Stars + Galaxies: Back of the Envelope Properties. David Spergel

Size: px
Start display at page:

Download "Stars + Galaxies: Back of the Envelope Properties. David Spergel"

Transcription

1 Stars + Galaxies: Back of the Envelope Properties David Spergel

2 Free-fall time (1) r = GM r 2 (2) r t = GM 2 r 2 (3) t free fall r3 GM 1 Gρ Free-fall time for neutron star is milliseconds (characteristic timescale for gravitational waves) Free-fall time for the Sun is 10 3 s (characteristic timescale for gravitational waves) Characteristic time for universe = Hubble Time

3 Cosmology (ȧ a ) 2 = 8π 3 Gρ t 2 Gρ

4 Kelvin-Helmholtz Time Time scale to radiate gravitational energy U = GM 2 /R t = GM 2 /RL 30 million years for the Sun Timescale for proto-star evolution

5 Einstein Time Time scale to radiate gravitational energy U = Mc 2 t = Mc 2 /L years for the Sun

6 Nuclear Energy U = Mc 2 t = Mc 2 /L Helium burning is 7 MeV nucleon Sun doesn t use all of the available fuel Lifetime ~ 1010 years Timescale

7 Nuclear Burning R = f(v)σ(v)dv v 2 exp ( m nv 2 ) S(E) 2kT E exp ( Z1 Z 2 e 2 ) hv

8 Stellar Structure Hydrostatic Equilibrium: Mass Conservation: Thermal Conduction: Equation of State: Energy Production:

9 Hydrostatic Equilibrium dp dr = GM(r) ρ R 2 Using ρ M /R 3, this implies p R = GM R 2 M R 3 = GM 2 R 5 Using ideal gas law, p = ρkt/µ, kt = GMµ R

10 Mass-Luminosity Relation dt dr = l(r) 3 κρ 4πr 2 16 σ B T 3 Using ρ M /R 3, this implies L = R 2T 3 ρ T R L M 3

11 Mass Luminosity Relation

12 Stellar Lifetimes t = ɛmc2 L t M 2 Massive Stars live short brilliant lives!

13 Stellar Populations Mass function: dn dm M 2.35 The lowest mass stars dominate the mass of a stellar population L(t) = Mmax (t) 0 M 2.35 L(M)dM = M 2.15 max(t) t 1.07 The most massive stars dominate the luminosity of a population

14 Radii and Temperature R M 0.9 L T 4 R 2 T L M R0.5

15 Spiral Arms

16 Later Stages of Stellar Evolution Red Giant Branch (RGB) Degenerate Core of Helium Envelope burning Hydrogen Helium Flash Horizontal Branch Core burning of Helium to Carbon Asymptotic Giant Branch (AGB) Degenerate Core of Carbon Envelope burning Helium

17 Fuel Consumption Thereom The contribution by any Post Main Sequence evolutionary phase to the total luminosity of a simple stellar population is proportional to the amount of nuclear fuel burned in that phase t HB t MS = L MS L HB U HB U MS L MS L HB E He C E H He

18 Degeneracy Pressure As a star burns H -> He, it leaves behind a degenerate gas supported by electron degeneracy pressure Nuclear burning cycles are alternated by period of rapid gravitational collapse Chandrasekhar Mass (maximum mass supported by degeneracy pressure) (followed by flashes)

19 Chandrasekhar Mass E G = GM 2 R When the electrons become relativistic, their total Fermi energy is approximately, ( ) E F = Ncp F = Nc = N 4/3 c x R = M 4/3 c m 4/3 p R Equating the two: ( ) 3/2 c 1 M ch = = M Pl 3 G m 2 p m 2 p

20 HR Diagram

21 Globular Cluster HR Diagram

22

23 Stellar Models MESA (Paxton et al. 2011, ApJS, 192, 3) mesa.sourceforge.net Can stably evolve stars through Helium flash, RGB and HB to White Dwarf

24 Dust and Gas Stars form in Molecular Clouds These clouds contain copious amounts of dust that absorb starlight (in the optical, UV and near IR) and reemit in the IR Dust grains are micron size and composed primarily of carbon and silicates

25 Dust Emission Electric Dipole Limit (Size << λ) σ abs λ 2 F ν ν 2 B ν (T ) ν 4

26 Galaxy Spectrum

27 Other Emission Processes Radio: Free-free emission Synchrotron emission Radio emission scales with synchrotron

28 X-ray UV VIS Near IR Mid IR Far IR Radio M81 D=3 Mpc

29 Galaxy Properties David Spergel

30

31 Tinker et al. 2008

32

33 Blanton et al Gyr burst

34 4000 Angstrom Break

35

36 Kauffmann et al. 2003

37 Galaxy Morphology

38 Spiral Galaxies Two parameter family: Luminosity and Surface Brightness Exponential distribution of stars Tully-Fisher Sanders and Verheijen 1998

39 Spiral Galaxy Formation Tidal torque generates solid body rotation in gas Gas cools and collapses to form a disk conserving angular momentum

40

41 Elliptical Galaxies R e effective radius I e mean surface brightness within eff. radius σ0 velocity dispersion log Dn = log Re log Ie

42 Black Hole Scaling Relation Gultekin et al. 2009

Stellar Evolution. Eta Carinae

Stellar Evolution. Eta Carinae Stellar Evolution Eta Carinae Evolution of Main Sequence Stars solar mass star: from: Markus Bottcher lecture notes, Ohio University Evolution off the Main Sequence: Expansion into a Red Giant Inner core

More information

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies?

