ASTRON 331 Astrophysics TEST 1 May 5, This is a closed-book test. No notes, books, or calculators allowed.

Similar documents
Cosmologists dedicate a great deal of effort to determine the density of matter in the universe. Type Ia supernovae observations are consistent with

Astro 242. The Physics of Galaxies and the Universe: Lecture Notes Wayne Hu

Gravitational Lensing. A Brief History, Theory, and Applications

Our Galaxy. Milky Way Galaxy = Sun + ~100 billion other stars + gas and dust. Held together by gravity! The Milky Way with the Naked Eye

Gravitational Efects and the Motion of Stars

Observational Cosmology

The Milky Way, Hubble Law, the expansion of the Universe and Dark Matter Chapter 14 and 15 The Milky Way Galaxy and the two Magellanic Clouds.

Structure of the Milky Way. Structure of the Milky Way. The Milky Way

REU Final Presentation

29:50 Stars, Galaxies, and the Universe Final Exam December 13, 2010 Form A

ASTR 200 : Lecture 22 Structure of our Galaxy

Microlensing (planet detection): theory and applications

Chapter 14 The Milky Way Galaxy

Survey of Astrophysics A110

Visible Matter. References: Ryden, Introduction to Cosmology - Par. 8.1 Liddle, Introduction to Modern Cosmology - Par. 9.1

The Gravitational Microlensing Planet Search Technique from Space

Our Galaxy. We are located in the disk of our galaxy and this is why the disk appears as a band of stars across the sky.

Brief update (3 mins/2 slides) on astrophysics behind final project

Astro Week 1. (a) Show that the transit duration for a non-central transit (see Figures) is: R R. b = a cos i

Relativity and Astrophysics Lecture 15 Terry Herter. RR Lyrae Variables Cepheids Variables Period-Luminosity Relation. A Stellar Properties 2

Chapter 23 The Milky Way Galaxy Pearson Education, Inc.

L2 point vs. geosynchronous orbit for parallax effect by simulations

BASICS OF GRAVITATIONAL LENSING

4. Structure of Dark Matter halos. Hence the halo mass, virial radius, and virial velocity are related by

80 2 Observational Cosmology L and the mean energy

Examination, course FY2450 Astrophysics Wednesday May 20, 2009 Time:

The Milky Way - Chapter 23

Aim: Understand equilibrium of galaxies

PHY323:Lecture 7 Dark Matter with Gravitational Lensing

4. Structure of Dark Matter halos. Hence the halo mass, virial radius, and virial velocity are related by

Number of Stars: 100 billion (10 11 ) Mass : 5 x Solar masses. Size of Disk: 100,000 Light Years (30 kpc)

AST1100 Lecture Notes

ASTRON 449: Stellar (Galactic) Dynamics. Fall 2014

Clusters: Observations

Chapter 10 Measuring the Stars

Searching for extrasolar planets using microlensing

Galaxies. The majority of known galaxies fall into one of three major classes: spirals (78 %), ellipticals (18 %) and irregulars (4 %).

ASTR 200 : Lecture 26. Gravitational Lensing

Clicker Question: Clicker Question: Clicker Question: Clicker Question: What is the remnant left over from a Type Ia (carbon detonation) supernova:

Microlensing Parallax with Spitzer

Remember from Stefan-Boltzmann that 4 2 4

Astronomy 114. Lecture 29: Internal Properties of Galaxies. Martin D. Weinberg. UMass/Astronomy Department

Examination paper for FY2450 Astrophysics

Astronomy A BEGINNER S GUIDE TO THE UNIVERSE EIGHTH EDITION

Gravitational microlensing. Exoplanets Microlensing and Transit methods

AST1100 Lecture Notes

Dark Matter. Galaxy Counts Redshift Surveys Galaxy Rotation Curves Cluster Dynamics Gravitational Lenses ~ 0.3 Ω M Ω b.

