
momentum. If the mass of the body stays constant, and mv changes, then the
velocity changes: acceleration. Forces can be in balance (gravity vs. molecular
forces holding your seat together). An imbalance, or net force, is required for a
change in momentum.
◆
Normal force: the force of the floor is equal and opposite to the force of gravity.
➔
Angular Momentum
◆
Angular momentum: the momentum involved in spinning/circling: M x V x R
◆
Examples of force: gravitational, electrostatic (electromagnetic), frictional,
tension, spring, technically nuclear as well (keeps your nuclei together.
➔
What are Newton’s Three Laws of Motion?
◆
Newton’s first law of motion: An object at rest or moving at constant velocity stays
that way unless a net force acts to change its speed or direction. Inertia!
◆
Motion at constant speed is the normal state
◆
Newton’s second law of motion: the change in a body’s velocity due to an applied
force is in the same direction as the force and proportional to it, but is inversely
proportional to the body’s mass. Force = mass x acceleration.
●
Force = the rate of change of momentum
◆
Newton’s third law of motion: for every force, there is always an equal and
opposite reaction force.
●
Action = reaction.
●
Reaction forces act on different objects.
●
For any force, there is always an equal and opposite reaction force.
●
Is the force Earth exerts on you larger, smaller, or the same as the force
you exert on it?
○
Earth and I exert equal and opposite forces on each other.
➔
How is Mass Different From Weight?
◆
Mass - the amount of matter in an object (m, units of kg)
◆
Weight - the force that acts upon an object (units of newtons, or kg m/s^2)
◆
On Earth, your weight is w = mg. When gravity is the ONLY force acting you are
said to be in “free-fall.”
◆
You are “weightless” in free-fall!
➔
Conservation Laws
◆
What keeps a planet rotating on its axis and orbiting around the Sun?
◆
What are the different forms of energy?
➔
3 Important Conservation Laws:
◆
Conservation of linear momentum (mv)
◆
Conservation of angular momentum (mvr) Angular momentum (= m x v x r) is
conserved as Earth orbits the Sun. When distance r is greater, so velocity is
smaller, and when distance r is smaller, velocity is greater.
◆
Conservation of energy
◆
These laws are embodied in Newton’s laws, but offer a different and sometimes
more powerful way to consider motion.
➔
What are the different forms of energy?
◆
Energy makes matter move
●
You could think of force being the result of a difference in energy between
two points
◆
Energy is conserved, but it can:
●
Transfer from one object to another.
●
Change in form.
◆
All energy can be traced back to the Big Bang…more on that later.
➔
Basic types of energy
◆
Kinetic (motion)
●
K.E. = 1/2mv^2
◆
Radiative (light)
◆
Potential (or stored)
◆
Energy can change type but cannot be destroyed.
◆
There are many forms of stored energy.
◆
Energy is measured in JOULES. Power is the rate of using energy. Power is
measured in joules per second or watts.
➔
Thermal Energy: a sub-type of kinetic energy
◆
The collective kinetic energy (energy due to motion) of many particles (in a rock,
in air, in water)
◆
Thermal energy (a sub-type of kinetic energy) is related to temperature but it is
NOT the same as temperature.
◆
Temperature is the average kinetic energy of the many particles in a substance,
not the sum of all their energies.
➔
Mass-Energy
◆
Mass itself is a form of potential energy
●
E = mc^2
◆
A small amount of mass can release a great deal of energy.
◆
1 megaton H-bomb converts only 100 grams (3 ounces) of matter to energy.
◆
Also, concentrated energy can spontaneously turn into particles (for example, in
machines called particle accelerators).
➔
The scale of the solar system
➔
Quick tour of the major solar system components
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➔
Clues to the formation of the solar system: organized orbits/rotation of planets; terrestrial
vs. jovian planets; the nature and locations of asteroids and comets; interesting
exceptions to the patterns (motion of Venus and Uranus, the large size of Earth’s moon).
➔
A model for the formation of the solar system.
➔
The timescale of the formation of the solar system.
◆
Age of meteorites, sun, etc.
Lecture 6: Overview of the Solar System
➔
Exam will have a mixture of multiple choice and true/false questions
➔
Exam will be based on the course material up through and including “The Solar System”
➔
This corresponds to lectures 1-6
➔
The relevant reading from the textbook are given in the syllabus
➔
Review:
◆
Nature of light (wave, particle), the electromagnetic spectrum.
◆
Nature of matter on atomic scales.
◆
What do we learn from light (i.e. spectra)?
●
Composition of matter, temperature of matter, motion of matter (along the
line of sight)
◆
Telescopes: collecting area, angular resolution, refracting vs. reflecting.
Multi-wavelength.
◆
Instrumentation:
imaging
and
spectroscopy
◆
Telescopes in space. Particularly impressive telescope technologies: adaptive
optics; interferometry. Both technologies provide increased angular resolution
(i.e., sharper images). Molecules like Osof or Oxygen are pretty indicative of life.
If the oxygen doesn’t have life, it will probably react with chemicals on the surface
and change up.
➔
Mercury
◆
Made of metal and rock; large iron core.
◆
Desolate, cratered like our Moon; long, tall, steep cliffs
◆
Very hot and very cold; 425 C (day) -170 C (night)
◆
Mercury *day* = 58.6 Earth days. 3 Mercury *days*,every 2 Mercury *years*
➔
Venus
◆
Nearly identical in size to Earth; surface hidden by thick clouds.
◆
Hellish conditions due to an extreme greenhouse effect
◆
Even hotter than Mercury 470 C both day and night
◆
Atmospheric pressure is equivalent to 1 km deep in Earth’s oceans
◆
No oxygen, no water
◆
How did it end up so different from Earth? Greenhouse gas effects.
◆
Rotates backwards, and slowly, Sun rises in the West.
➔
Mars
◆
Looks almost Earth-like, but don’t be fooled - it would be hard to breathe there,
with lots of harmful UV radiation
◆
Giant volcanoes, a huge canyon, polar caps, more…
◆
Water flowed in the distant past; could there have been life?
◆
Thin atmosphere of carbon dioxide (pressure like summit of Mt. Everest)
◆
2 moons (Phobos and Deimos)
➔
Jupiter
◆
Much farther from Sun than inner planets (more than 2x distance to Mars)
◆
Also very different in composition; mostly H/He gas ball.
◆
No solid surface
◆
Gigantic for a planet. 300 x Earth’s mass; > 1,000 x Earth’s volume.
◆
Many moons, rings.
➔
Uranus
◆
Much smaller than Jupiter/Saturn, but still much larger than Earth
◆
Made of H/He gas, and hydrogen compounds (H2O2 NH3 CH4)
◆
Extreme axis tilt - nearly tipped on its “side” - makes extreme seasons during its
84 year-old orbit
◆
Moons also tipped in their orbits.
➔
Terrestrial planets are small, rocky, and close to the Sun
➔
Jovian planets are large, gas-rich, and far from the Sun
➔
What about Pluto? We will come back to Pluto
➔
Thousands of rocky asteroids lie between Mars and Jupiter
➔
A successful theory of solar system formation must allow for exceptions to general rules,
such as Uranus’s odd tilt, orbit, Earth’s relatively large moon
➔
What theory best explains the Solar System?
➔
The Nebular Theory
◆
According to the nebular theory, our solar system formed from a giant cloud of
interstellar gas (hydrogen), which also contained tiny solid grains of heavier
elements. (Nebular = cloud) → orion nebula
➔
Conservation Laws
◆
Angular Momentum:
●
In the product m X v X r, extended arms mean larger radius and smaller
velocity of rotation.
●
Bringing in her arms decreases her radius and therefore increases her
rotational velocity.
◆
Energy:
●
T = 0, v = 0 at the top of building
●
t = 1, then t =2… v = 10 m/s, then v = 20 m/s…
➔
So, as clouds get compressed, it begins to spin faster and faster… there is a
conservation of energy.
◆
As the cloud begins to fall on itself, it begins to compress, and it begins to get
faster. Temperature is a result of this motion. Gravitational energy gets converted
to thermal energy.
◆
We know this because we have taken pictures of other solar systems forming.
➔
The temperature was greatest in the core near the forming star and dropped with
distance outwards in the disk. There was a critical distance called the FROST LINE.
◆
Inside the frost line: too hot for hydrogen compounds to form ices. Only rocks and
metals condense. Outside the frost line: cold enough for ices to form; ice is
important. 98% of the material within the solar nebula is hydrogen and helium
gas that doesn’t condense anywhere.
➔
The inner part had rocky compounds:
◆
Little pieces of matter condense out of solar nebula, called planetesimals.
◆
Gravity draws planetesimals together to form planets. This process of assembly
from small parts is called accretion.
➔
Jovian Planets
◆
Planetesimals in outer solar system contain large amounts of ice in addition to
metal/rock. Gravity attracts H/He gas to ice-rich planetesimals in outer solar
system, which are more massive than Earth. Jovian planets surrounded by disks
of gas, analogous to solar nebula.
◆
As the Sun was forming, Jupiter made its own Jupiter system around itself.
➔
Why are there two types of planets?
◆
Outer planets get bigger because abundant hydrogen compounds condense to
form ICES.
◆
Outer (icy) planets accrete more easily and can then retain H and He gas
because they are much more massive (bigger); more mass means stronger
gravity.
➔
Is there evidence for this accretion model?
◆
Yes! Comets and asteroids are leftover planetesimals. Asteroids are rocky
because they formed inside the frost line. Comets are icy because they formed
outside the frost line.
➔
Earth’s Moon
◆
Earth’s moon was probably created when a big planetesimals slammed into the
newly forming Earth (almost 4.5 billion years ago). Material from outer layer
blasted into orbit around Earth (ring) and accreted into the Moon.
◆
Consistent with: Moon’s lower density, small core, similar oxygen isotope
composition to Earth, relative lack of easily vaporized constituents.
◆
Other large impacts may be responsible for other exceptions like rotation of
Venus and Uranus.
➔
Finding the Age of the Solar System
◆
We cannot find the age of the planet, but we can find the ages of the rocks that
made it up.
◆
We can determine the age of a rock through careful analysis of the proportions of
various atoms and isotopes within it.
◆
This process is called radioactive dating.
➔
The decay of radioactive elements (e.g. Potassium-40) into other elements (e.g.