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies? Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies? Temperature Determines the λ range over which the radiation is emitted Chemical Composition metallicities

More information

Lecture 7: Stellar evolution I: Low-mass stars

Lecture 7: Stellar evolution I: Low-mass stars Lecture 7: Stellar evolution I: Low-mass stars Senior Astrophysics 2018-03-21 Senior Astrophysics Lecture 7: Stellar evolution I: Low-mass stars 2018-03-21 1 / 37 Outline 1 Scaling relations 2 Stellar

More information

Stars and their properties: (Chapters 11 and 12)

Stars and their properties: (Chapters 11 and 12) Stars and their properties: (Chapters 11 and 12) To classify stars we determine the following properties for stars: 1. Distance : Needed to determine how much energy stars produce and radiate away by using

More information

Stellar Models ASTR 2110 Sarazin

Stellar Models ASTR 2110 Sarazin Stellar Models ASTR 2110 Sarazin Jansky Lecture Tuesday, October 24 7 pm Room 101, Nau Hall Bernie Fanaroff Observing the Universe From Africa Trip to Conference Away on conference in the Netherlands

More information

Stellar Evolution ASTR 2110 Sarazin. HR Diagram vs. Mass

Stellar Evolution ASTR 2110 Sarazin. HR Diagram vs. Mass Stellar Evolution ASTR 2110 Sarazin HR Diagram vs. Mass Trip to Conference Away on conference in the Netherlands next week. Molly Finn, TA, will be our guest lecturer Stellar Evolution ASTR 2110 Sarazin

More information

HR Diagram, Star Clusters, and Stellar Evolution

HR Diagram, Star Clusters, and Stellar Evolution Ay 1 Lecture 9 M7 ESO HR Diagram, Star Clusters, and Stellar Evolution 9.1 The HR Diagram Stellar Spectral Types Temperature L T Y The Hertzsprung-Russel (HR) Diagram It is a plot of stellar luminosity

More information

AST101 Lecture 13. The Lives of the Stars

AST101 Lecture 13. The Lives of the Stars AST101 Lecture 13 The Lives of the Stars A Tale of Two Forces: Pressure vs Gravity I. The Formation of Stars Stars form in molecular clouds (part of the interstellar medium) Molecular clouds Cold: temperatures

More information

(2) low-mass stars: ideal-gas law, Kramer s opacity law, i.e. T THE STRUCTURE OF MAIN-SEQUENCE STARS (ZG: 16.2; CO 10.6, 13.

(2) low-mass stars: ideal-gas law, Kramer s opacity law, i.e. T THE STRUCTURE OF MAIN-SEQUENCE STARS (ZG: 16.2; CO 10.6, 13. 6.1 THE STUCTUE OF MAIN-SEQUENCE STAS (ZG: 16.2; CO 10.6, 13.1) main-sequence phase: hydrogen core burning phase zero-age main sequence (ZAMS): homogeneous composition Scaling relations for main-sequence

More information

Structure and Evolution of Stars Lecture 19: White Dwarfs

Structure and Evolution of Stars Lecture 19: White Dwarfs Structure and Evolution of Stars Lecture 19: White Dwarfs Physical Properties of White Dwarfs - density-mass relationship - mass-radius relationship - Chandrasekhar limiting mass - Cooling of White Dwarfs

More information

7. The Evolution of Stars a schematic picture (Heavily inspired on Chapter 7 of Prialnik)

7. The Evolution of Stars a schematic picture (Heavily inspired on Chapter 7 of Prialnik) 7. The Evolution of Stars a schematic picture (Heavily inspired on Chapter 7 of Prialnik) In the previous chapters we have seen that the timescale of stellar evolution is set by the (slow) rate of consumption

More information

Astronomy 1 Fall 2016

Astronomy 1 Fall 2016 Astronomy 1 Fall 2016 Lecture11; November 1, 2016 Previously on Astro-1 Introduction to stars Measuring distances Inverse square law: luminosity vs brightness Colors and spectral types, the H-R diagram

More information

Review from last class:

Review from last class: Review from last class: Properties of photons Flux and luminosity, apparent magnitude and absolute magnitude, colors Spectroscopic observations. Doppler s effect and applications Distance measurements

More information

Star Formation and Protostars

Star Formation and Protostars Stellar Objects: Star Formation and Protostars 1 Star Formation and Protostars 1 Preliminaries Objects on the way to become stars, but extract energy primarily from gravitational contraction are called

More information

The physics of stars. A star begins simply as a roughly spherical ball of (mostly) hydrogen gas, responding only to gravity and it s own pressure.