Lecture Outlines. Chapter 23. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

Stars: basic observations

Clusters of Galaxies Groups: Clusters poor rich Superclusters:

Astronomy 102: Stars and Galaxies Examination 3 April 11, 2003

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. Distances & the Milky Way. The Curtis View. Our Galaxy. The Shapley View 3/27/18

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. Dr. Joseph E. Pesce, Ph.D.

Charles Keeton. Principles of Astrophysics. Using Gravity and Stellar Physics. to Explore the Cosmos. ^ Springer

Exploring Dark Matter through Gravitational Lensing. Exploring the Dark Universe Indiana University June 2007

General Relativity. In GR, mass (or energy) warps the spacetime fabric of space.

Einführung in die Astronomie II

Chapter 19 Galaxies. Hubble Ultra Deep Field: Each dot is a galaxy of stars. More distant, further into the past. halo

Ay162, Spring 2006 Week 8 p. 1 of 15

Astro 242. The Physics of Galaxies and the Universe: Lecture Notes Wayne Hu

Gravitational Lensing

ASTRO 310: Galactic & Extragalactic Astronomy Prof. Jeff Kenney

1.1 Motivation. 1.2 The H-R diagram

Stellar Dynamics and Structure of Galaxies

Today in Astronomy 142: the Milky Way

Gravitational microlensing: an original technique to detect exoplanets

The cosmic distance scale

Our View of the Milky Way. 23. The Milky Way Galaxy

Measuring the Properties of Stars (ch. 17) [Material in smaller font on this page will not be present on the exam]

AS1001: Galaxies and Cosmology

Examination, course FY2450 Astrophysics Wednesday 23 rd May, 2012 Time:

Evidence for/constraints on dark matter in galaxies and clusters

Galaxies: The Nature of Galaxies

Gravitational Lensing: Strong, Weak and Micro

Ch. 25 In-Class Notes: Beyond Our Solar System

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Earth, Atmospheric, and Planetary Sciences Department. Quiz 2

Clusters of Galaxies Groups: Clusters poor rich Superclusters:

Astronomy 1 Fall 2016

THE GALAXY. Spitzer Space Telescope Images & Spectra: 3µm - 170µm

Astronomy 102: Stars and Galaxies Exam 2

Introduction to (Strong) Gravitational Lensing: Basics and History. Joachim Wambsganss Zentrum für Astronomie der Universität Heidelberg (ZAH/ARI)

The Milky Way Galaxy

Star systems like our Milky Way. Galaxies

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Quiz 2

Theoretical ideas About Galaxy Wide Star Formation! Star Formation Efficiency!

Neutron Stars. Chapter 14: Neutron Stars and Black Holes. Neutron Stars. What s holding it up? The Lighthouse Model of Pulsars

Astronomy 241: Review Questions #2 Distributed: November 7, 2013

AST1100 Lecture Notes

Test #2 results. Grades posted in UNM Learn. Along with current grade in the class

Exam 3 Astronomy 100, Section 3. Some Equations You Might Need

ASTRO 310: Galactic & Extragalactic Astronomy Prof. Jeff Kenney. Class 2 Jan 20, 2017 The Milky Way Galaxy: Stars in the Solar Neighborhood

Stars, Galaxies & the Universe Lecture Outline

Problem Set 2 Solutions

Ast 241 Stellar Atmospheres and Interiors

Results better than Quiz 5, back to normal Distribution not ready yet, sorry Correct up to 4 questions, due Monday, Apr. 26

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. Dr. Joseph E. Pesce, Ph.D.

Observational and modeling techniques in microlensing planet searches

BANG! Structure of a White Dwarf NO energy production gravity = degenerate gas pressure as it cools, becomes Black Dwarf. Lives of High Mass Stars

Stellar distances and velocities. ASTR320 Wednesday January 24, 2018

distribution of mass! The rotation curve of the Galaxy ! Stellar relaxation time! Virial theorem! Differential rotation of the stars in the disk

Transcription:

