e2 stellar radiation

60
E2. Stellar Radiation & Stellar Types IB Physics Power Points Option E Astrophysics www.pedagogics.ca

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Page 1: E2 stellar radiation

E2. Stellar Radiation

& Stellar Types

IB Physics Power Points

Option E

Astrophysics

www.pedagogics.ca

Page 2: E2 stellar radiation

E.2.1 State that fusion is the main energy source

of stars

The source of all energy in stars is hydrogen “burning”.

TWO fusion reaction pathways for hydrogen (which

pathway occurs depends on core temperature of the

star)

1. proton-proton chain – in stars like our Sun (core

temperature < 16 x 106 K)

2. carbon-nitrogen-oxygen (CNO) cycle (hotter core

temperatures) - not in the syllabus

Page 3: E2 stellar radiation

Energy release in fusion comes from mass defect in the

fusion reaction (products have less mass than reactants)

The proton-proton chain consists of three steps (each

step liberates energy)

Overall

MeV) (12.85 H H He He He .3

MeV) (5.49 He H H .2

MeV) (1.19 ν e H H H .1

1

1

1

1

4

2

3

2

3

2

3

2

2

1

1

1

0

1

2

1

1

1

1

1

1 4 0

1 2 14 2 2 H He e

Page 4: E2 stellar radiation
Page 5: E2 stellar radiation

Practice Problem

Determine the energy (in Joules) released in the

following reaction:

n He H H 1

0

3

2

2

1

2

1

Given the following nuclide masses

Deuteron = 2.015 u

Helium-3 = 3.017 u click for solution

Neutron = 1.009 u(1.009 3.017) 2(2.015)

0.004

0.004 931.5

3.73 MeV

m

E

E

Page 6: E2 stellar radiation

As a result of fusion, stars lose mass! The rate of

mass loss by our Sun to fusion reactions is about

4.33 × 109 kg s-1.

Estimate the power output of our Sun.

click for solution

2

9 2

26

(for 1 second)

(4.33 10 )

3.90 10 W

E mc

E c

E

Page 7: E2 stellar radiation

Star Stability

E.2.2 Explain that in a stable star (for example, our Sun) there

is an equilibrium between radiation pressure and

gravitational pressure.

In stars . . .

An outward force exists due to emitted radiation “pressure”

(the energy emitted by fusion reactions)

Gravity pulls the outer part of the star inward towards the

core.

In a stable star these two forces are a balanced equilibrium

Page 8: E2 stellar radiation

Nature of core changes as star ages

Page 9: E2 stellar radiation

Observing Stars – Key Characteristics

There are six principle characteristics used to describe

stars. They are:

1. Luminosity

2. Temperature

3. Radius

4. Mass

5. Chemical composition

6. Age

STUDY TIP: Stellar characteristics are often measured indirectly (like

using brightness to determine luminosity, or peak wavelength to

find surface temperature) AND these characteristics are often

mathematically interrelated.

Page 10: E2 stellar radiation

Luminosity and Brightness

Luminosity (L) is an absolute value that measures the

total power radiated by a star (in all directions).

• Luminosity is measured in watts

• our Sun has a luminosity of about 3.90 x 1026 W.

Luminosity is very important in providing information

about star structure and age.

E.2.3 Define the luminosity of a star

Page 11: E2 stellar radiation

Luminosity and Brightness

E.2.4 Define apparent brightness and state how it is

measured.

Apparent brightness (l) is a relative value.

• we measure apparent star brightness as the fraction

of the luminosity received by us.

• brightness is measured in watts per square meter.

Page 12: E2 stellar radiation

Apparent brightness is proportional to the

luminosity L of the star.

Apparent brightness is inversely proportional to

the square of the distance d between the star

and the observer.

24

Lb

d

Apparent brightness b depends on two variables:

Page 13: E2 stellar radiation

This can be misleading . . . .

This means that a brighter star is not necessarily closer

to Earth, or larger, or hotter.

A high luminosity star that is farther

from Earth can appear brighter.

Page 14: E2 stellar radiation

What you can conclude . . . .

For two stars the same distance from Earth, the star

with the greatest luminosity will appear brighter.

Note: both the surface

temperature and size of a

star affect luminosity.

Page 15: E2 stellar radiation

E.2.5 Apply the Stefan-Boltzmann law to compare

the luminosities of different stars.