The physics of stars. A star begins simply as a roughly spherical ball of (mostly) hydrogen gas, responding only to gravity and it s own pressure. Lecture 4 Stars The physics of stars A star begins simply as a roughly spherical ball of (mostly) hydrogen gas, responding only to gravity and it s own pressure. X-ray ultraviolet infrared radio To understand

More information

Introductory Astrophysics A113. Death of Stars. Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM

Introductory Astrophysics A113. Death of Stars. Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM Goals: Death of Stars Relation between the mass of a star and its death White dwarfs and supernovae Enrichment of the ISM Low Mass Stars (M

More information

Announcement: Quiz Friday, Oct 31

Announcement: Quiz Friday, Oct 31 Announcement: Quiz Friday, Oct 31 What is the difference between the giant, horizontal, and asymptotic-giant branches? What is the Helium flash? Why can t high-mass stars support themselves in hydrostatic

More information

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS Main Categories of Compact Systems Formation of Compact Objects Mass and Angular Momentum Loss Evolutionary Links to Classes of Binary Systems Future Work

More information

Stellar Evolution. Stars are chemical factories The Earth and all life on the Earth are made of elements forged in stars

Stellar Evolution. Stars are chemical factories The Earth and all life on the Earth are made of elements forged in stars Lecture 11 Stellar Evolution Stars are chemical factories The Earth and all life on the Earth are made of elements forged in stars A Spiral Galaxy (Milky Way Type) 120,000 ly A few hundred billion stars

More information

AST 101 Introduction to Astronomy: Stars & Galaxies

AST 101 Introduction to Astronomy: Stars & Galaxies AST 101 Introduction to Astronomy: Stars & Galaxies The H-R Diagram review So far: Stars on Main Sequence (MS) Next: - Pre MS (Star Birth) - Post MS: Giants, Super Giants, White dwarfs Star Birth We start

More information

UNIVERSITY OF SOUTHAMPTON

UNIVERSITY OF SOUTHAMPTON UNIVERSITY OF SOUTHAMPTON PHYS3010W1 SEMESTER 2 EXAMINATION 2014-2015 STELLAR EVOLUTION: MODEL ANSWERS Duration: 120 MINS (2 hours) This paper contains 8 questions. Answer all questions in Section A and

More information

Pre Main-Sequence Evolution

Pre Main-Sequence Evolution Stellar Astrophysics: Stellar Evolution Pre Main-Sequence Evolution The free-fall time scale is describing the collapse of the (spherical) cloud to a protostar 1/2 3 π t ff = 32 G ρ With the formation

More information

AST-1002 Section 0459 Review for Final Exam Please do not forget about doing the evaluation!

AST-1002 Section 0459 Review for Final Exam Please do not forget about doing the evaluation! AST-1002 Section 0459 Review for Final Exam Please do not forget about doing the evaluation! Bring pencil #2 with eraser No use of calculator or any electronic device during the exam We provide the scantrons

More information

THIRD-YEAR ASTROPHYSICS

THIRD-YEAR ASTROPHYSICS THIRD-YEAR ASTROPHYSICS Problem Set: Stellar Structure and Evolution (Dr Ph Podsiadlowski, Michaelmas Term 2006) 1 Measuring Stellar Parameters Sirius is a visual binary with a period of 4994 yr Its measured

More information

read 9.4-end 9.8(HW#6), 9.9(HW#7), 9.11(HW#8) We are proceding to Chap 10 stellar old age

read 9.4-end 9.8(HW#6), 9.9(HW#7), 9.11(HW#8) We are proceding to Chap 10 stellar old age HW PREVIEW read 9.4-end Questions 9.9(HW#4), 9(HW#4) 9.14(HW#5), 9.8(HW#6), 9.9(HW#7), 9.11(HW#8) We are proceding to Chap 10 stellar old age Chap 11 The death of high h mass stars Contraction of Giant

More information

dp dr = GM c = κl 4πcr 2

dp dr = GM c = κl 4πcr 2 RED GIANTS There is a large variety of stellar models which have a distinct core envelope structure. While any main sequence star, or any white dwarf, may be well approximated with a single polytropic

More information

Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012

Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012 Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012 Choose the answer that best completes the question. Read each problem carefully and read through all the answers.

More information

Comparing a Supergiant to the Sun

Comparing a Supergiant to the Sun The Lifetime of Stars Once a star has reached the main sequence stage of it life, it derives its energy from the fusion of hydrogen to helium Stars remain on the main sequence for a long time and most

More information

P M 2 R 4. (3) To determine the luminosity, we now turn to the radiative diffusion equation,

P M 2 R 4. (3) To determine the luminosity, we now turn to the radiative diffusion equation, Astronomy 715 Final Exam Solutions Question 1 (i). The equation of hydrostatic equilibrium is dp dr GM r r 2 ρ. (1) This corresponds to the scaling P M R ρ, (2) R2 where P and rho represent the central

More information

The Evolution of Low Mass Stars

The Evolution of Low Mass Stars The Evolution of Low Mass Stars Key Ideas: Low Mass = M < 4 M sun Stages of Evolution of a Low Mass star: Main Sequence star star star Asymptotic Giant Branch star Planetary Nebula phase White Dwarf star

More information

Stellar Evolution Stars spend most of their lives on the main sequence. Evidence: 90% of observable stars are main-sequence stars.