ASTRON 331 Astrophysics TEST 1 May 5, 2003 Name: This is a closed-book test. No notes, books, or calculators allowed. Orders of Magnitude (20 points): simply circle the correct answer. 1. The brightest supergiants, which have absolute magnitudes M V 6, can be seen with the naked eye out to a distance of about 12 AU 12 pc 0.5 kpc 2.5 kpc 2. A large telescope with an angular resolution of 0.1 is used to observe a binary system in which the two stars are orbiting each other at 10 AU. The maximum distance out to which the two stars in this binary system can be resolved by the telescope is about 1 pc 10 pc 100 pc 1 kpc 3. A typical 1 M red giant expands to a maximum radius of about 4. The age of the universe in seconds is about 1 R 10 R 1 AU 1 pc 1.2 10 23 4 10 17 2 10 10 3 10 7 5. Because of differential rotation in the Galactic disk, stars near the Sun in the direction of galactic longitute l 30 o have their spectra red shifted blue shifted absorbed horribly distorted 6. The characteristic luminosity L in the Schechter luminosity function is of order L 100 L 10 6 L 10 10 L 7. A large globular cluster contains about how many stars? 10 10 10 6 10 3 10 2 8. Gravity deflects starlight that just grazes the surface of Jupiter by about 20 mas 2 2 mas 2 o 9. The fraction of M c 2 that the Sun will radiate during its entire life as a star is of order 10 9 10 6 10 3 0.007 10. In a star cluster with velocity dispersion σ 30 km s 1, the distance of closest approach for strong encounters between solar-like stars is of order 1 AU 1 pc 1 R 10 km

Problem 1. Gravitational Potentials. (30 points) For each part of this problem it is crucial that you explain clearly your reasoning, using words and pictures as necessary. (a) Using Gauss s law, prove Newton s theorem about the gravitational potential inside a hollow spherical shell of matter. (b) Consider a mass distribution concentrated in a very long, thin, and straight filament with mass per unit length λ. (Examples could be cosmic strings or filaments in the large scale structure of the universe.) Derive an expression for the gravitational potential at a distance R from the filament. (c) In cylindrical coordinates (R, z) the potential of a Kuzmin disk is given by GM Φ K = [R 2 + (a K + z ) 2 ]. 1/2 Derive the expression for the corresponding surface mass density Σ K (R). (d) How would the surface gravity g = GM /R 2 at a point P on the surface of the Earth be changed if a hollow spherical cavity of radius R h were present at depth d just below this point? Take the center of the cavity to be at a distance d below the surface and on the radius from the center of the Earth to point P, with R h < d. Also assume that the density inside the Earth is a constant ρ = M /(4πR 3 /3).

Problem 2. Gravitational lensing. (30 points) Recall that the relation between the apparent angular position θ and the true position β of a gravitationally lensed star can be written where θ E is the Einstein radius, given by θ β = θ2 E θ, θ 2 E = 4GM c 2 d LS d L d S for a lens of mass M at distance d L ; the other two distances are the distance to the source, d S, and the distance from the lens to the source, d LS = d S d L. (a) Derive the expression for the total magnification M in the limit where β θ E. Explain clearly your reasoning in words and pictures. (b) For a stationary source derive an expression for the shape of the microlensing lightcurve (magnification as a function of time) of a strong event near its peak, for a MACHO moving through the Galactic halo with proper motion µ. Take t = 0 to be at the peak, where β = β 0 θ E for a strong microlensing event (with large magnification). (c) Estimate roughly the total duration of a microlensing event for MACHOs in our Galactic halo. Scale your result to (M/M ). If repeated photometric observations of each source star are done once per day, what limit does this set on the mass of MACHOs that could be detected? (Useful numbers: GM /c 2 1.5 km; 1 pc = 3 10 18 cm)

Problem 3. Dynamical Mass Estimates. (20 points) (a) From some of the data on satellites of the Milky Way in Table 4.1 of S&G (appended), obtain a dynamical mass estimate for our Galaxy, and calculate the corresponding massto-light ratio (M/L V in solar units). Explain how you would do a better job if you had more time. (b) Think carefully and list all the assumptions you had to make in part (a).

Additional space:

Additional space: