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Stars: Properties and Classification

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<strong>Stars</strong>:<br />

<strong>Properties</strong> <strong>and</strong><br />

<strong>Classification</strong>


Announcements<br />

n Homework # 5 starts today. Due Tuesday, Nov 15 th .<br />

n Grades for Quiz # 4 are available in the OWL<br />

Gradebook<br />

n In-class Exam # 2 will take place on Tuesday, Nov<br />

8 th .<br />

– Please check www.astro.umass.edu/~calzetti/astro100 for<br />

more infos


Assigned Reading<br />

n Units 52.1-2-3, 54.1-2-3, 55, 56, 57.1-3


Goals for the Day<br />

n To begin a study of stars – what theyre<br />

made of, what kinds are out there, how<br />

they are born, <strong>and</strong> how they die.<br />

Are all stars similar to our Sun?<br />

How far away are they?<br />

Where did they come from?<br />

What do they do?<br />

Do they live forever?<br />

How do they die?


n There are four principal characteristics<br />

of a star:<br />

– Luminosity<br />

– Surface Temperature<br />

– Size<br />

– Mass<br />

Three of them (luminosity, size, <strong>and</strong> mass) require<br />

knowledge of the distance of the star from us.


Stellar Parallax<br />

The measurements are taken six months apart.<br />

The baseline is the diameter of the Earth’s orbit.<br />

What is seen<br />

What is seen<br />

The ½ of the angle between the current location <strong>and</strong> the<br />

6-month location is called the stellar parallax = P.


1 (AU)<br />

D (in Parsecs) =<br />

P (in arcseconds)<br />

P, the parallax angle, is measured in arcseconds<br />

60 arcseconds = 1 arcminute<br />

60 arcminutes = 1 degree<br />

There are 3600 arcseconds in a degree<br />

The larger P, the smaller D<br />

The smaller P, the larger D<br />

1 parsec = 3.26 light years<br />

= 3.086x10 16 meter<br />

Parallax Distance


Parallax would be easier to measure if<br />

1) the stars were further away.<br />

2) Earth's orbit were larger.<br />

3) Earth moved backwards along its<br />

orbit.<br />

4) none of these.


Parallax would be easier to measure if<br />

1) the stars were further away.<br />

2) Earth's orbit were larger.<br />

3) Earth moved backwards along its<br />

orbit.<br />

4) none of these.


Star A has a parallax angle that is twice that<br />

of Star B. What is the relationship between<br />

their distances?<br />

n Star A is closer than Star B<br />

n Star B is closer than Star A<br />

n The stars are at the same distance<br />

n Not enough information is given


Luminosity<br />

Luminosity is the total amount of power given off by<br />

a star.<br />

- Since its a power, Luminosity is measured in Watts<br />

- For convenience, we often refer to the luminosity of<br />

a star in terms of the luminosity of the Sun.<br />

- Eg,<br />

- That star has a luminosity of 22L Sun <br />

- That galaxy has a luminosity of 2x10 12 L Sun


There is a Big Range of Stellar<br />

Luminosities Out there!<br />

Star<br />

Luminosity (in units<br />

of solar Luminosity)<br />

Sun 1<br />

Proxima Centauri 0.0006<br />

Rigel (Orion) 70,000<br />

Deneb (Cygnus) 170,000


The Sun radiates an enormous amount of energy<br />

(L Sun =4 x 10 26 Watts). Only about 10 -9 of this<br />

actually hits the Earth. Yet, the power of sunlight<br />

that illuminates a patch of desert 100 km x 100 km<br />

is equal to the total power consumption of the US.<br />

4 x 10 26 Watts radiated<br />

over entire surface<br />

~10 17 Watts striking<br />

the Earth<br />

4 x 10 26 Watts generated<br />

in core


Recall the inverse square law….