Stellar Evolution Stars spend most of their lives on the main sequence. Evidence: 90% of observable stars are main-sequence stars. Stellar Evolution Stars spend most of their lives on the main sequence. Evidence: 90% of observable stars are main-sequence stars. Stellar evolution during the main-sequence life-time, and during the post-main-sequence

More information

The distance modulus in the presence of absorption is given by

The distance modulus in the presence of absorption is given by Problem 4: An A0 main sequence star is observed at a distance of 100 pc through an interstellar dust cloud. Furthermore, it is observed with a color index B-V = 1.5. What is the apparent visual magnitude

More information

1.1 Motivation. 1.2 The H-R diagram

1.1 Motivation. 1.2 The H-R diagram 1.1 Motivation Observational: How do we explain stellar properties as demonstrated, e.g. by the H-R diagram? Theoretical: How does an isolated, self-gravitating body of gas behave? Aims: Identify and understand

More information

Guiding Questions. Stellar Evolution. Stars Evolve. Interstellar Medium and Nebulae

Guiding Questions. Stellar Evolution. Stars Evolve. Interstellar Medium and Nebulae Guiding Questions Stellar Evolution 1. Why do astronomers think that stars evolve? 2. What kind of matter exists in the spaces between the stars? 3. What steps are involved in forming a star like the Sun?

More information

Notes for Wednesday, July 16; Sample questions start on page 2 7/16/2008

Notes for Wednesday, July 16; Sample questions start on page 2 7/16/2008 Notes for Wednesday, July 16; Sample questions start on page 2 7/16/2008 Wed, July 16 MW galaxy, then review. Start with ECP3Ch14 2 through 8 Then Ch23 # 8 & Ch 19 # 27 & 28 Allowed Harlow Shapely to locate

More information

Star Death ( ) High Mass Star. Red Supergiant. Supernova + Remnant. Neutron Star

Star Death ( ) High Mass Star. Red Supergiant. Supernova + Remnant. Neutron Star Star Death High Mass Star Red Supergiant A star with mass between 8 M and 20 M will become a red supergiant and will subsequently experience a supernova explosion. The core of this star will have a mass

More information

Lifespan on the main sequence. Lecture 9: Post-main sequence evolution of stars. Evolution on the main sequence. Evolution after the main sequence

Lifespan on the main sequence. Lecture 9: Post-main sequence evolution of stars. Evolution on the main sequence. Evolution after the main sequence Lecture 9: Post-main sequence evolution of stars Lifetime on the main sequence Shell burning and the red giant phase Helium burning - the horizontal branch and the asymptotic giant branch The death of

More information

Life and Death of a Star. Chapters 20 and 21

Life and Death of a Star. Chapters 20 and 21 Life and Death of a Star Chapters 20 and 21 90 % of a stars life Most stars spend most of their lives on the main sequence. A star like the Sun, for example, after spending a few tens of millions of years

More information

Stellar Structure and Evolution

Stellar Structure and Evolution Stellar Structure and Evolution Achim Weiss Max-Planck-Institut für Astrophysik 01/2014 Stellar Structure p.1 Stellar evolution overview 01/2014 Stellar Structure p.2 Mass ranges Evolution of stars with

More information

Chapter 6: Stellar Evolution (part 1)

Chapter 6: Stellar Evolution (part 1) Chapter 6: Stellar Evolution (part 1) With the understanding of the basic physical processes in stars, we now proceed to study their evolution. In particular, we will focus on discussing how such processes

More information

Brock University. Test 1, February, 2017 Number of pages: 9 Course: ASTR 1P02 Number of Students: 480 Date of Examination: February 6, 2017

Brock University. Test 1, February, 2017 Number of pages: 9 Course: ASTR 1P02 Number of Students: 480 Date of Examination: February 6, 2017 Brock University Test 1, February, 2017 Number of pages: 9 Course: ASTR 1P02 Number of Students: 480 Date of Examination: February 6, 2017 Number of hours: 50 min Time of Examination: 18:00 18:50 Instructor:

More information

Stellar evolution Part I of III Star formation

Stellar evolution Part I of III Star formation Stellar evolution Part I of III Star formation The interstellar medium (ISM) The space between the stars is not completely empty, but filled with very dilute gas and dust, producing some of the most beautiful

More information

The Birth Of Stars. How do stars form from the interstellar medium Where does star formation take place How do we induce star formation

The Birth Of Stars. How do stars form from the interstellar medium Where does star formation take place How do we induce star formation Goals: The Birth Of Stars How do stars form from the interstellar medium Where does star formation take place How do we induce star formation Interstellar Medium Gas and dust between stars is the interstellar