The Stefan-Boltzmann law states:

4

8 2 4

Total Power Radiated

5.67 10

surface surfaceA T

where Wm K

NOTE:

Total Power Radiated = LUMINOSITY

Surface area of a sphere 24A r

Page 16: E2 stellar radiation

Sample problem: F1 (c) M02 exam

Antares A has a surface temperature of 3000 K and is part of

a binary star system. The companion star Antares B has a

surface temperature of 15 000 K and a luminosity that is

1/40 of that of Antares A. Calculate the ratio of the radius

of Antares A to Antares B.

Click for solution

STUDY TIP: Many problems are encountered like the one above

where the answer is a ratio of two variables. Get used to

working with variables and not always looking for a “plug and

chug” type of solution strategy.

Page 17: E2 stellar radiation

2 42 4

2 4 2 4

18 2 13 2

use Stefan-Boltzmann Law40

(4 )(4 )

40

40 (15000) (3000)

2.025 10 8.1 10

160 (2 SF)

AB

A AB B

B A

B A

A

B

LL

r Tr T

r r

r r

r

r

Page 18: E2 stellar radiation

E.2.6 State Wien’s (displacement) law and apply it to explain

the connection between the color and temperature of stars.

The color of a star is determined by the intensity of the

wavelengths of visible light emitted by the star.

Recall – in the visible spectrum

RED light (longer wavelength, lower frequency)

VIOLET light (shorter wavelength, higher frequency)

Page 19: E2 stellar radiation

Peak wavelength emission

gives an idea of surface

temperature.

The shorter the peak

wavelength, the hotter

the blackbody.

A star’s emission spectra is similar to a

theoretical blackbody spectra

Page 20: E2 stellar radiation

Wein’s displacement law relates the peak wavelength

(in metres) of an emission spectrum to surface

temperature (in Kelvin).

shorter peak wavelength = higher surface temperature.

Determine the surface temperature of our Sun if the

peak wavelength is 500 nm. Click for solution

3

max a constant (2.9 10 )surfaceT m K

3

9

2.9 105800 K

500 10T

Page 21: E2 stellar radiation

E.2.7 Explain how atomic spectra may be used to

deduce chemical and physical data for stars

Stellar Spectra – Star Data

Recall: what important characteristic of stars can be

estimated from stellar spectra? Click for answer

In addition, wavelengths missing from stellar spectra

indicate chemical nature of the outer layers of a star. Think

resonance, and relate this idea to greenhouse gases.

Surface temperature can be

determined from peak wavelength

Page 22: E2 stellar radiation

E.2.7 Explain how atomic spectra may be used to

deduce chemical and physical data for stars

Stellar Spectra – Star Data

Recall: what important characteristic of stars can be

estimated from stellar spectra? Click for answer

In addition, wavelengths missing from stellar spectra

indicate chemical nature of the outer layers of a star. Think

resonance, and relate this idea to greenhouse gases.

Page 23: E2 stellar radiation
Page 24: E2 stellar radiation

5 minute physics concept – the Doppler Effect

If a wave source is moving towards or away from an

observer, what the observer detects depends on their

position relative to the wave source.

Surface temperature can be

determined from peak wavelength

Page 25: E2 stellar radiation

Applied to stellar spectra

Red shifts in the position of absorption lines indicate

motion away from us

Blue shifts indicate motion towards us

Page 26: E2 stellar radiation

Class Surface Temp. K Colour

O 28000 - 50000 Blue

B 9900 - 28000 Blue-white

A 7400 - 9900 White

F 6000 - 7400 Yellow-white

G 4900 - 6000 Yellow

K 3500 - 4900 Orange

M 2000 - 3500 Orange-red

E.2.8

Describe the overall classification system of spectral classes

Oh be a fine girl/guy, kiss me!

Page 27: E2 stellar radiation
Page 28: E2 stellar radiation

E.2.9 Describe the different types of stars

Stellar Spectra – Star Data

Ursa Major : The Big Dipper

Page 29: E2 stellar radiation
Page 30: E2 stellar radiation

Mizar

Page 31: E2 stellar radiation

Types of Stars – Binary Stars

- two stars in orbit about their mutual centre of mass

Visual binary stars can be distinguished as separate stars

using a telescope.

Page 32: E2 stellar radiation

Spectroscopic Binary Stars

- identified by spectral analysis – look at absorption lines

- spectral frequency of each star will shift depending on

orbit position.

A B

A B

A

B

A + B

B A

B A

Blue Red

Page 33: E2 stellar radiation

Interpreting Spectrum Shifts – The Doppler Effect

A higher frequency than the source is observed if the source

is approaching the observer i.e. a BLUE SHIFT.

If the light source is receding from the observer, a RED SHIFT

is observed.