Argon-40) is a key tool in finding the ages of rocks.
◆
Analysis based on knowing how much Argon-40 there was to start with (e.g.,
none), and how much has escaped (e.g., none).
➔
What have we learned?
◆
What features of our solar system provide clues to how it formed?
●
Four major features provide clues: (1) The Sun, planets, and large moons
generally rotate and orbit in a very organized way. (2) With the exception
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of Pluto, the planets divide clearly into two groups: terrestrial and jovian.
(3) The solar system contains huge numbers of asteroids and comets. (4)
There are some notable exceptions to these general patterns.
◆
What theory best explains the features of our solar system?
●
The nebular theory, which holds that the solar system formed from the
gravitational collapse of a great cloud of gas.
●
Radiometric dating of meteorites sets the age of the solar system as 4.6
billion years.
◆
What caused the orderly patterns of motion in our solar system?
●
A collapsing gas cloud naturally tends to heat up, spin faster, and flatten
out as it shrinks in size. Thus, our solar system began as a spinning disk
of gas. The orderly motions we observe today all came from the orderly
motion of this spinning disk of gas.
◆
Why are there two types of planets?
●
Planets formed around seeds
Review Midterm 1
➔
Mass of the hydrogen atoms: 10^-27 kg
➔
Age of the universe in seconds 10^17 sec
➔
If earth was a basketball
◆
The moon would be a tennis ball 30 ft.away
◆
Sun would be 2.2 miles away
◆
Pluto would be 80 miles away
◆
The nearest star would be 500,000 miles away.
➔
Light year
◆
The speed of light is 300,000 km/s
◆
There are about 31.5 million seconds in a year
◆
Alpha Centauri takes 4.2 years to travel going speed of light
➔
Universe
◆
Milky way contains 100 billion stars and is 100,000 light years across
◆
Solar system is about 28,000 light years from the center of the Milky Way
◆
Nearest galaxies (Magellic Clouds) are 200,000 light years away.
◆
Nearest spiral galaxy (Andromeda) is 2.3 million light years away)
◆
Most distant galaxies are about 10 billion ly away
◆
We see these galaxies as they were billions of years ago
➔
We are going about 1650 km/hour or 1000 mph at the equator
➔
Earth orbits revolves around the Sun once every year traveling at an avg speed of 30
km/s
◆
Earth’s average orbital speed is 108,000 km/hr
◆
Perihelion nearest point to the Sun in orbit is 147.1 million km and 152.1 million
km is our aphelion: farthest point from the Sun in orbit
➔
Our Sun and solar system orbit around the center of the Milky Way Galaxy every 230
million years! This speed is at about 540,000 mph
➔
Mass-Energy
◆
Mass itself is a form of potential energy E = mc^2
◆
A small amount of mass can release a great deal of energy.
◆
1 megaton H-bomb converts only 100 grams (3 ounces) of matter to energy.
◆
Also, concentrated energy can spontaneously turn into particles (for example, in
machines called particle accelerators); m = E/C^2
➔
The Force of Gravity
◆
One of Isaac Newton’s most important discoveries
◆
Masses attract each other through the force of gravity,
Fg
.
◆
The strength of the gravitational force,
Fg
, between two masses,
M1
and
M2
, is
proportional to the product of
M1
and
M2
.
◆
The strength of the gravitational force,
Fg
, between two masses,
M1
and
M2
, is
inversely proportional
to the square of the distance between the two objects,
d
.
◆
What’s another force that falls off according to the inverse square of the
distance? What’s a force that follows a different proportionality?
◆
What happens when th distance approaches infinity?
➔
WHAT DETERMINES THE STRENGTH OF GRAVITY?
◆
The Universal Law of Gravitation
◆
(1) Every mass attracts every other mass
◆
(2) Attraction is directly proportional to the product of their masses.
◆
(3) Attraction is inversely proportional to the square of the distance between their
centers.
◆
Fg = G * (M1*M2)/d^2
◆
Gravity is not a constant force; its value changes with distance
➔
What happens to the strength of the force is we double one of the masses?
◆
A. ½ as strong. B. 2 times stronger. C. 16 times stronger. D. ¼ as strong
➔
Escape Velocity
◆
If an object gains enough orbital energy, it may
escape
(change from a bound to
an unbound orbit).
◆
Escape velocity
from Earth = 11.1 km/s from sea level (about 40,200 km/hr;
25,000 mph or 7 miles per second). This velocity depends on the mass and
radius of the Earth, not the mass of the object - i.e.
Vesc = (2GMearth/Rearth)^½
➔
Newton’s Version of Kepler’s 3rd Law
◆
If
a small object orbits a larger one, and you measure the orbiting
object’s orbital
period
AND
average orbital radius
◆
THEN you can calculate the
mass
of the larger object
◆
Examples
(
know these
):
●
Calculate mass of Sun from Earth’s orbital period (1 year) and average
distance (1 AU).
●
Calculate mass of Earth from the orbital period and average distance of
any orbiting satellite, including the Moon.
●
Calculate mass of Jupiter from the orbital period and distance from Jupiter
of one of its moons.
◆
Newton’s Version of Kepler’s 3rd Law
●
p^2 = ((4pi^2)/G(M1+M2))*a^3
●
Where, p = orbital period; a = average orbital distance (between centers)
●
(M1 + M2) = sum of object masses
●
So, if M2 is tiny compared to M1, then M1 = 4pi^2a^3/Gp^2
●
Period of Moon around Earth takes about 27 days.
➔
Light: The Cosmic Messenger
◆
Basic Properties of Light and Matter
◆
Newton showed that white light is composed of all the colors of the rainbow. But
just as there are sounds we cannot hear, there are colors we cannot see. Visible
light is a tiny part of a vast electromagnetic spectrum of radiant energy.
➔
Light is an electromagnetic wave
◆
If you could line up electrons they would wiggle up and down as a light
wave passed by.
◆
Light waves are vibrations in electric and magnetic fields caused by (and
causing) the motions of charged particles. Radio waves and X-rays are forms of
light, just like the visible waves we see. All are electromagnetic waves.
◆
Wavelength x Frequency = c
◆
C = 300,000 km/s
◆
All light travels with speed c = 300,000 km/s
◆
Frequency tells us how many times any point on the rope bobs up and down
each second. Wavelength is the distance between adjacent peaks of the electric
field. Frequency is the number of times each second that the electric field peaks
at any point.
➔
The Electromagnetic Spectrum
◆
Gamma rays - shortest wavelength; highest energy
◆
X-Rays - wavelengths about size of atoms
◆
Ultra Violet (UV)
◆
Visible light - the wavelengths our eyes can “detect”
◆
Infra Red (IR)
◆
Microwaves - wavelengths of a few millimeters
◆
Radio waves - longest wavelength; lowest energy
◆
All travel at the same speed in outer space; only visible light, radio and some
infrared waves pass through Earth’s atmosphere.
➔
Light is also a particle!
◆
From measurements of the
photoelectric
effect in which light seems to knock
electrons out of atoms, Einstein came up with the idea of “photons.”
◆
Photons
: “pieces” of light (radiant energy), each with precise wavelength,
frequency and
energy
. The more compact the photon wavelength, the higher its
energy: in fact,
E = h * frequency
or
E = hc/wavelength
◆
Where
h
is a constant called Planck’s constant (6.626 x 10^-34Jxs). Photons
come from electrically charged particles (usually electrons in atoms).
➔
What is matter?
◆
Atomic structure: atoms have a nucleus and orbiting electrons
◆
The nucleus is nearly 100,000 times smaller than the atom but contains nearly all
of its mass
➔
Atomic Terminology
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◆
Atomic Number = # of protons in nucleus
◆
Atomic Mass Number = # of protons + neutrons
➔
Isotopes
◆
Isotope: same # of protons but different # of neutrons.
◆
Molecules: consist of two or more atoms
◆
Ion: atom or molecule with net positive or negative charge (because # of protons
and electrons doesn’t balance
◆
Different isotopes of the same element contain the same number of protons but
different number of neutrons
➔
How do light and matter interact?
◆
Emission
…photons are produced
◆
Absorption
…photons are consumed
◆
Transmission
…photons pass through freely
◆
Reflection or Scattering
…photons are redirected, in the same (reflection) or
random (scattering) directions
➔
What types of light spectra can we observe?
◆
Continuous spectrum
◆
Absorption line spectrum
◆
A plot of energy versus wavelength is a spectral energy distribution, or simply a
spectrum
➔
How does light tell us what things are made of?
◆
Electrons in atoms have distinct
energy levels
.
◆
We say that the electron energy is
quantized
.
◆
You could think of this as orbital energy.
◆
Each chemical element, ion, molecule,
has a unique set of energy levels
.
◆
The energy levels are tiny, and given in special units called electron volts; 1
eV = 1.6 x 10^-19 joules
➔
Distinct energy levels in atoms lead to distinct emission or absorption lines
◆
The Unique Hydrogen energy levels and hydrogen spectra in emission and
absorption.
➔
How does light tell us the temperatures of planets and stars?
◆
Thermal Radiation:
●
Nearly all large or dense objects emit
thermal radiation
, including stars,
planets, you…
◆
An object’s thermal radiation spectrum depends on only one property: its
temperature
●
Temperature represents
average kinetic energy
●
In a dense object, the many random bounces of photons means that the
photons end up with energies that match the kinetic energies of atoms or
molecules of the object.
●
Because the photon's energies depend only on the object’s temperature,
we call this light “
thermal radiation
.”
●
Electromagnetic radiation produced this way has a
continuous
spectrum
of energy with a
peak at one wavelength
. That wavelength is
determined only by the temperature of the object.
➔
Two Properties of Thermal Radiation
◆
(1) Hotter objects emit more light at all frequencies per unit area
◆
(2) Hotter objects emit photons with a higher average energy.
➔
Two Laws of Physics:
◆
Stefan-Boltzmann
: Emitted intensity per square meter = constant * T^4
◆
Wien’s Law
: Wavelength of maximum emission = constant/T
➔
The Doppler Effect:
◆
Frequency changes with directional movement of the auditory source. Light
waves do the same.
➔
Thought Question:
➔
I measured a line in the lab at 500.7nm. The same line in a star has a wavelength 502.8
nm. What can I say about this star?
◆
Longer wavelength means shift to red due to recession (moving away).
◆
The Doppler shift tells us only about the part of an object’s motion toward or
away from us, also called the “line of sight” motion. The object could be moving
partially across our line of sight.
➔
Doppler Effect Summary
◆
Motion toward or away from an observer causes a shift in the observed
wavelength of light:
◆
Blueshift (shorter wavelength) → motion toward you
◆
Redshift (longer wavelength) → motion away from you
◆
V = change in wavelength / original wavelength * C (speed of light km/s)
◆
Greater shift → Greater speed
◆
502.8 - 500.7 / * c → 2.1 / 500.7 * c = 0.00149 * 300,000 km/s = about 1.2 million
m/s
◆
The Doppler effect tells us how fast an object is moving toward or away from us.
◆
Blushift: objects moving toward us.
◆
Redshift: objects moving away from us.
◆
Every kind of atom, ion, molecule, produces a unique set of spectral lines.
◆
We get temperature from the spectrum of thermal radiation.
➔
Collecting Light With Telescopes
◆
We collect more light with telescopes than with our eyes. And we have a stronger
sharpness of things in the cosmos close together.
◆
Telescopes collect more light than our eyes → light-collecting area
●
Scales as (Telescope Diameter)^2
●
10-m telescope is 100 times better than a 1-m telescope
◆
Telescopes can see more detail than our eyes → angular resolution
●
Smallest angular size resolved scales as 1/(Telescope Diameter)
●
10-m telescope can resolve 10 times finer detail than 1-m telescope
●
Telescopes + instruments can detect light that is invisible to our eyes
(e.g., infrared, ultraviolet)
➔
Angular Resolution
◆
The
minimum
angular separation that the telescope can distinguish.
◆
The headlights are always the same real distance apart, but when far away it is
hard to distinguish them as a pair.
➔
Refracting → Lenses
◆
Rarely used by professional astronomers now
◆
Refracting telescope, Yerkes 1-m refractor, Chicago.
➔
Reflecting → Curved Mirrors
◆
Most research telescopes today are reflecting. Why?
●
Lenses refract different wavelengths of light different amounts (chromatic
aberration)
●
Lenses must have two good surfaces.
●
Lenses can only be supported on their perimeters; mirrors can be
supported from behind.
➔
Reflecting → Curved mirrors
◆
Most research telescopes today are reflecting
◆
Keck 2 x 10-m Hawaii
➔
Instrumentation
◆
What do astronomers do with telescopes?
◆
Imaging
: cameras record “photographs” (i.e., digital images) of astronomical
objects on detectors, often using specific color filters. Measure how much light
there is from the object, and its structure.
◆
Spectroscopy
: spectrographs use dispersive elements (e.g., diffraction grating
or prism) to separate light of different wavelengths into spectra, recorded on
detectors. Spectra contains important information (As discussed).
➔
Why do we put telescopes into space?
◆
It is NOT because they are closer to the stars!
◆
On a 1-to-10 billion scale:
●
Sun size of grapefruit. Earth size of ball point, 15 m from Sun.
●
Nearest stars 4,000 km away (LA to NY)!
●
Hubble’s orbit is microscopically above ball-point size Earth.
●
So, why go to space?
➔
Observing problems due to Earth’s atmosphere
◆
Light pollution, Air turbulence caused blurred images.
◆
Atmosphere absorbs most of the electromagnetic (EM) spectrum, including all
UV and X-ray, most infrared.
➔
Telescopes in space solve 3 problems
◆
However, location and new technology can help overcome light pollution and
turbulence for ground-baseed telescopes. Very large telescopes can be built on
the ground for less cost than smaller ones in space.
◆
Nothing short of going to space can solve problem of atmospheric absorption of
light (X-Ray, UV, infrared)
●
Chandra X-ray observatory
➔
How is technology revolutionizing astronomy?
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◆
Adaptive optics and digital imaging
◆
Turbulence in the atmosphere blurs images and prevents telescopes from
reaching their natural degree of angular resolution.
➔
Adaptive Optics and Digital Imaging
◆
Rapid changes (700 times per second) in the shape of a special mirror can
compensate for atmospheric turbulence
●
Without adaptive optics; single blurred object.
●
With adaptive optics; resolved into 2 objects.
➔
The planets are tiny compared to the distance between them. Two groups: the inner 4
terrestrial planets and the outer 4 Jovian planets and pluto.
➔
Venus, Mercury, Earth, all the planets orbit on the same orbital plane, so they are NOT
orbiting perpendicular to the ecliptic plane.
➔
If Ben Frank lit a candle at the moment of the declaration of independence, how far has
it reached?
◆
250 yr * 3e7 s/yr * 3e8 m/s = 2e18m
➔
Which of the following statements is true about a star and planet system?
◆
The star and planet move around a common center of gravity that is much closer
to the star than to the planet.
MIDTERM 2 PRACTICE - LECTURE 8
➔
Jovian Planet Basics
◆
What are Jovian Planets made of?
●
Hydrogen and helium
◆
What are jovian planets like on the inside?
◆
What is the weather like on Jovian planets
➔
Bigger than Earth, and with more mass than Earth
◆
Lower density, so different composition from Earth
◆
Rings. Numerous moons. Studied by space missions: Pioneer 10, 11; Voyager 1,
2,; Galileo; Cassini
➔
What are jovian planets made of?
◆
Jupiter and Saturn: almost all H and He, very little metal and rock (therefore less
dense.)
◆
Uranus and Neptune: <50% H and He, the rest hydrogen compounds (water,
methane, ammonia), with some metal and rock.
◆
Why are they different in composition?
➔
Jovian Planet formation
◆
Recall the conditions in the solar nebula
◆
Beyond the Frost Line, planetesimals could accumulate ICE
◆
Hydrogen compounds are more abundant than rock/metal so jovian planets got
bigger.
◆
The gravity of such large cores pulled in hydrogen and helium from the nebula
and so these objects acquired H/He atmospheres
➔
Jovian planet formation
◆
All the Jovian cores are very similar: ~10 x Earth masses
◆
The jovian differences are in the amount of H/He gas accumulated.
➔
Why did that amount differ?
➔
Differences in Jovian planet formation
◆
Timing
: the planet that forms earliest captures the most hydrogen and helium
has. Capture ceases after the first solar wind blew the leftover gas away.
◆
Location
: the planet that forms in a denser part of the nebula forms its core first
and grows bigger.
➔
More distant Jovian planets (Uranus, Neptune) started forming later than closer-in ones
(Jupiter, Saturn).
➔
Since the solar wind blew out remaining gas at a certain point, Uranus/Neptune had less
time to accumulate gas → ended up smaller.
➔
Jovian Planet Densities
◆
Stacking pillows
◆
Adding one more results in greater compression of the lower layers; the stack
gets smaller.
◆
Jupiter and Saturn are nearly the same size (radius). More massive planets
could even be smaller!
➔
What are jovian planets like on the inside?
◆
No solid surface. Layers and layers of gas under ever higher pressure and
temperatures.
◆
Cores (~10 Earth masses) made of hydrogen compounds, metals & rock.
◆
The layers are different for the different planets. Why?
➔
Layers Differ in Phase
◆
Density of liquid water is ~ 1g/cm^3
◆
Gaseous hydrogen: cold and very low density.
◆
Liquid hydrogen:
caused by compression of overlying layers; much denser and
hotter.
◆
Metallic hydrogen
conducts electricity; it is not solid, but a very viscous fluid.
◆
Core
is hydrogen compounds, metals, rocks. But not in a form you’d recognize…
10x the mass of Earth inside a volume the size of Earth.
➔
Why different?
◆
Less mass → less gravity → less compression.
◆
Mass controls everything.
◆
Boundaries of the layers are deeper in less massive jovian planets.
◆
The physical states of the less massive jovians are less extreme (could even be
liquid).
➔
Rotation
◆
Jovian planets rotate rapidly (“day” is ~10 hours for Jupiter and Saturn, and
16-17 hours for Uranus and Neptune).
◆
Saturn is flattened by rotation! More so than Jupiter since Saturn’s surface gravity
is weaker.
◆
Gravity pulls material inward in all directions…but rapid rotation flings material
outward near the equator.
◆
That is why Saturn is not a perfect sphere. Compare its actual shape to the
dashed circle.
➔
Magnetic Fields
◆
Jupiter has a very powerful magnetic field generated by its rotating, convection
layer of metallic hydrogen. (Behaves like the Earth’s iron core.) Strongest among
jovian planets, since it has the largest amount of electrically conducting metallic
hydrogen.
➔
What is the weather like on jovian planets?
◆
Colorful surface features reveal: –
●
Clouds of different chemical compositions (in the atmosphere of hydrogen
and helium).
●
High wind speeds.
●
Storms, some very long-lasting.
➔
Jupiter’s Colors
◆
Compounds in the ammonium hydrosulfide (NH4SH) bearing clouds reflect
red/brown.
◆
Ammonia, the highest coldest layer, reflects white.
◆
Atmosphere features alternating bands of rising and falling air (alternating
colors), controlled by rapid rotation.
➔
Saturn’s Colors
◆
Saturn’s layers are the same, but deeper in and farther from the Sun --- more
subdued.
◆
Layers occur deeper because Saturn’s atmosphere is overall colder, so clouds
condense at lower altitudes
➔
Uranus and Neptune’s upper layers are colder still, allowing
methane
to condense.
➔
Methane gas absorbs red light and transmits blue light reflected by clouds.
➔
The Great Red Spot
◆
The Coriolis force diverts winds.
◆
High pressure in the middle of the storm.
◆
Twice as wide as the Earth. This storm has existed for at least 300 years.
Review - Lecture January 18, 2022
➔
What determines the strength of gravity?
➔
How does Newton’s law of gravity extend Kepler’s laws?
➔
How do gravity and energy together allow us to understand orbits?
➔
(If time at the end): How does gravity cause tides?
LECTURE JANUARY 25th, 2022 - 7
➔
Why is Earth Geologically Active?
◆
Short Answer: Earth is a big enough planet to still have a hot interior.
◆
So what do we know about the interior of Earth and why is it hot?
●
Geologically active = surface reshaped by processes such as volcanoes,
earthquakes, erosion, and plate tectonics.