More information

Physics 556 Stellar Astrophysics Prof. James Buckley. Lecture 9 Energy Production and Scaling Laws

Physics 556 Stellar Astrophysics Prof. James Buckley. Lecture 9 Energy Production and Scaling Laws Physics 556 Stellar Astrophysics Prof. James Buckley Lecture 9 Energy Production and Scaling Laws Equations of Stellar Structure Hydrostatic Equilibrium : dp Mass Continuity : dm(r) dr (r) dr =4πr 2 ρ(r)

More information

Stellar Death. Final Phases

Stellar Death. Final Phases Stellar Death Final Phases After the post-agb phase, the death of the star is close at hand. Function of Mass (For stars < ~ 4 solar masses) 1. Lowest mass stars will never have sufficient pressure and

More information

Evolutionary Status of Epsilon Aurigae

Evolutionary Status of Epsilon Aurigae September 3, 2010 Outline Background Material 1 Background Material Why we care about stellar evolution The HR Diagram 2 3 Why we care about evolutionary state Why we care about stellar evolution The HR

More information

ASTRONOMY II Spring 1995 FINAL EXAM. Monday May 8th 2:00pm

ASTRONOMY II Spring 1995 FINAL EXAM. Monday May 8th 2:00pm ASTRONOMY II - 79202 Spring 1995 FINAL EXAM Monday May 8th 2:00pm Name: You have three hours to complete this exam. I suggest you read through the entire exam before you spend too much time on any one

More information

5) What spectral type of star that is still around formed longest ago? 5) A) F B) A C) M D) K E) O

5) What spectral type of star that is still around formed longest ago? 5) A) F B) A C) M D) K E) O HW2 Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) The polarization of light passing though the dust grains shows that: 1) A) the dust grains

More information

Evolution from the Main-Sequence

Evolution from the Main-Sequence 9 Evolution from the Main-Sequence Lecture 9 Evolution from the Main-Sequence P. Hily-Blant (Master PFN) Stellar structure and evolution 2016-17 111 / 159 9 Evolution from the Main-Sequence 1. Overview

More information

LIFE CYCLE OF A STAR

LIFE CYCLE OF A STAR LIFE CYCLE OF A STAR First stage = Protostar PROTOSTAR Cloud of gas and dust many light-years across Gravity tries to pull the materials together Eventually, at the center of the ball of dust and gas,

More information

Review Questions for the new topics that will be on the Final Exam

Review Questions for the new topics that will be on the Final Exam Review Questions for the new topics that will be on the Final Exam Be sure to review the lecture-tutorials and the material we covered on the first three exams. How does speed differ from velocity? Give

More information

A1199 Are We Alone? " The Search for Life in the Universe

A1199 Are We Alone?  The Search for Life in the Universe ! A1199 Are We Alone? " The Search for Life in the Universe Instructor: Shami Chatterjee! Summer 2018 Web Page: http://www.astro.cornell.edu/academics/courses/astro1199/! HW2 now posted...! So far: Cosmology,

More information

Stellar Evolution - Chapter 12 and 13. The Lives and Deaths of Stars White dwarfs, neutron stars and black holes

Stellar Evolution - Chapter 12 and 13. The Lives and Deaths of Stars White dwarfs, neutron stars and black holes Stellar Evolution - Chapter 12 and 13 The Lives and Deaths of Stars White dwarfs, neutron stars and black holes During the early stages of a star formation the objects are called a protostars. The internal

More information

Brock University. Test 1, January, 2015 Number of pages: 9 Course: ASTR 1P02 Number of Students: 500 Date of Examination: January 29, 2015

Brock University. Test 1, January, 2015 Number of pages: 9 Course: ASTR 1P02 Number of Students: 500 Date of Examination: January 29, 2015 Brock University Test 1, January, 2015 Number of pages: 9 Course: ASTR 1P02 Number of Students: 500 Date of Examination: January 29, 2015 Number of hours: 50 min Time of Examination: 18:00 15:50 Instructor:

More information

What tool do astronomers use to understand the evolution of stars?

What tool do astronomers use to understand the evolution of stars? What tool do astronomers use to understand the evolution of stars? Groups indicate types of stars or stages in their evolution. What is plotted? How does an individual star move around the diagram? What

More information

Exam # 3 Tue 12/06/2011 Astronomy 100/190Y Exploring the Universe Fall 11 Instructor: Daniela Calzetti

Exam # 3 Tue 12/06/2011 Astronomy 100/190Y Exploring the Universe Fall 11 Instructor: Daniela Calzetti Exam # 3 Tue 12/06/2011 Astronomy 100/190Y Exploring the Universe Fall 11 Instructor: Daniela Calzetti INSTRUCTIONS: Please, use the `bubble sheet and a pencil # 2 to answer the exam questions, by marking

More information

Gravitational collapse of gas

Gravitational collapse of gas Gravitational collapse of gas Assume a gas cloud of mass M and diameter D Sound speed for ideal gas is c s = γ P ρ = γ nkt ρ = γ kt m Time for sound wave to cross the cloud t sound = D == D m c s γ kt

More information

Spiral Structure. m ( Ω Ω gp ) = n κ. Closed orbits in non-inertial frames can explain the spiral pattern

Spiral Structure. m ( Ω Ω gp ) = n κ. Closed orbits in non-inertial frames can explain the spiral pattern Spiral Structure In the mid-1960s Lin and Shu proposed that the spiral structure is caused by long-lived quasistatic density waves The density would be higher by about 10% to 20% Stars, dust and gas clouds

More information

Astronomy 104: Second Exam

Astronomy 104: Second Exam Astronomy 104: Second Exam Stephen Lepp October 29, 2014 Each question is worth 2 points. Write your name on this exam and on the scantron. Short Answer A The Sun is powered by converting hydrogen to what?

More information

The Later Evolution of Low Mass Stars (< 8 solar masses)

The Later Evolution of Low Mass Stars (< 8 solar masses) The Later Evolution of Low Mass Stars (< 8 solar masses) http://apod.nasa.gov/apod/astropix.html The sun - past and future central density also rises though average density decreases During 10 billion

More information

AST1002 Spring 2018 Final Exam Review Questions

AST1002 Spring 2018 Final Exam Review Questions AST1002 Spring 2018 Final Exam Review Questions Douglas H. Laurence Department of Physical Sciences, Broward College, Davie, FL 33314 Abstract This is a set of review questions for the upcoming midterm

More information

Scale height and Luminosity

Scale height and Luminosity The Milky Way I suggest to consult the excellent lectures held at Saas-Fee by Gilmore, King and van der Kruit in the Book The Milky Way as a Galaxy edited by Buser & King and published by the University

More information

Inhalt. Einführung JR. Urknall TS. Stellaratmosphere 3.7. TS. He-Verbrennung. r,rp, p Prozesse TS

Inhalt. Einführung JR. Urknall TS. Stellaratmosphere 3.7. TS. He-Verbrennung. r,rp, p Prozesse TS Inhalt Einführung 24.4. JR Grundlagen der Kernphysik 8.5. JR Urknall 15.5. TS Urknall-Nukleosynthese 29.5. JR Stellaratmosphere 3.7. TS H-Verbrennung 10.7. JR He-Verbrennung Supernova 17.77 TS r,rp, p

More information

Astronomy II (ASTR1020) Exam 3 Test No. 3D

Astronomy II (ASTR1020) Exam 3 Test No. 3D Astronomy II (ASTR1020) Exam 3 Test No. 3D 23 October 2001 The answers of this multiple choice exam are to be indicated on the Scantron with a No. 2 pencil. Don t forget to write your name and the Test

More information

Stellar Interiors - Hydrostatic Equilibrium and Ignition on the Main Sequence.

Stellar Interiors - Hydrostatic Equilibrium and Ignition on the Main Sequence. Stellar Interiors - Hydrostatic Equilibrium and Ignition on the Main Sequence http://apod.nasa.gov/apod/astropix.html Outline of today s lecture Hydrostatic equilibrium: balancing gravity and pressure

More information

Remember from Stefan-Boltzmann that 4 2 4

Remember from Stefan-Boltzmann that 4 2 4 Lecture 17 Review Most stars lie on the Main sequence of an H&R diagram including the Sun, Sirius, Procyon, Spica, and Proxima Centauri. This figure is a plot of logl versus logt. The main sequence is

More information

Why Do Stars Leave the Main Sequence? Running out of fuel

Why Do Stars Leave the Main Sequence? Running out of fuel Star Deaths Why Do Stars Leave the Main Sequence? Running out of fuel Observing Stellar Evolution by studying Globular Cluster HR diagrams Plot stars in globular clusters in Hertzsprung-Russell diagram

More information

The Death of Stars. Today s Lecture: Post main-sequence (Chapter 13, pages ) How stars explode: supernovae! White dwarfs Neutron stars

The Death of Stars. Today s Lecture: Post main-sequence (Chapter 13, pages ) How stars explode: supernovae! White dwarfs Neutron stars The Death of Stars Today s Lecture: Post main-sequence (Chapter 13, pages 296-323) How stars explode: supernovae! White dwarfs Neutron stars White dwarfs Roughly the size of the Earth with the mass of

More information

Astronomy Stars, Galaxies and Cosmology Exam 3. Please PRINT full name

Astronomy Stars, Galaxies and Cosmology Exam 3. Please PRINT full name Astronomy 132 - Stars, Galaxies and Cosmology Exam 3 Please PRINT full name Also, please sign the honor code: I have neither given nor have I received help on this exam The following exam is intended to

More information

Lecture 16: The life of a low-mass star. Astronomy 111 Monday October 23, 2017

Lecture 16: The life of a low-mass star. Astronomy 111 Monday October 23, 2017 Lecture 16: The life of a low-mass star Astronomy 111 Monday October 23, 2017 Reminders Online homework #8 due Monday at 3pm Exam #2: Monday, 6 November 2017 The Main Sequence ASTR111 Lecture 16 Main sequence

More information

Stellar Evolution: Outline

Stellar Evolution: Outline Stellar Evolution: Outline Interstellar Medium (dust) Hydrogen and Helium Small amounts of Carbon Dioxide (makes it easier to detect) Massive amounts of material between 100,000 and 10,000,000 solar masses

More information

Announcements. L! m 3.5 BRIGHT FAINT. Mass Luminosity Relation: Why? Homework#3 will be handed out at the end of this lecture.

