The Cosmic Distance Ladder – Student Guide Exercises the Cosmic Distance Ladder Module Consists of Material on Seven Different Distance Determination Techniques
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The Hubble Constant H0 --- Describing How Fast the Universe Is Expanding A˙ (T) H(T) = , A(T) = the Cosmic Scale Factor A(T)
Determining H0 and q0 from Supernova Data LA-UR-11-03930 Mian Wang Henan Normal University, P.R. China Baolian Cheng Los Alamos National Laboratory PANIC11, 25 July, 2011,MIT, Cambridge, MA Abstract Since 1929 when Edwin Hubble showed that the Universe is expanding, extensive observations of redshifts and relative distances of galaxies have established the form of expansion law. Mapping the kinematics of the expanding universe requires sets of measurements of the relative size and age of the universe at different epochs of its history. There has been decades effort to get precise measurements of two parameters that provide a crucial test for cosmology models. The two key parameters are the rate of expansion, i.e., the Hubble constant (H0) and the deceleration in expansion (q0). These two parameters have been studied from the exceedingly distant clusters where redshift is large. It is indicated that the universe is made up by roughly 73% of dark energy, 23% of dark matter, and 4% of normal luminous matter; and the universe is currently accelerating. Recently, however, the unexpected faintness of the Type Ia supernovae (SNe) at low redshifts (z<1) provides unique information to the study of the expansion behavior of the universe and the determination of the Hubble constant. In this work, We present a method based upon the distance modulus redshift relation and use the recent supernova Ia data to determine the parameters H0 and q0 simultaneously. Preliminary results will be presented and some intriguing questions to current theories are also raised. Outline 1. Introduction 2. Model and data analysis 3. -
AS1001: Galaxies and Cosmology Cosmology Today Title Current Mysteries Dark Matter ? Dark Energy ? Modified Gravity ? Course
AS1001: Galaxies and Cosmology Keith Horne [email protected] http://www-star.st-and.ac.uk/~kdh1/eg/eg.html Text: Kutner Astronomy:A Physical Perspective Chapters 17 - 21 Cosmology Title Today • Blah Current Mysteries Course Outline Dark Matter ? • Galaxies (distances, components, spectra) Holds Galaxies together • Evidence for Dark Matter • Black Holes & Quasars Dark Energy ? • Development of Cosmology • Hubble’s Law & Expansion of the Universe Drives Cosmic Acceleration. • The Hot Big Bang Modified Gravity ? • Hot Topics (e.g. Dark Energy) General Relativity wrong ? What’s in the exam? Lecture 1: Distances to Galaxies • Two questions on this course: (answer at least one) • Descriptive and numeric parts • How do we measure distances to galaxies? • All equations (except Hubble’s Law) are • Standard Candles (e.g. Cepheid variables) also in Stars & Elementary Astrophysics • Distance Modulus equation • Lecture notes contain all information • Example questions needed for the exam. Use book chapters for more details, background, and problem sets A Brief History 1860: Herchsel’s view of the Galaxy • 1611: Galileo supports Copernicus (Planets orbit Sun, not Earth) COPERNICAN COSMOLOGY • 1742: Maupertius identifies “nebulae” • 1784: Messier catalogue (103 fuzzy objects) • 1864: Huggins: first spectrum for a nebula • 1908: Leavitt: Cepheids in LMC • 1924: Hubble: Cepheids in Andromeda MODERN COSMOLOGY • 1929: Hubble discovers the expansion of the local universe • 1929: Einstein’s General Relativity • 1948: Gamov predicts background radiation from “Big Bang” • 1965: Penzias & Wilson discover Cosmic Microwave Background BIG BANG THEORY ADOPTED • 1975: Computers: Big-Bang Nucleosynthesis ( 75% H, 25% He ) • 1985: Observations confirm BBN predictions Based on star counts in different directions along the Milky Way. -
Measurements and Numbers in Astronomy Astronomy Is a Branch of Science