The “shift” in wavelength can be used to

determine the speed the source is

travelling.

ref

v c

Page 34: E2 stellar radiation

observer

Page 35: E2 stellar radiation

observer

AB

Page 36: E2 stellar radiation

A

B

Page 37: E2 stellar radiation

observer

Page 38: E2 stellar radiation

Sample problem: F2 M02 exam

20 days

Day 6 and 26 are at the same phase of the cycle.

On Day 6, the lines in the spectra from Star A are

red shifted (right) and those for Star B are blue

shifted (left)

B A

B A

Day 6

A

B

B + A

Day 1

Page 39: E2 stellar radiation

Sample problem: F2 M02 exam

Circular or elliptical orbits drawn around the centre of

mass.

Star spectra shifts towards blue when moving towards

Earth and towards red when moving away. As one star

is moving towards Earth while the other moves away, a

red shift in a binary system is always accompanied by a

blue shift.

No shift occurs when stars are moving perpendicular to

Earth.

Page 40: E2 stellar radiation

Mass of star / system

5 -10.261.74 10 ms

448.3ref

v c c

Page 41: E2 stellar radiation
Page 42: E2 stellar radiation

In an eclipsing binary system, the binary brightness shows

regular variation. This occurs because one star gets between

the other and the observer blocking some of the emitted

radiation.

Eclipsing Binaries

Page 43: E2 stellar radiation

Eclipsing binary information gives astronomers information

about orbital period and the separation of the stars.

Page 44: E2 stellar radiation

Background information - apparent brightness

Page 45: E2 stellar radiation

A Hertzsprung-Russell diagram is a

plot of luminosity against surface

temperature.

The Hertzsprung-Russell Diagram

Page 46: E2 stellar radiation

When plotted this way, a diagonal band appears that

contains the majority of stars. These are called main

sequence stars.

main sequence stars

• are stable

• derive their energy from hydrogen fusion.

• comprise 90% of stars visible in the night sky

The two fundamental factors that determine a star's

position in the main sequence its mass and

evolutionary state.

Page 47: E2 stellar radiation

20 days

Low luminosity,

high temperature

dwarf stars

high luminosity,

low temperature

giant starsHigh mass

short life

low mass

long life

Page 48: E2 stellar radiation
Page 49: E2 stellar radiation

L

Apparent

brightness if

10 pc away

Page 50: E2 stellar radiation

L

Apparent

brightness if

10 pc away

Page 51: E2 stellar radiation

L

Apparent

brightness if

10 pc away

Page 52: E2 stellar radiation

L

Page 53: E2 stellar radiation
Page 54: E2 stellar radiation

Practice Problem 1

A parsec (pc) is a unit of distance (see Data Booklet)

Page 55: E2 stellar radiation

Practice Problem 1

A parsec (pc) is a unit of distance (see Data Booklet)

Page 56: E2 stellar radiation

Practice Problem 2

Suppose that the distances to two nearby stars can be

reasonably estimated and this data, together with

measured apparent brightness suggests that the two

stars have a similar luminosity. The peak wavelength for

one star is 700 nm (reddish) while for the other it is 350

nm (bluish). Determine a) the surface temperature of

each star and b) how much larger one star is than the

other.

Page 57: E2 stellar radiation
Page 58: E2 stellar radiation

Summary

Luminosity is the total power output of a star. Luminosity

can measured as a absolute value (in Watts) or relative to

the Sun (in L

where L

= 3.90 x 1026 W)

Apparent brightness (or intensity) is a relative value and

represents the portion (measured in W m-2) of a star’s

luminosity that is observed on Earth. Apparent brightness,

stellar distance and luminosity are related by:

24

Lb

d

Page 59: E2 stellar radiation

Stars emit a radiation spectrum similar to that of a

theoretical black-body. This allows the surface temperature

of a star to be estimated from the peak wavelength in a

spectrum using Wien’s Law

The temperature can be related to the luminosity

and size of a star using the Stefan-Boltzmann Law

Recalling that

4

8 2 4

L

5.67 10

surface surfaceA T

where Wm K

3

max 2.9 10surfaceT m K

24surfaceA r

Page 60: E2 stellar radiation

Stellar spectra are very important for a number of reasons

1. Most peak wavelength indicates surface temperature

(and color of star)

2. The area under a stellar spectrum is an indication of total

power emitted i.e. luminosity.

3. Absorption lines in stellar spectra give an indication of

what elements are present in the atmosphere of the star

and therefore an idea of what fusion reactions are taking

place (helps with star age etc)

4. Stellar spectra give us important information about

binaries