Announcements. L! m 3.5 BRIGHT FAINT. Mass Luminosity Relation: Why? Homework#3 will be handed out at the end of this lecture. Announcements BRIGHT Homework#3 will be handed out at the end of this lecture. Due October 14 (next Thursday) Review of Mid-term exam will be handed out Tuesday. Mid-term exam will be variants (if not

More information

The Stars. Chapter 14

The Stars. Chapter 14 The Stars Chapter 14 Great Idea: The Sun and other stars use nuclear fusion reactions to convert mass into energy. Eventually, when a star s nuclear fuel is depleted, the star must burn out. Chapter Outline

More information

Supernovae and gamma- ray bursts

Supernovae and gamma- ray bursts Supernovae and gamma- ray bursts Supernovae Observa(ons: a star that temporarily becomes extremely bright, some:mes comparable to a whole galaxy Supernovae Supernovae Visible at very great distance (cosmology)

More information

Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 9

Phys 100 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 9 Phys 0 Astronomy (Dr. Ilias Fernini) Review Questions for Chapter 9 MULTIPLE CHOICE 1. We know that giant stars are larger in diameter than the sun because * a. they are more luminous but have about the

More information

Clicker Question: Clicker Question: What is the expected lifetime for a G2 star (one just like our Sun)?

Clicker Question: Clicker Question: What is the expected lifetime for a G2 star (one just like our Sun)? How Long do Stars Live (as Main Sequence Stars)? A star on Main Sequence has fusion of H to He in its core. How fast depends on mass of H available and rate of fusion. Mass of H in core depends on mass

More information

LIFE CYCLE OF A STAR

LIFE CYCLE OF A STAR LIFE CYCLE OF A STAR First stage = Protostar PROTOSTAR Cloud of gas and dust many light-years across Gravity tries to pull the materials together Eventually, at the center of the ball of dust and gas,

More information

Heading for death. q q

Heading for death. q q Hubble Photos Credit: NASA, The Hubble Heritage Team (STScI/AURA) Heading for death. q q q q q q Leaving the main sequence End of the Sunlike star The helium core The Red-Giant Branch Helium Fusion Helium

More information

The life of a low-mass star. Astronomy 111

The life of a low-mass star. Astronomy 111 Lecture 16: The life of a low-mass star Astronomy 111 Main sequence membership For a star to be located on the Main Sequence in the H-R diagram: must fuse Hydrogen into Helium in its core. must be in a

More information

Astro 1050 Fri. Apr. 10, 2015

Astro 1050 Fri. Apr. 10, 2015 Astro 1050 Fri. Apr. 10, 2015 Today: Continue Ch. 13: Star Stuff Reading in Bennett: For Monday: Finish Chapter 13 Star Stuff Reminders: Ch. 12 HW now on Mastering Astronomy, due Monday. Ch. 13 will be

More information

The Stellar Black Hole

The Stellar Black Hole The Stellar Black Hole Kenneth Dalton e-mail: kxdalton@yahoo.com Abstract A black hole model is proposed in which a neutron star is surrounded by a neutral gas of electrons and positrons. The gas is in

More information

Last time: looked at proton-proton chain to convert Hydrogen into Helium, releases energy.

Last time: looked at proton-proton chain to convert Hydrogen into Helium, releases energy. Last time: looked at proton-proton chain to convert Hydrogen into Helium, releases energy. Last time: looked at proton-proton chain to convert Hydrogen into Helium, releases energy. Fusion rate ~ Temperature

More information

LECTURE 1: Introduction to Galaxies. The Milky Way on a clear night

LECTURE 1: Introduction to Galaxies. The Milky Way on a clear night LECTURE 1: Introduction to Galaxies The Milky Way on a clear night VISIBLE COMPONENTS OF THE MILKY WAY Our Sun is located 28,000 light years (8.58 kiloparsecs from the center of our Galaxy) in the Orion

More information

Mass loss from stars

Mass loss from stars Mass loss from stars Can significantly affect a star s evolution, since the mass is such a critical parameter (e.g., L ~ M 4 ) Material ejected into interstellar medium (ISM) may be nuclear-processed:

More information

Distance Measuring Techniques and The Milky Way Galaxy

Distance Measuring Techniques and The Milky Way Galaxy Distance Measuring Techniques and The Milky Way Galaxy Measuring distances to stars is one of the biggest challenges in Astronomy. If we had some standard candle, some star with a known luminosity, then

More information

AST1100 Lecture Notes

AST1100 Lecture Notes AST1100 Lecture Notes 20: Stellar evolution: The giant stage 1 Energy transport in stars and the life time on the main sequence How long does the star remain on the main sequence? It will depend on the

More information

Age-redshift relation. The time since the big bang depends on the cosmological parameters.