Name: ________________________________Lab Day & Time: ____________________________ Measurements and Numbers in Astronomy Astronomy is a branch of science. You will be exposed to some numbers expressed in SI units, large and small numbers, and some numerical operations such as addition / subtraction, multiplication / division, and ratio comparison. Let’s watch part of an IMAX movie called Cosmic Voyage. https://www.youtube.com/watch?v=xEdpSgz8KU4 Powers of 10 In Astronomy, we deal with numbers that describe very large and very small things. For example, the mass of the Sun is 1,990,000,000,000,000,000,000,000,000,000 kg and the mass of a proton is 0.000,000,000,000,000,000,000,000,001,67 kg. Such numbers are very cumbersome and difficult to understand. It is neater and easier to use the scientific notation, or the powers of 10 notation. For large numbers: For small numbers: 1 no zero = 10 0 10 1 zero = 10 1 0.1 = 1/10 Divided by 10 =10 -1 100 2 zero = 10 2 0.01 = 1/100 Divided by 100 =10 -2 1000 3 zero = 10 3 0.001 = 1/1000 Divided by 1000 =10 -3 Example used on real numbers: 1,990,000,000,000,000,000,000,000,000,000 kg -> 1.99X1030 kg 0.000,000,000,000,000,000,000,000,001,67 kg -> 1.67X10-27 kg See how much neater this is! Now write the following in scientific notation. 1. 40,000 2. 9,000,000 3. 12,700 4. 380,000 5. 0.017 6. -
Spectroscopy of Variable Stars
Spectroscopy of Variable Stars Steve B. Howell and Travis A. Rector The National Optical Astronomy Observatory 950 N. Cherry Ave. Tucson, AZ 85719 USA Introduction A Note from the Authors The goal of this project is to determine the physical characteristics of variable stars (e.g., temperature, radius and luminosity) by analyzing spectra and photometric observations that span several years. The project was originally developed as a The 2.1-meter telescope and research project for teachers participating in the NOAO TLRBSE program. Coudé Feed spectrograph at Kitt Peak National Observatory in Ari- Please note that it is assumed that the instructor and students are familiar with the zona. The 2.1-meter telescope is concepts of photometry and spectroscopy as it is used in astronomy, as well as inside the white dome. The Coudé stellar classification and stellar evolution. This document is an incomplete source Feed spectrograph is in the right of information on these topics, so further study is encouraged. In particular, the half of the building. It also uses “Stellar Spectroscopy” document will be useful for learning how to analyze the the white tower on the right. spectrum of a star. Prerequisites To be able to do this research project, students should have a basic understanding of the following concepts: • Spectroscopy and photometry in astronomy • Stellar evolution • Stellar classification • Inverse-square law and Stefan’s law The control room for the Coudé Description of the Data Feed spectrograph. The spec- trograph is operated by the two The spectra used in this project were obtained with the Coudé Feed telescopes computers on the left. -
PHAS 1102 Physics of the Universe 3 – Magnitudes and Distances
PHAS 1102 Physics of the Universe 3 – Magnitudes and distances Brightness of Stars • Luminosity – amount of energy emitted per second – not the same as how much we observe! • We observe a star’s apparent brightness – Depends on: • luminosity • distance – Brightness decreases as 1/r2 (as distance r increases) • other dimming effects – dust between us & star Defining magnitudes (1) Thus Pogson formalised the magnitude scale for brightness. This is the brightness that a star appears to have on the sky, thus it is referred to as apparent magnitude. Also – this is the brightness as it appears in our eyes. Our eyes have their own response to light, i.e. they act as a kind of filter, sensitive over a certain wavelength range. This filter is called the visual band and is centred on ~5500 Angstroms. Thus these are apparent visual magnitudes, mv Related to flux, i.e. energy received per unit area per unit time Defining magnitudes (2) For example, if star A has mv=1 and star B has mv=6, then 5 mV(B)-mV(A)=5 and their flux ratio fA/fB = 100 = 2.512 100 = 2.512mv(B)-mv(A) where !mV=1 corresponds to a flux ratio of 1001/5 = 2.512 1 flux(arbitrary units) 1 6 apparent visual magnitude, mv From flux to magnitude So if you know the magnitudes of two stars, you can calculate mv(B)-mv(A) the ratio of their fluxes using fA/fB = 2.512 Conversely, if you know their flux ratio, you can calculate the difference in magnitudes since: 2.512 = 1001/5 log (f /f ) = [m (B)-m (A)] log 2.512 10 A B V V 10 = 102/5 = 101/2.5 mV(B)-mV(A) = !mV = 2.5 log10(fA/fB) To calculate a star’s apparent visual magnitude itself, you need to know the flux for an object at mV=0, then: mS - 0 = mS = 2.5 log10(f0) - 2.5 log10(fS) => mS = - 2.5 log10(fS) + C where C is a constant (‘zero-point’), i.e. -