Brightness is different from Luminosity<br />

n Luminosity – the total amount of power being released<br />

from a star (this is an intrinsic property of the star).<br />

n Brightness – the power from that star that actually gets<br />

to us. This is the quantity we measure with a telescope.<br />

A <strong>Stars</strong> brightness depends on its distance from us.<br />

- there are stars much more luminous than our sun<br />

in the sky, however, they are not nearly as bright because<br />

they are far away.<br />

A stars apparent brightness B = luminosity<br />

4π (distance) 2 =<br />

L<br />

4π d 2


Surface Temperature<br />

n We determine a stars surface<br />

temperature by examining its blackbody<br />

emission (a.k.a. its continuous<br />

spectrum or color)<br />

n No information on distance is<br />

necessary!<br />

n For reference: the Suns surface<br />

(photosphere) temperature is 5,800 K


Surface Temperature


Another (more accurate) method to<br />

measure Temperatures in <strong>Stars</strong><br />

Using spectra (recall the Fraunhofer spectrum of the Sun):<br />

The `dark lines are created when the atoms in the photosphere<br />

have energy levels that match the photons that are emitted<br />

from the star.<br />

1. They `reveal the composition of the star.<br />

2. The strength of the lines (how `dark they are) depend on<br />

the stars surface temperature.


Spectral Types<br />

For historical<br />

reasons, astronomers<br />

classify the<br />

temperatures of stars<br />

on a scale defined by<br />

spectral types, called<br />

O B A F G K M L T,<br />

ranging from the<br />

hottest (type O) to<br />

the coolest (type M)<br />

stars.<br />

The Sun has spectral type G2


Stellar Size<br />

n <strong>Stars</strong> are very spherical so we<br />

characterize a stars size by its radius.<br />

R<br />

Stellar Radii vary in size<br />

from ~1500xR Sun for a<br />

large Red Giant to<br />

0.008xR Sun for a White<br />

Dwarf.


Use Temperature <strong>and</strong> Luminosity<br />

to Measure Size<br />

A stars luminosity, surface temperature, <strong>and</strong> size are all<br />

related by the Stefan-Boltzmann Law:<br />

A refresher: the Stefan-Boltzmann Law<br />

L=4πR 2 σT 4<br />

Luminosity<br />

Stellar<br />

radius<br />

Surface<br />

temperature


L=4πR 2 σT 4<br />

Survey Question<br />

Two stars have the same surface temperature, but<br />

the radius of one is 10 times the radius of the other.<br />

The larger star is<br />

1) 10 times more luminous<br />

2) 100 times more luminous<br />

3) 1000 times more luminous<br />

4) 1/10 th as luminous<br />

5) 1/100 th as luminous


L=4πR 2 σT 4<br />

Survey Question<br />

Suppose two stars are at equal distance <strong>and</strong> have the same<br />

radius, but one has a temperature that is twice as great as the<br />

other. The luminosity of the hotter star is ____ as<br />

the other.<br />

1) 1/2 as great<br />

2) 1/4 as great<br />

3) the same<br />

4) 4 times as great<br />

5) 16 times as great


L=4πR 2 σT 4<br />

Survey Question<br />

Suppose two stars are at equal distance <strong>and</strong> have the same<br />

radius, but one has a temperature that is twice as great as the<br />

other. The apparent brightness of the hotter star is ____ as<br />

the other.<br />

1) 1/2 as great<br />

2) 1/4 as great<br />

3) the same<br />

4) 4 times<br />

5) 16 times as great


Stellar <strong>Properties</strong> Survey Questions<br />

1) Luminosity 2) Radius<br />

3) Surface Temperature<br />

Question #1:<br />

Which property do we determine by first measuring<br />

the stars apparent brightness <strong>and</strong> distance?


Stellar <strong>Properties</strong> Survey Questions<br />

1) Luminosity 2) Radius<br />

3) Surface Temperature<br />

Question #2:<br />

Which property do we determine by measuring<br />

the wavelength of peak emission (i.e., its color)?


Mass: How do you measure the<br />

mass of a star?<br />

n Mass is the single most important<br />

property in determining how a stars life<br />

<strong>and</strong> death will proceed.<br />

n We can weigh stars that are in binary<br />

systems (two stars orbiting each other).<br />

Fortunately, most stars (about 70%) fall<br />

into this category.


Center of Mass (or Barycenter)<br />

n <strong>Stars</strong> orbiting<br />

each other orbit<br />

around their<br />

`center of mass<br />

or barycenter<br />

n They behave<br />

like children on a<br />

seesaw<br />

M a<br />

M b<br />

C.M.<br />

R b<br />

R a<br />

C.M. (center of mass) is where:<br />

R a M a = R b M b


Binary <strong>Stars</strong>: use the Generalized Keplers Third Law<br />

Star A<br />

- Binary stars are in orbit around<br />

each other.<br />

- They orbit around their C.M.<br />

C.M.<br />

R b<br />

R a<br />

- Their orbital period depends on<br />

their separation <strong>and</strong> their masses.<br />

Star B<br />

Generalized Keplers Third Law<br />

(M a +M b ) P 2 = a 3<br />

Keplers Third Law<br />

G/4π 2 M sun P 2 = a 3<br />

a= (R a +R b )/2<br />

Big P = Small Masses<br />

Small P = Big Masses


I. Visual Binaries


Summary<br />

n There are four principal characteristics<br />

of a star:<br />

– Luminosity (brightness <strong>and</strong> distance)<br />

– Surface Temperature (black-body spectrum)<br />

– Size (Stefan-Boltzmann Law)<br />

– Mass (generalized Keplers Third Law)<br />

Are these quantities related with each other?


Lets recall:<br />

Hydrostatic Equilibrium of <strong>Stars</strong><br />

Thermal<br />

Pressure<br />

Gravitational<br />

Contraction


Nuclear fusion rate<br />

rises dramatically<br />

The Stellar Thermostat<br />

Outward thermal pressure of core<br />

is larger than inward gravitational<br />

pressure<br />

Core exp<strong>and</strong>s<br />

Exp<strong>and</strong>ing core cools<br />

Contracting core heats up<br />

Nuclear fusion rate<br />

drops dramatically<br />

Core contracts<br />

Outward thermal pressure<br />

of core drops (<strong>and</strong> becomes<br />

smaller than inward grav. pressure)


What happens if we increase the<br />

mass of the star?<br />

n More mass = more gravitational<br />

contraction<br />

n = need for more balancing pressure =<br />

higher temperature at the center (<strong>and</strong><br />

on the surface)<br />

n Higher temperature = more hydrogen<br />

fusion = higher energy production =<br />

more luminous


Thus…<br />

n More massive =<br />

n Higher Temperature<br />

(bluer color) =<br />

n More luminous<br />

L ~ M 3.5<br />

A star 10 times more massive than the Sun is ~3000<br />

times more luminous!


The Hertzsprung-Russell Diagram


The Hertzsprung-Russell Diagram


The Hertzsprung-Russell Diagram<br />

The Main Sequence<br />

- all main sequence<br />

stars fuse H into He<br />

in their cores<br />

- this is the defining<br />

characteristic of a<br />

main sequence star.<br />

- more massive stars<br />

are more luminous <strong>and</strong><br />

hotter: L=4πR 2 σT 4


The Hertzsprung-Russell Diagram<br />

L=4πR 2 σT 4<br />

Red Giants<br />

- Red Giant stars<br />

are very large, cool<br />

<strong>and</strong> quite bright.<br />

Ex. Betelgeuse is<br />

100,000 times more<br />

luminous than the Sun<br />

but is only 3,500K on<br />

the surface. Its radius<br />

is 1,000 times that of the<br />

Sun.


The Hertzsprung-Russell Diagram


The Hertzsprung-Russell Diagram<br />

White Dwarfs<br />

- White Dwarfs<br />

are hot but since<br />

they are so small,<br />

they are not very<br />

luminous.<br />

L=4πR 2 σT 4


The Hertzsprung-Russell Diagram<br />

Mass of<br />

Star<br />

Size of Star

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