Age-redshift relation. The time since the big bang depends on the cosmological parameters. Age-redshift relation The time since the big bang depends on the cosmological parameters. Lyman Break Galaxies High redshift galaxies are red or absent in blue filters because of attenuation from the neutral

More information

Protostars evolve into main-sequence stars

Protostars evolve into main-sequence stars Understanding how stars evolve requires both observation and ideas from physics The Lives of Stars Because stars shine by thermonuclear reactions, they have a finite life span That is, they fuse lighter

More information

Before proceeding to Chapter 20 More on Cluster H-R diagrams: The key to the chronology of our Galaxy Below are two important HR diagrams:

Before proceeding to Chapter 20 More on Cluster H-R diagrams: The key to the chronology of our Galaxy Below are two important HR diagrams: Before proceeding to Chapter 20 More on Cluster H-R diagrams: The key to the chronology of our Galaxy Below are two important HR diagrams: 1. The evolution of a number of stars all formed at the same time

More information

Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012

Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012 Astronomy 1504 Section 002 Astronomy 1514 Section 10 Midterm 2, Version 1 October 19, 2012 Choose the answer that best completes the question. Read each problem carefully and read through all the answers.

More information

S381 The Energetic Universe. Block 2 Nucleosynthesis and Stellar Remnants. Paul Ruffle

S381 The Energetic Universe. Block 2 Nucleosynthesis and Stellar Remnants. Paul Ruffle Sponsored by the Chemistry and Physics Societies of the Open University S381 The Energetic Universe Block 2 Nucleosynthesis and Stellar Remnants Paul Ruffle Visiting Research Fellow Astrophysics Research

More information

Chapter 17: Stellar Evolution

Chapter 17: Stellar Evolution Astr 2310 Thurs. Mar. 30, 2017 Today s Topics Chapter 17: Stellar Evolution Birth of Stars and Pre Main Sequence Evolution Evolution on and off the Main Sequence Solar Mass Stars Massive Stars Low Mass

More information

The Later Evolution of Low Mass Stars (< 8 solar masses)

The Later Evolution of Low Mass Stars (< 8 solar masses) The sun - past and future The Later Evolution of Low Mass Stars (< 8 solar masses) During 10 billion years the suns luminosity changes only by about a factor of two. After that though, changes become rapid

More information

Stellar Populations: Resolved vs. unresolved

Stellar Populations: Resolved vs. unresolved Outline Stellar Populations: Resolved vs. unresolved Individual stars can be analyzed Applicable for Milky Way star clusters and the most nearby galaxies Integrated spectroscopy / photometry only The most

More information

University of Naples Federico II, Academic Year Istituzioni di Astrofisica, read by prof. Massimo Capaccioli. Lecture 16

University of Naples Federico II, Academic Year Istituzioni di Astrofisica, read by prof. Massimo Capaccioli. Lecture 16 University of Naples Federico II, Academic Year 2011-2012 Istituzioni di Astrofisica, read by prof. Massimo Capaccioli Lecture 16 Stellar populations Walter Baade (1893-1960) Learning outcomes The student

More information

Supernovae, Neutron Stars, Pulsars, and Black Holes

Supernovae, Neutron Stars, Pulsars, and Black Holes Supernovae, Neutron Stars, Pulsars, and Black Holes Massive stars and Type II supernovae Massive stars (greater than 8 solar masses) can create core temperatures high enough to burn carbon and heavier

More information

Sunday, May 1, AGB Stars and Massive Star Evolution

Sunday, May 1, AGB Stars and Massive Star Evolution AGB Stars and Massive Star Evolution Iben The Helium Flash (< 2 Msun) The central core becomes dense enough, that degeneracy pressure dominates over thermal pressure. Still, the core radiates energy and

More information

20. Stellar Death. Interior of Old Low-Mass AGB Stars

20. Stellar Death. Interior of Old Low-Mass AGB Stars 20. Stellar Death Low-mass stars undergo three red-giant stages Dredge-ups bring material to the surface Low -mass stars die gently as planetary nebulae Low -mass stars end up as white dwarfs High-mass

More information

Stellar structure and evolution

Stellar structure and evolution Stellar structure and evolution Ulrike Heiter Uppsala University July 2012, Nordic-Baltic Summer School Outline 1. The lives of stars Overview of stellar evolution 2. Physics of stellar evolution Stellar

More information

The Virial Theorem for Stars

The Virial Theorem for Stars The Virial Theorem for Stars Stars are excellent examples of systems in virial equilibrium. To see this, let us make two assumptions: 1) Stars are in hydrostatic equilibrium 2) Stars are made up of ideal

More information