Cosmic Distance Ladder
Cosmic Distance Ladder How do we know the distances to objects in space? Jason Nishiyama Cosmic Distance Ladder Space is vast and the techniques of the cosmic distance ladder help us measure that vastness. Units of Distance Metre (m) – base unit of SI. 11 Astronomical Unit (AU) - 1.496x10 m 15 Light Year (ly) – 9.461x10 m / 63 239 AU 16 Parsec (pc) – 3.086x10 m / 3.26 ly Radius of the Earth Eratosthenes worked out the size of the Earth around 240 BCE Radius of the Earth Eratosthenes used an observation and simple geometry to determine the Earth's circumference He noted that on the summer solstice that the bottom of wells in Alexandria were in shadow While wells in Syene were lit by the Sun Radius of the Earth From this observation, Eratosthenes was able to ● Deduce the Earth was round. ● Using the angle of the shadow, compute the circumference of the Earth! Out to the Solar System In the early 1500's, Nicholas Copernicus used geometry to determine orbital radii of the planets. Planets by Geometry By measuring the angle of a planet when at its greatest elongation, Copernicus solved a triangle and worked out the planet's distance from the Sun. Kepler's Laws Johann Kepler derived three laws of planetary motion in the early 1600's. One of these laws can be used to determine the radii of the planetary orbits. Kepler III Kepler's third law states that the square of the planet's period is equal to the cube of their distance from the Sun. -
The Distance to NGC 1316 \(Fornax
A&A 552, A106 (2013) Astronomy DOI: 10.1051/0004-6361/201220756 & c ESO 2013 Astrophysics The distance to NGC 1316 (Fornax A): yet another curious case,, M. Cantiello1,A.Grado2, J. P. Blakeslee3, G. Raimondo1,G.DiRico1,L.Limatola2, E. Brocato1,4, M. Della Valle2,6, and R. Gilmozzi5 1 INAF, Osservatorio Astronomico di Teramo, via M. Maggini snc, 64100 Teramo, Italy e-mail: [email protected] 2 INAF, Osservatorio Astronomico di Capodimonte, salita Moiariello, 80131 Napoli, Italy 3 Dominion Astrophysical Observatory, Herzberg Institute of Astrophysics, National Research Council of Canada, Victoria BC V82 3H3, Canada 4 INAF, Osservatorio Astronomico di Roma, via Frascati 33, Monte Porzio Catone, 00040 Roma, Italy 5 European Southern Observatory, Karl–Schwarzschild–Str. 2, 85748 Garching bei München, Germany 6 International Centre for Relativistic Astrophysics, Piazzale della Repubblica 2, 65122 Pescara, Italy Received 16 November 2012 / Accepted 14 February 2013 ABSTRACT Aims. The distance of NGC 1316, the brightest galaxy in the Fornax cluster, provides an interesting test for the cosmological distance scale. First, because Fornax is the second largest cluster of galaxies within 25 Mpc after Virgo and, in contrast to Virgo, has a small line-of-sight depth; and second, because NGC 1316 is the single galaxy with the largest number of detected Type Ia supernovae (SNe Ia), giving the opportunity to test the consistency of SNe Ia distances both internally and against other distance indicators. Methods. We measure surface brightness fluctuations (SBF) in NGC 1316 from ground- and space-based imaging data. The sample provides a homogeneous set of measurements over a wide wavelength interval. -
The Distance to Andromeda
How to use the Virtual Observatory The Distance to Andromeda Florian Freistetter, ARI Heidelberg Introduction an can compare that value with the apparent magnitude m, which can be easily Measuring the distances to other celestial measured. Knowing, how bright the star is objects is difficult. For near objects, like the and how bright he appears, one can use moon and some planets, it can be done by the so called distance modulus: sending radio-signals and measure the time it takes for them to be reflected back to the m – M = -5 + 5 log r Earth. Even for near stars it is possible to get quite acurate distances by using the where r is the distance of the object parallax-method. measured in parsec (1 parsec is 3.26 lightyears or 31 trillion kilometers). But for distant objects, determining their distance becomes very difficult. From Earth, With this method, in 1923 Edwin Hubble we can only measure the apparant was able to observe Cepheids in the magnitude and not how bright they really Andromeda nebula and thus determine its are. A small, dim star that is close to the distance: it was indeed an object far outside Earth can appear to look the same as a the milky way and an own galaxy! large, bright star that is far away from Earth. Measuring the distance to As long as the early 20th century it was not Andrimeda with Aladin possible to resolve this major problem in distance determination. At this time, one To measure the distance to Andromeda was especially interested in determining the with Aladin, one first needs observational distance to the so called „nebulas“. -