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◆
Internal Structure and the Lithosphere
●
The “lithosphere” is the cool rigid rock that forms a planet’s outer layer;
the crust and some of the mantle.
◆
The lithosphere floats on the lo er layers.
●
If the lithosphere is near the surface then the planet will be geologically
active.
➔
Differentiation
◆
Layers ordered by density.
◆
Highest density on the bottom.
◆
Gravity sorts materials by density
➔
Differentiation converts gravitational potential energy to heat.
◆
As dense materials sink they convert gravitational energy to kinetic energy (heat).
◆
That’s definitely why the very dense core of Earth and other planets are hotter.
◆
This is what drives geological activity.
➔
Heat transfer drives geological activity
◆
As planet cools, internal heat must transfer to planetary surface. For Earth, most
important heat transfer process is convection.
◆
Convection
: hot molten rock rises, cool rock falls.
◆
1 mantle convection cycle takes 100 million years on Earth (1 cm/year).
◆
Mantle convection: hot rock rises and cooler rock falls.
➔
Planet size matters
◆
A large terrestrial planet
◆
Is still warm inside (surface-area/volume ratio)
◆
Has a “convecting” mantle
◆
Has a thinner, weaker lithosphere
◆
Has molten rock nearer the surface.
●
Which makes it more geologically active
●
Earth and Venus should be geologically active, whereas Mercury and
Moon should not. Mars is intermediate.
◆
Venus has too thin of crust, so the crust does not float, it breaks.
➔
Planet Size Matters
◆
Volume: total amount of heat contained in a planet
◆
Surface area: rate at which heat escapes a planet
◆
Ratio of surface-area-to-volume determines the time it takes for planet to
cool off.
◆
Larger surface-area-to-volume → shorter cooling time.
◆
Smaller surface-area-to-volume → longer cooling time.
◆
Surface area relies on square of the radius.
➔
Surface-area-to-volume = surface area / volume
➔
Surface area of a sphere? 4piR^2
➔
Volume of a sphere? 4/3piR^3
➔
Surface-area-to-volume = 4piR^2 / (4/3piR^3) = 3/R
➔
This means that, as R gets bigger (i.e., in larger objects), surface-area-to-volume
decreases.
◆
Since smaller surface-area-to-volume means longer cooling times, this
means that larger objects take longer to cool off!
◆
This rule applies to the terrestrial planets.
➔
Mars vs. Earth
◆
50% Earth’s radius, 10% Earth’s mass
◆
1.5 A.U. from the Sun; so (1.5)^2 less heat and light
◆
Axis tilt about the same as Earth; seasons
◆
Similar rotation period (23.96 hours vs. 24.6 hours)
◆
Orbit is more elliptical than Earth; seasons more extreme in the South than
the north.
◆
Very thin CO2 atmosphere: little greenhouse effect.
◆
Cold desert, despite warm red look due to soil color.
◆
So main difference is…Mars is smaller!
◆
Orbit is a little bit more elliptical than earth, so the seasons are more
extreme.
➔
Why did Mars change?
◆
It was too small, it cooled off too quickly, lost its magnetic field and then
the solar wind stripped away its atmosphere. Temps dropped and it “freeze
dried” (3 billion years ago). Solar radiation wiped out atmosphere.
➔
Planetary Magnetic Fields
◆
Moving charged particles create magnetic fields.
◆
Magnetic fields are very important for many reasons:
●
A planet’s interior can also create a magnetic field, if the core is
electrically conducting (e.g. iron), convecting (molten), and rotating.
●
Internal heat contributes to planetary magnetic field.
●
Earth is only terrestrial planet with strong magnetic field.
◆
Dynamo effect
➔
Earth has both rotation and liquified metals in the interior, thus giving it that
magnetic charge because its moving (rotating) and it has electrically conducting
metals inside that are convecting.
➔
Mars has rotation, but not the liquified metals in the interior.
➔
Venus has an interior really good core, but it is not rotating fast enough to generate
a magnetic field.
➔
Jupiter has a very strong magnetic field, because it is rotating fast, and on top of
that there’s something called metallic hydrogen in the center which can generate
the magnetic field.
➔
Earth’s Magnetosphere
◆
Earth’s magnetic fields protect us from charged particles from the Sun - the
Solar Wind
◆
The charged particles can create aurorae - the “Northern Lights”
◆
They are nothing but charged high-energy particles arriving on Earth from
the Sun, carried by the Solar Wind.
◆
You’re actually more prone to cancer if you fly a lot or go on space
missions in the atmosphere, because of your exposure to these charged
particles.
➔
What processes shape Earth’s surface?
◆
Impact cratering: creation of bowl-shaped features by asteroids or comets
striking a planet’s surface.
◆
Volcanism: eruption of molten rock from a planet’s interior onto its surface.
◆
Tectonics: disruption of planet’s surface by internal stresses.
◆
Erosion: wearing down/building up of geological features by wind, water,
ice (i.e., planetary “weather”).
➔
Tectonics: any surface reshaping from forces acting on the lithosphere
◆
Internal heat required.
➔
Plate tectonics: pieces of lithosphere moving around. Collisions of plates cause
mountains to be built. Sideways motion of plates cause earthquakes.
◆
Only Earth has plate tectonics.
➔
What is an atmosphere?
◆
Atmosphere: thin layer of gas surrounding a world.
◆
Earth’s atmosphere N2 (78%) and O2 (21%) and other stuff (1%)
◆
Other common molecules in terrestrial atmospheres: H20, C02.
➔
How does Earth’s atmosphere affect Earth?
◆
Weather/erosion
◆
Protection from radiation
◆
Changes surface temperature: the greenhouse effect.
◆
Makes the sky blue!
◆
Blue photons are scattered most and red photons least.
➔
What is a “greenhouse gas”
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◆
Any gas that absorbs infrared light
◆
Greenhouse gas: molecules with 2 different types of elements (c02, h20,
ch4) - carbon dioxide, water vapor and methane are all greenhouse hases.
◆
Not a greenhouse gas: molecules with single or 2 atoms of the sam element
- oxygen and nitrogen.
◆
The Earth is much warmer (roughly 30K) because of the greenhouse effect
than it would be without an atmosphere…but so is Venus. It is only bad if it
is a “runaway” effect .
◆
A “runaway” greenhouse effect would then occur.
◆
Eventually, water molecules would break down and escape to space, just as
apparently happened on Venus.
Lecture February 3rd, 2022 - Lecture 9 - Extrasolar Planets
➔
A minimalist definition. Celestial body that is:
◆
Gravitationally bound to a star. No nuclear fusion.
➔
How do we find them? As of Jan 29, 2022 - 4949 known
◆
Radial velocities: 988
◆
Transit: 3495
◆
Microlensing: 168
◆
Direct Imaging: 186
◆
Timing: 45 (not discussed here)
➔
The Challenge
◆
Even though it seems likely that the galaxy is teeming with exoplanets,
finding them isn’t easy.
◆
Planets are millions of times dimmer than the stars they orbit, and these star
systems are incredibly distant.
◆
The challenge of observing extrasolar planets steam from three basic facts:
●
1. Planets don’t produce any light of their own, except when young
●
2. Exoplanets are at an enormous distance away from us
●
3. Exoplanets are lost in the blinding glare of their parent stars
➔
Newton’s Laws applied to planetary motions around their star
◆
F(star on planet) = - F(planet on star) (third law) equal and opposite forces
◆
M(planet) a(planet) = -M(star) a(star) (second law) means that Mass and
acceleration of the planets are equal and opposite.
◆
a(star) = a(planet) x {M(planet) / M(star)} if you divide both sides, you can
see that the acceleration of the star is equal to the acceleration of the planet
times the ratio of the mass of the planet to that of the mass of star.
◆
Sun is only pushed around by 1m/s by Earth
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◆
Both objects orbit around their common center-of-mass
●
In reality, the motions caused by all planets must be added together.
➔
Gravitational Interactions
◆
Two techniques
: the
Astrometric
method and the
Doppler
method.
◆
Both rely on observing the
motion of the star
caused by small gravitational
tugs from orbiting planets.
➔
The center of mass of a planetary system can be thought of as a fulcrum on a
see-saw
◆
Jupiter may
seem
to orbit the Sun, but it actually orbits every 12 years
around the center of mass of the solar system.
➔
Doppler Effect:
◆
When you can tell the velocity of an object by the displacement of the
frequency of wavelength of light. Blackbody. The Doppler effect is kind of
like what the police uses to tell if someone is speeding.
◆
Shorter wavelength, moving towards us. Longer wavelength, moving away
from us.
➔
Center of Mass of the Solar System
◆
For the solar system,
the center of mass is just outside the surface of the
Sun.
◆
The sun matches pace with Jupiter, making a tiny 12 year orbit around the
same center of mass.
◆
The Sun’s position wobbles on the sky as seen from a distance.
◆
Limited use of Astrometric Method
➔
Radial Velocities
◆
Very difficult measurement! Speed < m/s. Orbital inclination
●
When the star is moving towards us, we see the light from the star
blueshifted.
●
When the star is moving away from us, we see the light from the star
redshifted. (This is all within an orbit).
➔
Multi-Planet Systems
◆
A 7-Earth mass planet
●
At 0.021 AU from its star, its “year” = 2 days
◆
Planet Transit
●
Mercury’s 2006 Transit as imaged by NASA satellite Soho
➔
Extrasolar Planets Transit
◆
Y-Axis = delta L/L
◆
X-Axis = time (hrs + JD)
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◆
What creates the depth of the transit is the ratio of the surface area of the
planet and the surface area of the star.
➔
Surface Area of a Sphere: 4pi(r)^2
◆
Area of a circle = pi(r)^2
◆
Much easier to detect bigger planets than smaller ones using the transit.
➔
Kepler - 2009 through 2018
◆
Stared a patch in the sky, and measured the luminosity of many many stars
◆
The reason that it needed to be above the atmosphere was because the
turbulence in the atmosphere will screw with vision.
➔
Direct Methods
◆
Neither the Doppler radial velocity method nor the Transit Method allow us
to “see” the planet directly.
◆
Instead, to do that we need direct images - but this is not easy.
➔
There are two problems:
◆
Contrast
: even a giant planet like Jupiter is about 1 billion times fainter
than the Sun - infrared helps (why?)
◆
Angular resolution
: atmospheric turbulence blurs images. At ~300ly; a
typical blurred image corresponds to a region larger than solar system
(~100 AU). With the giant Keck telescope and Adaptive Optics in the
infrared we improve the angular resolution by ~50x, allowing us to see
things on the scale of 2 AU.
➔
Question 2:
◆
Jupiter’s mass is approximately 317x that of Earth. Aliens are trying to
detect planets around the Sun using the radial velocity method. How much
stronger will be Jupiter’s signal compared to Earth?
●
317 times.
➔
Demographics
◆
How we measure properties of extrasolar planets
●
Period
●
Distance
●
Eccentricity
●
Inclination
●
Mass
●
Size (radius)
●
Density
●
Atmospheric composition and temperature
➔
Properties of the Exoplanets
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◆
Exoplanetary systems are common - 10% stars have one or more planets -
could be 50%
◆
Jupiter size planets - dominate radial velocity detections due to large mass,
but are rare - planets with measured radii have low mean densities ~ 1000
kg/m^3 - many orbit close to star, some in highly elliptical orbits (not
circular as expected) - surface temperatures are high, and radii larger than
expected from jupiter models.
◆
Super-Earths - Kepler has detected ~ 2300 Earth/Super-Earth, 1600
Neptune planets in transit - mass and radii → high mean density → rocks
and metals; moderate mean density → rocks and ice
➔
Many Worlds
◆
~400 billion stars in our galaxy alone.
◆
G (7%)
, K (15%) and M (75%) stars = 97% of all stars in the galaxy.
◆
Our existence proves that G stars can have habitable zones.
◆
Statistically, ~40 billion Earth-sized planets
orbit in the habitable zones
of sun-like stars or red dwarf stars.
➔
Summary
◆
Exoplanets
◆
Since 1995 we have discovered more than 4000!
◆
They are hard to find because they are dim and light compared to their
parent star.
◆
How do we find them?
●
Direct imaging. Needs extremely high resolution
●
Doppler shift. Very high precision spectroscopy. Gives mass and
period.
●
Transit. Very high precision imaging. Gives size of planet and period
●
Microlensing.
◆
We know that there are LOTS of planets in our Galaxy! Some of them may
be habitable and host life!
➔
Radial Velocities
◆
We can not see the star move because the movement is too small for us to
see. But we can observe light coming from the star and we can see the shift
in the wavelength of the planet. We can see a shift in oxygen transition and
we can measure that very very accurately, maybe even to m/s. We can use
that motion to infer the presence of a planet. And the period of that
movement gives us the period of the planet as well. And the amplitude
gives us the mass/duration of the period of the planet as well.
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➔
Question 1:
◆
Jupiter’s radius is approximately 11x that of Earth. Aliens are trying to
detect planets around the Sun using the transit method. How much stronger
will be Jupiter’s signal be compared to Earth?
●
11^2 = 121 times.
●
Depth of the transit, apparent luminosity depends on the size of the
planet, so the square of the radius because Area = pi(r)^2. So the
square of the radius 11 = 11^2 = 121 times.
➔
Question 2:
◆
Jupiter’s mass is approximately 317x that of Earth. Aliens are trying to
detect planets around the Sun using the radial velocity method. How much
stronger will be Jupiter’s signal be compared to Earth?
◆
317 times.
◆
When you are using the radial velocity method, it depends on the ratio of
the masses. Jupiter is 317x more massive than earth, so the signal will be
317x bigger.
Lecture 10 - The Sun
➔
Review
◆
Techniques for finding extrasolar planets:
●
RV method, direct imaging, transits
◆
The Kepler mission
◆
Revising models of planet formation.
➔
The Sun: Our Star
◆
Contains 99.9% of the mass in the solar system
◆
Source of heat and light for Earth
●
Life impossible without it
◆
Only star we can study in such exquisite detail
➔
Stars are simple
◆
Spherical distributions of hot gas
◆
Radiate huge amounts of energy
◆
Held together by balance between gravity and gas pressure.
➔
Basic Properties of the Sun
◆
Distance: 1.49 x 10^11 m = 1 AU
◆
Mass: 1.99 x 10^30 kg (300,000 Earths)
◆
Radius: 6.96 x 10^8 m (109 Earths)
◆
Density: 1.41 x 10^3 kg/m^3
◆
Luminosity: 3.83 x 10^26 watts
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➔
Composition of the Sun
◆
Sun is transforming Hydrogen into helium
◆
70% Hydrogen and 28% Helium
●
And so there is a little less hydrogen than from the Big Bang, and a
little MORE helium than from the Big Bang, because the star is
releasing hydrogen and MAKING helium.
◆
But, there is also Oxygen, and 0.3% carbon, 0.2% Iron
●
This comes from the fusion of light into elements.
●
Where did this happen? So, the Sun is currently fusing hydrogen into
helium, it is not fusing oxygen, carbon, or iron.
●
These elements come from OTHER STARS.
◆
The mere fact that we see these elements mean that the Sun is not the
FIRST star to be formed in the universe, there were other stars that
exploded prior and those gasses were enriched by the death of previous
stars to eventually become the Sun.
➔
How do we know? Spectroscopy
◆
On top of the blackbody curve, there are absorption features on the surface
of the Sun. Identified by transitions of known elements. There is a certain
abundance of these elements. We can use other forms of reasoning to
estimate the total composition of the Sun.
➔
Layers of the Sun:
◆
Temperature
Thickness
➔
Core:
◆
1.5 x 10^K ; 0.2 R
➔
Radiation
◆
> 2 x 10^6K ; (0.713-0.20) R
➔
Convection Zone, Photosphere, Chromosphere, Corona, Solar Wind,
◆
See the slides for all the numbers
➔
The Solar Wind:
◆
A flow of charged particles, protons and electrons, from the visually opaque
“surface of the Sun.
◆
Remember: the Sun is a ball of gas throughout. There is no solid surface.
➔
Corona:
◆
The outermost gaseous layer of the solar “atmosphere”.
◆
Very thin; fast moving particles.
◆
T~1 million K
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◆
Remember that temperature is equivalent to average kinetic energy of the
gas.
➔
Chromosphere:
➔
Middle layer of the solar atmosphere; can be seen as pinkish in eclipse due to
hydrogen emission - hence the “chromo” in the name.
◆
T ~ 10^4 - 10^5 K
➔
Chromosphere and Corona visible during an eclipse
➔
Photosphere:
◆
Visible “surface” of Sun. Not really a surface in the normal sense.
◆
This is just as far into the Sun as we can SEE. The gas becomes dense and
opaque below this level.
◆
T ~ 6,000 K
➔
Convection Zone:
◆
Hot, dense turbulent gas.
◆
Energy transported upward by rising hot gas.
◆
Breaks through photosphere to cause a granulation appearance that reminds
one of boiling water.
◆
Granulation in Photosphere: Tops of convective cells
➔
Radiation Zone:
◆
A much hotter and denser region. Energy transported upward by photons,
not by the mass motion of gas.
➔
Core:
◆
Extremely dense region, but still gaseous!
◆
Energy generated here.
◆
Temperature: ~ 15 million K
◆
Hydrogen gas in the Sun is almost a “perfect” gas. Pressure is related to
temperature and density:
P = nkT
➔
Methods of Energy Transport
◆
Radiation Zone
●
Energy travels as photons of light, which continually collide with
particles
●
Always changing direction (
random walk
), photons can change
wavelengths
●
This is called
radiative diffusion
○
This is a slow process!
○
It takes about 10^5 years for energy to travel from the core to
the surface.
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➔
Methods of Energy Transport
◆
Convection Zone
●
Photons arriving at bottom of convection zone are absorbed instead
of scattered by matter
●
The bottom of the zone is heated…hot gases rise to the top
●
Cooler gas sinks to the bottom…just like when you boil a pot of
water!
●
Energy is brought to the surface via bulk motions of matter
(convection).
➔
The Sun’s Energy Source
◆
The first scientific theories involved chemical reactions or gravitational
collapse
◆
Development of nuclear physics led to the correct answer:
●
The Sun generates energy via nuclear fusion reactions.
●
Divide the amount of energy you have by the burn rate to get
seconds
◆
Chemical Energy Content / Luminosity ~ 10,000 years
➔
Energy needs to go somewhere
➔
Nuclear Fusion/Fission
◆
Fission: larger nucleus split into smaller nucleus
●
Take an atom and split it
◆
Fusion: Smaller nuclei combined into larger nucleus
●
Take two and combine them
◆
Both processes lose energy (fission) is done on Earth and is in a controlled
environment.
◆
Fusion is only used in non-controlled places, like a hydrogen bomb.
➔
Why does fusion occur in the Sun’s core?
◆
Nuclear fusion
●
A reaction where heavier nuclei are created by combining (fusing)
lighter nuclei.
●
All nuclei are positively charged
◆
Electromagnetic force causes nuclei to repel each other.
●
For fusion to occur, nuclei must be moving fast enough to overcome
E-M repulsion
●
This requires high temperatures and pressures (present in the core of
the Sun)
◆
When nuclei touch, the nuclear (strong) force binds them together.
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➔
Potential Energy of Matter Itself
◆
Energy is stored in matter itself
◆
This mass-energy is what would be released if an amount of mass, m, were
converted into energy
◆
E = mc^2
➔
{C = 3 x 10^8 m/s is the speed of light; m is in kg, then E is in Joules}
◆
{1 kg gives 10^17 joules}
➔
Effectively, 4 hydrogen nuclei are converted into 1 Helium nucleus and energy is
released.
➔
How does fusion release energy?
◆
Mass of 4 x 1 Hydrogen = 4 m sub(proton)
◆
Mass of 4He = 3.97mproton
◆
Net deficit of 0.03mptoron converted to energy (photons, KE of positrons
and neutrinos) since mass and energy are equivalent (E=mc^2)
●
Efficiency = delta (m)/m = 0.03/4 = 0.007
➔
How does fusion release energy?
◆
0.7% of mass of Hydrogen in Sun is converted into energy
◆
Total energy available Enuc = 0.007Mc^2 GO TO THE SLIDES FOR
THIS
◆
Nuclear lifetime = 10^11 years
◆
Sun lives about 10^10 years, about half-way through its lifetime.
Lecture 11 - February 10th, 2022
➔
Surveying the Stars
◆
Everything we know about stars deduced from light we receive
◆
Luminosity: Amount of power a star radiates (energy per second)
◆
The unit of power is 1 joule per second = 1 watt
➔
Apparent brightness (flux)
:
◆
Amount of starlight that reaches Earth - the energy per second per square
meter
◆
The unit of apparent brightness is:
1 Joule per second per square meter =
1 Watt / meter^2
◆
So, apparent brightness (flux) of a star depends on
luminosity and
distance
.
➔
Thought Question:
◆
These two stars have about the same luminosity -- which one appears
brighter?
●
Alpha Centauri
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●
The Sun
➔
Luminosity/App. Brightness of Stars
◆
Luminosity - the total amount of power radiated by a star into space.
◆
Apparent brightness or Flux refers to the amount of a star’s light which
reachus us per unit area
●
At distance, d, same luminosity is spread out over an invisible sphere
of increasing area with distance from source, A = 4pi(d)^2
●
The amount of luminosity per unit area decreases, the farther the star
is, so the fainter it appears, according to an inverse square law - i.e.,
its apparent brightness decreases as the (distance)^2.
◆
The apparent brightness (flux) of a star depends on two things:
●
How much light it is emitting: luminosity (L) [watts]
●
How far away it is: distance (d) [meters]
◆
Apparent Brightness
= Flux = L / (4pi(d)^2) in Units: Watts/m^2
➔
The relationship between apparent brightness and luminosity depends on distance:
◆
Apparent Brightness = Luminosity / 4pi (distance)^2
➔
We can determine a star’s luminosity if we can measure its distance and apparent
brightness:
◆
Luminosity = 4 pi (distance)^2 * (Apparent Brightness)
➔
Apparent brightness (energy received per unit time per unit area) is easily
measured with a photo-meter.
◆
Stellar brightness range is enormous so astronomers use a logarithmic scale
to compress the range or MAGNITUDE scale. The brightest stars in the sky
are “first” magnitude; fifth magnitude stars are 100x fainter.
➔
Thought Question
◆
How would the apparent brightness of Alpha Centauri change if it were
three times farther away?
●
It would be 1/9th as bright.
○
Because of the inverse square law
➔
Parallax
◆
D (parsecs) = 1/p (arcsecs)
●
1 parsec is the distance that gives a parallax angle of 1 second of arc
= 3.26 light years = 206265 AU
●
P can be as small as 0.01 arcsec. Nearest star has p = 0.7 arcsec.
How far away?
➔
How hot are stars?
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◆
Every object emits
thermal radiation
with a spectrum that depends on its
temperature
.
◆
The correct temperature of the Sun is the temperature of the photosphere.
◆
Once it gets to the photosphere it propogates out, kind of like skin
temperature.
➔
Laws of Thermal Radiation - BLACKBODY DIAGRAM
◆
Hotter objects emit more light at all wavelengths
●
Stefan-Boltzmann Law: Luminosity per square meter = constant x
T^4
●
Hotter objects emit light at shorter wavelengths (higher frequencies)
○
Wien’s Law: Temperature (K) = 2,900,000/wavelength (nm)
◆
See blackbody chart -
●
15,000 K star and above = ultraviolet
●
The Sun (5,800K) = Thermal
●
3,000 K star = infrared.
➔
Lines in a star’s spectrum correspond to a spectral type that reveals its
temperature. Spectral type (letter/number) is shorthand for temperature.
➔
Hottest
O
B
A
F
G
K
M
Coolest
◆
Remember that the Sun is like a G star, K and M are cooler stars.
➔
Mass
◆
Gravitationally bound stars
●
Two stars orbiting each other = binary
●
Binary stars yield stellar masses by Newton’s form of Kepler’s 3rd
Law.
◆
Types of Binary Star Systems
●
Visual binary
●
Eclipsing Binary
●
Spectroscopic Binary
◆
Note: About half of all stars are in binary systems.
➔
The mass ratio here is closer to one, so the radial velocity effect will be bigger.
◆
So, too, will the transit. So they are way easier to see.
◆
We can directly observe the orbital motions.
●
We can directly determine orbital periods, projected size, we don’t
know inclination of the plane of the orbit.
➔
Eclipsing Binary
◆
When one star passes in front of the other there is a change in brightness
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●
Inclination of the orbit is essentially zero (Edge-on), causing
eclipses.
◆
Periodic eclipses implies orbital period; duration gives RADIUS.
➔
Spectroscopic Binary
◆
No eclipses, but orbital motion causes a Doppler Effect in the spectrum
●
Star B spectrum at time 1: approaching, therefore blue shifted.
●
Star B spectrum at time 2: receding, therefore redshifted.
◆
Back and forth motion of lines is periodic; period = orbital period. From
Doppler shifts we get orbital velocity. Period and velocity is equivalent to
period and orbital radius.
➔
We measure mass using gravity.
◆
Newton’s Form of Kepler’s 3rd Law:
●
Direct mass measurements are possible only for stars in binary
star systems.
●
P^2 = 4pi^2 / G(M1 + M2) * a^3
○
P = period
○
A = average separation
●
If you only have p and a then you get M1 + M2, but if you have the
separate orbits then you can get M1 and M2 separately.
➔
How massive are stars?
◆
The range of stellar masses runs from 0.08 times the mass of the Sun to
about 100 times the mass of the Sun.
●
0.08 is the minimum mass for a star to ignite fusion
◆
Masses are only known for stars that form binary systems, but about half of
all stars are in fact in binary systems!
●
0.08M sun is ~~ 80 M jupiter
○
Objects LESS massive than 0.08Msun do exist; discovered in
1995 - called Brown Dwarfs.
➔
How Luminous are stars?
◆
The apparent brightness of a star in our sky depends on both its luminosity -
the total amount of light it emits to space - and its distance from Earth, as
expressed by the inverse square law for light
◆
The range of stellar masses runs from 0.08 times the mass of the Sun to
about 100 times the mass of the Sun.
◆
Masses are only known for stars that form binary systems, but about half of
all stars are in fact in binary systems!
➔
Most normal stars are fusing hydrogen into helium in their cores like the Sun.
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◆
Luminous normal stars are hot (blue)
◆
Less luminous ones are cooler (yellow or red)
➔
Stellar Luminosity/Radius
◆
Two stars can have the same temperature, but vastly different luminosities.
How does this happen?
◆
The Luminosity of a star depends on 2 things:
●
Surface temperature
(determines thermal flux, or power emitted
per unit area, i.e., (SEE SLIDES) sigma T^4)
●
Surface area (radius)
○
L = sigma T^4 * 4pi(R)^2
◆
Flux,
surface area
○
The stars have different sizes!
➔
A star’s
full classification
includes
spectral type
(temperature) and
luminosity
class
(related to the size of the star):
◆
I - supergiant
◆
II - bright giant
◆
III - giant
◆
IV - Subgiant
◆
V - main sequence
➔
Examples: Sun - G2 V
●
Sirius - A1 V
●
Proxima Centauri - M5.5 V
●
Betelgeuse - M2 I
◆
Measurements of the
shape
of spectral lines give
size
.
➔
Stellar Properties Review
◆
Luminosity
: From brightness and distance
●
(0.08Msun) 10^-4 Lsun - 10^6 Lsun (100 Msun)
○
The one on the left will burn longer, because, while is has less
fuel (0.08 Msun), it burns at a rate of only 10^-4 Lsun
◆
Temperature
: from color and spectral type
●
(0.08 Msun) 3,000 K - 50,000 K (100 Msun)
◆
Mass
: from period (p) and average separation (a) of binary-star orbit
●
0.08 M sun - 100 M sun
➔
Mass and Lifetime
◆
Star’s life expectancy: fuel/(rate at which fuel is used up)
◆
Sun’s life expectancy: 10 billion years → until core hydrogen (10% of
total) is used up.
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◆
Life expectancy of 10 Msun star:
●
10 times as much fuel, but it uses 10^4 times as fast.
●
10 million years ~ 10 billion years x 10 / 10^4
◆
Life expectancy of 0.1 Msun star:
●
0.1 times as much fuel, uses it 0.01 times as fast
●
100 billion years ~ 10 billion years x 0.1 / 0.01
➔
Normal Star Summary
◆
High Mass: high luminosity
●
Short-lived
●
Large radius
●
Blue
◆
Low Mass:
●
Low luminosity
●
Long-lived
●
Small radius
●
Red
➔
Luminosity (Y) as a function of Temperature (X)
◆
It is called a Hertzsprung-Russell Diagram
◆
It tells us everything in one picture!
➔
You see them neatly organized by their mass.
➔
Normal hydrogen-burning stars reside on the main sequence of the H-R diagram.
◆
Mass increases from lower right to upper left.
➔
Gravitational Equilibrium for each mass
◆
Which star is most like our Sun?
◆
Least massive stars C category will last the longest. Can live 100 billion
years
◆
Hotter temperature stars with more luminosity will live shorter. High mass
stars are short lived.
➔
How do we classify stars?
◆
We classify stars according to their
spectral type
and
luminosity class
.
◆
The spectral type tells us the star’s surface temperature.
◆
The luminosity class tells us how much light it puts out (surface area)
➔
Why is a star’s mass its most important property?
◆
A star’s
mass
at birth determines
virtually everything
that happens to it
throughout its life.
➔
What is a Hertzsprung-Russell (H-R) diagram?
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◆
An H-R diagram plots stars according to their surface temperatures and
luminosities.
●
Note: temperature is plotted backwards.
➔
Why are star clusters important?
◆
The cluster of stars formed at more or less the same time out of a giant
cloud that fragmented.
◆
Massive blue stars use up their fuel fastest and die first, followed by white
yellow, orange, and red stars. [we will explain later what it means for a star
to die. For now it means that it is no longer easily visible]
◆
We know the life cycle of each type of star, so look at the cluster to see
which types are present.
◆
The most massive star remaining on the Main Sequence determines the
Age. The cluster cannot be older than the lifetime of that star,
otherwise that star would have died and be missing from the Main
Sequence.
◆
Plot the H-R diagram of the cluster.
➔
Pleiades
now has no stars with life expectancy less than around 100 million years.
◆
Notice that the most massive stars remaining seem to
“turning off”
towards the giant region.
➔
Main-sequence turnoff point of a cluster tells us its age; the more hot, blue stars
there are, the younger it is.
◆
The older the cluster, the more red giants it has.
➔
Detailed modeling of the oldest globular clusters reveal that they are about 13
billion years old - much older than the Sun.
➔
What are the two types of star clusters?
◆
Open clusters contain up to several thousand stars and are found in the disk
of the Milky Way Galaxy
◆
Globular clusters contain hundreds of thousands of stars, all closely packed
together. They are found mainly in a “halo” around our galaxy.
➔
How do we measure the age of a star cluster?
◆
Because all of a cluster’s stars were born at the same time, we can measure
a cluster’s age by finding the
main sequence turnoff point
on an H-R
diagram of its stars.
◆
The cluster’s age is equal to the hydrogen-burning lifetime of the hottest,
most luminous stars that remain on the main sequence.
Lecture 12 - February 15, 2022
➔
Stellar Life Cycles
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➔
How do stars form?
◆
Stars are born in cold, giant, interstellar
molecular clouds
consisting
mostly of
hydrogen
molecules (H2).
◆
Stars form in places where gravity can overcome thermal pressure in a
cloud.
◆
The cloud heats up as gravity causes it to contract.
●
Conservation of energy
◆
Contraction can continue if thermal energy is radiated away.
◆
As gravity forces a cloud to become smaller, it begins to spin faster and
faster.
●
Conservation of angular momentum
➔
Angular momentum leads to:
◆
Rotation of the protostar Disk formation
●
And sometimes…
◆
Jets
from the proto-star or
◆
Fragmentation
into binary or multiple stars.
➔
Stages of Star formation on the H-R Diagram
◆
1. A protostar assembles from a collapsing cloud fragment. It is concealed
beneath a shroud of dusty gas.
◆
2. Protostar shrinks and heats as gravitational potential energy is converted
into thermal energy.
◆
3. Surface temperature rises when radiation becomes the dominant mode of
energy flow within the protostar
◆
4. The fusion rate increases until it balances the energy radiated from the
star’s surface.
◆
Once it gets into a stage of cold production of Helium it is stable.
➔
Proto-star to Main Sequence
◆
The large proto-star contracts and heats until its core temperature is
sufficient for hydrogen fusion.
◆
Contraction ends when the energy released by hydrogen fusion balances the
energy radiated from the surface.
◆
For a star like the Sun, this process takes 50 million years (less time for
more massive stars).
➔
Range of Star Masses
◆
Below 0.08 of the Mass of the Sun can not sustain fusion → therefore it is
not a real star. It is a failed star called BROWN DWARFS.
➔
What is a Brown Dwarf?
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◆
An object less massive than 0.08 Msun.
◆
Radiates mostly infrared light (T < 2000K)
◆
Has thermal energy from gravitational contraction, but no heat from fusion.
◆
Balance against gravity caused by pressure of “degenerate” (tightly packed)
electrons - independent of temperature - in core.
◆
Brown Dwarfs (they actually look magenta or red in color rather than
brown) are “failed stars that merely cool off after degeneracy pressure stops
gravitational contraction.
◆
They are only recently discovered and represent a link between small stars
and giant planets
➔
Life on the Main Sequence
◆
Where a star lands on the Main Sequence depends on its mass
●
O stars are most massive
●
M stars are least massive
◆
Main Sequence stars convert H → He in their cores.
◆
The star is stable, in balance.
●
Gravity vs. Pressure from heat provided by H fusion reactions.
●
Balance is what keeps it in its early stage for all that time
➔
Pressure vs. Gravity
◆
What happens when outward thermal pressure exceeds inward pull of
gravity?
●
Gas expands and cools
◆
What happens when inward pull of gravity exceeds outward thermal
pressure?
●
Gas contracts and heats up.
◆
The outward push of pressure precisely balances the inward pull of gravity.
Pressure is greatest deep in the Sun where the overlying weight is greatest.
➔
What happens when a star can no longer fuse hydrogen to helium in its core?
◆
Core shrinks and heats up.
➔
What happens as a star’s inert helium core starts to shrink and heat up?
◆
Hydrogen fuses in shell around core
●
Fusing helium is a harder problem than hydrogen. The Hydrogen left
around it also shrinks, that is reaches the temp that stars fusing
hydrogen before the core can reach the temperature it needs to start
fusing helium. So, before you compress helium to the center, you
compress remaining hydrogen in the shell.
●
The consequence for the outer layers of the star is expansion.
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➔
Expansion into a Giant
◆
When H in the core is exhausted, there is no internal energy source.
He
core
contracts and heats up
◆
H-fusion begins in shell surrounding He core, heats outer layers of star.
◆
Envelope expands and cools.
●
Star becomes first a subgiant and then a Red Giant
●
10 to 100 times the radius of the present Sun.
◆
Timescale: < 10^9 years.
➔
Helium Flash, Part 1
◆
As He core contracts, densities become extremely high.
◆
Densities so high that core doesn’t behave like regular gas (
where pressure
is proportional to density x temperature
). Gas is supported by
degeneracy pressure
.
◆
Pressure comes from trying to squeeze lots of electrons into small volume.
◆
Helium fusion begins with the helium flash, after which the star’s surface
shrinks and heats, making the star’s life track move downward and to the
left on the H-R diagram.
➔
Helium Flas, Part 2
◆
As more
He
“ash” from H-burning shell collects, He core also becomes
hotter.
◆
When core temperature reaches 10^8 K, fusion of Helium into Carbon
occurs
●
Degenerate gas lacks thermostat, so fusion is explosive
○
For a few minutes, energy output exceeds entire galaxy
●
Helium Flash
➔
Helium Fusion
◆
The He core contracts
until it heats to 10^8 K
●
He fusion begins (He → C)
●
Sometimes called the triple-alpha process
◆
3 He nuclei close to each other to form one Carbon nuclei + ENERGY
◆
He fusing into carbon core, meanwhile hydrogen-burning shell
➔
Helium-Burning Stars
◆
Helium burning stars neither shrink nor grow because thermostat is
temporarily fixed. Helium is fusing carbon in the core.
➔
What happens when the star’s core runs out of helium?
◆
Think in terms of our sun
◆
For more massive stars, the star might explode
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◆
But, the correct answer is: Helium fuses in a shell around the core.
➔
In a star like the Sun, the shrinking carbon core
never gets hot enough
(~600
million K) to
fuse
carbon
◆
The double shells burning helium to carbon and hydrogen to helium
generate enough heat to push away the outer layers of the star. The result is
a
planetary nebula
with a
white dwarf
at the center
◆
That little white dwarf is the remaining carbon in the center.
➔
Sun’s (and Earth’s) Fate
◆
Sun
gradually brightens on main-sequence for next 5 billion years.
●
3-4 billion years from now, Sun will be bright enough to cause
runaway greenhouse effect on Earth.
◆
In ~5 billion years, H in core is exhausted, core contracts, envelope expands
during
Red Giant
phase over hundreds of millions of years.
●
At this point, Earth’s surface will be heated to 1000K
◆
Helium flash, to horizontal branch: He core burning, H shell burning.
●
A little cooler on Earth.
◆
After ~ 100 million years: Second Red Giant Phase. Sun becomes ~ 1000
times more luminous than currently. He and H shell burning, C core.
●
Radius grows to almost 1 AU (near Earth’s orbit)
◆
After ~ 1 million years, Sun ejects its envelope; becomes planetary nebula.
●
Ejecta engulf Jupiter and Saturn
◆
Core revealed as white dwarf.
●
Size on Earth, but initially much hotter than present Sun; gradually
cools and gets dimmer.
➔
Life as a High-mass Star
◆
Early stages of main-sequence and post-main-sequence evolution are
similar to those of low-mass star:
●
Main sequence: H fuses to He in core
●
Red Supergiant: H fuses to He in shell around inert He core; the star
started off bigger and now becomes red supergiant
●
Helium Core Burning: He fuses to C in core (no flash this time)
➔
Hydrogen Fusion in High-Mass Stars
◆
CNO cycle is just another way to fuse H into He, using carbon, nitrogen,
and oxygen as catalysts.
◆
CNO cycle is main mechanism for H fusion in high mass stars because core
temperature is higher.
◆
Effectively 4 H nuclei go IN and 1 He nucleus plus energy comes OUT
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●
This is COMPLICATED! Just know that there is another way to
make helium from hydrogen.
➔
High-Mass Stars in the H-R diagram
◆
High-mass stars become red supergiants after core H runs out because they
start larger and generate more heat.
◆
The luminosity doesn’t change much because the cooling is compensated
by the growth in surface area.
◆
What does a horizontal track (left to right) in H-R diagram mean
physically?
➔
What’s Happening Inside?
◆
In massive stars that have evolved off the main sequence, with higher core
temperatures than lower-mass stars, helium-capture reactions and two
protons at a time to go from Carbon to Oxygen to Neon to Magnesium.
➔
Advanced nuclear burning occurs in multiple shells.
◆
For massive stars H → He takes several million years.
◆
Si → Fe takes ~ 1 day.
➔
How far can this go?
◆
Iron
(Fe) is a dead end for fusion because nuclear reactions involving iron
do not release energy by E = mc^2.
◆
(Fe has lowest mass per nuclear particle). You need to add energy to iron.
◆
Iron is the bottom of the tier
●
Fusion from hydrogen → iron. Fission from Iron ← Uranium
➔
In the iron core, electron degeneracy pressure goes away in the high mass star
because enormous temperatures and pressure force electrons to combine with
protons, making neutrons and neutrinos: “neutronization”
◆
Neutrons collapse to the center, forming a dense, small object called a
neutron star. Has the density of solid nucleus, with a mass of a star.
Collapses from 10,000 km down to 10 km in 0.1 sec.
◆
The neutrons can’t be stacked into one another, but they shrink dramatically
in abidance to Poley’s Principle.
➔
The rest of the star blows up in an enormous explosion - SUPERNOVA
◆
While the rest compresses extremely.
➔
What are the life stages of a high-mass star?
◆
A high-mass star lives a much shorter life than a low-mass star, fusing
hydrogen into helium via the CNO cycle. After exhausting its core
hydrogen, a high-mass star begins hydrogen shell burning and then goes
through a series of stages burning successively heavier elements. The
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furious rate of this fusion makes the star swell in size to become a
supergiant. When core consists of Fe, no more burning takes place. Core
crushed by gravity into neutron star…or black hole…along with supernova
explosion.
◆
Neutron stars collide and can create elements like gold, etc.
◆
Brown dwarfs keep shrinking, but white dwarfs stay constant.
●
The pressure is not high enough in a white dwarf for the electrons
and protons fuse to form neutrons.
●
In a neutron star, the electrons can’t survive by themselves, so they
form into neutrons.
➔
White Dwarfs
◆
White dwarfs are the remaining cores of dead stars like the Sun.
◆
The outer layers of the original star have been blown into a planetary
nebula during red giant phase.
◆
The carbon core (for a 1 Msun star) is very dense.
●
Electron degeneracy pressure
balances gravity.
●
No input source of energy (no fusion).
●
When fusion runs out, all of a sudden we don’t have any more
energy source or pressure to counterbalance gravity, so the core will
SHRINK.
➔
With no internal nuclear energy source, White Dwarfs (WD) cool off, and grow
dimmer with time until they become black.
◆
For a 1 Msun star the core ends up as carbon, leading to a carbon White
Dwarf; for a smaller mass star the core never fuses He to Carbon and so the
white dwarf is made of Helium.
➔
White Dwarfs
◆
1.0 Msun white dwarf
◆
Msun = 333,000 Mearth
◆
A white dwarf is about the same size as Earth!
◆
WD density = 333,000 x 5.5g/cc = 1.8 tons/cc~2000 kg/cc
●
A sugar cube of WD material would weigh 1.8 tons (a small truck)
on Earth!
➔
White Dwarf Pressure
◆
Pressure and temperature are normally related.
●
As you heat a balloon, it expands
●
Gas pressure increases
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◆
This
thermal pressure
dominates at low to moderate densities (main
sequence star)
◆
P=nkT
◆
In very dense,
degenerate
gas, quantum mechanics takes over. Different
kind of pressure,
degeneracy pressure
, prevents such a dense gas from
collapsing. The WD interior is not like a regular gas. Dense sea of electrons
between C nuclei.
◆
Pauli Exclusion principle
prevents electrons from occupying the same
quantum states.
●
The electrons cannot get on top of one another, electrons cannot all
have the same position and “quantum state” (fundamental
properties)
●
The denser the gas, the faster the electrons whiz around, the higher
the electron degeneracy pressure.
➔
White Dwarfs
◆
Degenerate matter responds differently to pressure.
◆
The more mass the star has, the
smaller
the star becomes!
●
Increased gravity makes the star denser
●
Greater density increases degeneracy pressure to balance gravity
➔
Shrinkage of White Dwarfs
◆
Quantum mechanics says that electrons in the same place cannot be in the
same “State.”
◆
Adding mass to a white dwarf increases its gravity, forcing electrons into a
smaller space.
◆
In order to avoid being in the same state some of the electrons need to
move faster.
◆
Is there a limit to how much you can shrink a white dwarf?
◆
Nothing can exceed the speed of light, but they need to compress at higher
and higher velocities, but there is no other way to release the pressure, so
when gravity releases the pressure, the white dwarf shrinks.
➔
The White Dwarf Limit
◆
Einstein’s theory of relativity says that nothing can move faster than light -
so that must be the limit.
◆
When electron speeds in a White Dwarf approach speed of light, electron
degeneracy pressure can no longer support the weight.
◆
Chandrasekhar found that this happens when a white dwarf’s mass reaches
1.4 Msun.
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●
This is the famous Chandrasekhar Limit. Supported by
observations of WD masses, which are <1.4 Msun.
➔
WDs with neighbors (i.e., supernova)
◆
Isolated white dwarf boring, simply cools forever (makes them good
“clocks”)
◆
White dwarfs in binary systems are more interesting.
●
If binary stars are close enough (<1 AU), mass transfer can occur.
➔
Accretion onto a white dwarf
◆
Most stars in multiple/binary systems. If two stars are close, and one
evolves off of main sequence, it can accrete from other one.
➔
Star loses mass, an accreditation disk around the white dwarf begins to occur.
◆
Supernova explosion as white dwarf grows to M ~ 1.4 M sun
➔
Type la (white dwarf) supernova
◆
Thermonuclear explosion of entire WD near Chandrasekhar mass limit,
uncontrolled fusion of carbon, with L ~ 6x10^9 L sun.
●
Undergoes nuclear fusion, luminosity billions of times that of the
sun for a small period of time.
◆
Since every Type la SuperNova progenitor is the same size (~1.4 solar
masses), they may be good
standard candles
for measuring distance.
●
It’s like a bomb going off ALWAYS with the same amount of
explosives.
◆
Standard candle
is an object with known constant luminosity (think about
why this works).
➔
TWO Types of Supernova!
◆
Massive star supernova: Neutron Star
●
Iron core of massive (~> 8 Msun) star exceeds White Dwarf mass
limit and collapses into a neutron star, causing a huge explosion of
outer layers of the star.
◆
White Dwarf supernova:
●
Carbon fusion
suddenly begins throughout the compact White
Dwarf in a binary system (There’s TWO STARS < 1AU apart) when
accretion (IT SUCKS THE OTHER ONE) takes its mass above the
1.4 Msun Chandrasekhar Limit. The result is an explosion called a
white dwarf supernova.
➔
Supernova Type: How can we tell?
◆
Light Curves differ
- i.e. the way the light fades with time.
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◆
Spectra differ
(exploding white dwarfs don’t have hydrogen absorption
lines because they are made of either carbon or helium). Indicate different
composition of ejected gas.
➔
One way to tell supernova types apart is with a
light curve
showing how
luminosity changes with time. Another is by studying the patterns of absorption
lines in their spectra.
➔
Neutron Stars
◆
A neutron “star” is the ball of neutrons left behind by a massive-star
supernova.
◆
Degeneracy pressure of neutrons supports a neutron star against gravity.
◆
When neutrons packed together, they need to get to higher velocities.
➔
When core mass > 1.4 M sun electron degeneracy pressure goes away because
electrons combine with protons, making neutrons and neutrinos
◆
Neutrons collapse to the center, forming a
neutron star
.
➔
Neutron Stars
◆
Neutron star about the same size as a small city (10 km) but more mass than
the Sun. A teaspoon of neutron materials weighs billions of tons on Earth!
◆
Neutron stars should be born rapidly rotating with a strong magnetic field.
Why?
◆
(most) neutron stars are too small to be visible directly at optical
wavelengths. How do we know that they exist?
➔
Pulsars: Evidence that NS exist
◆
Sources of radio waves.
◆
Radio pulses at regular intervals
◆
Periods from 0.001 to 10 seconds.
➔
In 1967, Jocelyn Bell discovered Vulpecula
◆
It was a sharp pulse which recurred every 1.3 sec
◆
They called it a pulsar
◆
Pulsars are rotating neutron stars that act like lighthouses
◆
Beams of intense radiation coming from the poles look like pulses as they
sweep by the Earth.
◆
The electromagnetic radiation is generated by electrons spiraling in a strong
magnetic field.
➔
A pulsar’s rotation axis is not aligned with magnetic poles.
➔
Why Pulsar’s Must be Neutron Stars
◆
Circumference of NS = 2pi (radius = 10km) ~ 60 km
◆
Spin rate of fast pulsars ~ 500 cycles per second
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◆
Surface rotation velocity ~ 30,000 km/s
●
~10% speed of light
●
< escape velocity from NS
◆
The fastest White Dwarf can spin is ~once per second.
●
Otherwise, it will break up because material at surface will be
moving faster than escape velocity.
◆
Anything less dense/compact than a NS would be torn to pieces.
◆
Older neutron star doesn’t rotate as fast bc of angular momentum
➔
Black Holes
➔
The Neutron Star Limit
◆
Quantum mechanics says that neutrons in the same place cannot be in the
same state (like electrons)
◆
Neutron degeneracy pressure can no longer support a neutron star against
gravity if the neutron mass exceeds about 3 M sun, i..e., end state of the
most massive (>20 Msun) stars.
◆
(Analagous to white dwarf limit)
●
Beyond the neutron star limit, no known force can resist the crush of
gravity.
●
As far as we know, gravity crushes all the matter into a single point
known as a singularity.
●
Black hole: region of space in which the matter is so dense that
nothing can escape from it, not even light. \
●
Mass and location
➔
Black Holes: Gravity’s Ultimate Victory
➔
Two main types of black holes:
◆
Stellar-mass black holes (formed from collapse of really masive (>20msun)
stars
◆
Supermassive black holes (exist at the cetners of galaxies) and can contain
up to ~Msun.
➔
ESCAPE VELOCITY
◆
Vescape = sqrt(2GM/r)
●
Earth: V esc = 11 km/s
●
Sun: V esc = 600km/s
◆
For fixed Mass, V esc increases as r decreases.
●
Denser objects require a GREATER ESCAPE VELOCITY
●
Think about this in terms of a dense-ass black hole.
➔
White Dwarf
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◆
M = 1.0 M sun
◆
R = 5800 km
◆
Vesc = 0.02c or 2% the speed of light.
➔
V esc of a Neutron Star
◆
M = 1.5 M sun
◆
R = 10km
◆
V esc = 0.7 c or 70% the speed of light
➔
Black Hole
◆
Suppose escape velocity was equal to the speed of light, c. For an object
with mass, M, and radius = R (sun), where this is the case:
◆
C = sqrt(2GM / Rs) OR Rs = 2GM / c^2, or also Rs = 3 M/Msun km
➔
Black Hole: region of space in which the matter is so dense that nothing can
escape from it, not even light
➔
How do we define the radius of a black hole?
◆
Singularity point to the event horizon, where nothing can escape (not even
light), this is Rs
➔
The “surface of black hole is the radius at which the escape velocity equals the
speed of light.
◆
This imaginary spherical surface is known as the event horizon
◆
The radius of the event horizon is known as the schwarzschild radius (Rs).
➔
When you get close to a black hole, and deeper into the gravitational field, time
slows down. You don’t realize that you are falling into it, and time slows down. If
you witness someone fall in, it appears as though it’s taking them forever to fall
down.
➔
Tidal forces would be lethal at M = 3 Msun. The force is trillions of times that
which raises the tides on the Earth.
➔
X-Ray Binary Systems
◆
Binary system consists of main-sequence star and unseen companion
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