The Distance Modulus in the Presence of Absorption Is Given by from Appendix 4 Table 3, We Have, for an A0V Star, Where the Magn
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 of the star? The distance modulus in the presence of absorption is given by mM–5= logd– 5 + A From Appendix 4 Table 3, we have, for an A0V star, M = 0.6 BV–0= where the magnitudes and absorption are in the visual (V) band. Therefore, the color excess is 1.5−0=1.5, and so A=3×1.5=4.5. This gives m==0.6+ 5log 100 – 5 + 4.5 10.1 for the apparent magnitude. Problem 3: Imagine that all of the Sun’s mass is concentrated in a thin spherical shell at the Sun’s radius. Imagine further that the Sun is powered by this mass slowly falling piece by piece into a black hole at the center of the sphere. If 100% of this energy is radiated away from the surface of the Sun, calculate the lifetime of the Sun, given its observed luminosity. Comment on your answer. If a small bit of mass ∆m falls from a radius r onto a radius R, then the energy released is given by GM∆m GM∆m GM∆m ∆E = – ------------------ –– ------------------ ≈ ------------------ r R R where, in this case, the black hole radius R is much smaller than the Sun’s radius r. 2 Using the Schwarzschild radius R=2GM/c for the black hole, we calculate the luminosity as ∆ E GM ∆ m 1 ∆ m L ==------- --------------------------- -------- =--- -------- c 2 ∆ t ()2GM ⁄c2∆ t 2 ∆ t This is precisely the same relationship used when we studied Cygnus X-1 and also appeared on the second class exam. -
Stellar Streams Discovered in the Dark Energy Survey
Draft version January 9, 2018 Typeset using LATEX twocolumn style in AASTeX61 STELLAR STREAMS DISCOVERED IN THE DARK ENERGY SURVEY N. Shipp,1, 2 A. Drlica-Wagner,3 E. Balbinot,4 P. Ferguson,5 D. Erkal,4, 6 T. S. Li,3 K. Bechtol,7 V. Belokurov,6 B. Buncher,3 D. Carollo,8, 9 M. Carrasco Kind,10, 11 K. Kuehn,12 J. L. Marshall,5 A. B. Pace,5 E. S. Rykoff,13, 14 I. Sevilla-Noarbe,15 E. Sheldon,16 L. Strigari,5 A. K. Vivas,17 B. Yanny,3 A. Zenteno,17 T. M. C. Abbott,17 F. B. Abdalla,18, 19 S. Allam,3 S. Avila,20, 21 E. Bertin,22, 23 D. Brooks,18 D. L. Burke,13, 14 J. Carretero,24 F. J. Castander,25, 26 R. Cawthon,1 M. Crocce,25, 26 C. E. Cunha,13 C. B. D'Andrea,27 L. N. da Costa,28, 29 C. Davis,13 J. De Vicente,15 S. Desai,30 H. T. Diehl,3 P. Doel,18 A. E. Evrard,31, 32 B. Flaugher,3 P. Fosalba,25, 26 J. Frieman,3, 1 J. Garc´ıa-Bellido,21 E. Gaztanaga,25, 26 D. W. Gerdes,31, 32 D. Gruen,13, 14 R. A. Gruendl,10, 11 J. Gschwend,28, 29 G. Gutierrez,3 B. Hoyle,33, 34 D. J. James,35 M. D. Johnson,11 E. Krause,36, 37 N. Kuropatkin,3 O. Lahav,18 H. Lin,3 M. A. G. Maia,28, 29 M. March,27 P. Martini,38, 39 F. Menanteau,10, 11 C. -
Astronomy General Information
ASTRONOMY GENERAL INFORMATION HERTZSPRUNG-RUSSELL (H-R) DIAGRAMS -A scatter graph of stars showing the relationship between the stars’ absolute magnitude or luminosities versus their spectral types or classifications and effective temperatures. -Can be used to measure distance to a star cluster by comparing apparent magnitude of stars with abs. magnitudes of stars with known distances (AKA model stars). Observed group plotted and then overlapped via shift in vertical direction. Difference in magnitude bridge equals distance modulus. Known as Spectroscopic Parallax. SPECTRA HARVARD SPECTRAL CLASSIFICATION (1-D) -Groups stars by surface atmospheric temp. Used in H-R diag. vs. Luminosity/Abs. Mag. Class* Color Descr. Actual Color Mass (M☉) Radius(R☉) Lumin.(L☉) O Blue Blue B Blue-white Deep B-W 2.1-16 1.8-6.6 25-30,000 A White Blue-white 1.4-2.1 1.4-1.8 5-25 F Yellow-white White 1.04-1.4 1.15-1.4 1.5-5 G Yellow Yellowish-W 0.8-1.04 0.96-1.15 0.6-1.5 K Orange Pale Y-O 0.45-0.8 0.7-0.96 0.08-0.6 M Red Lt. Orange-Red 0.08-0.45 *Very weak stars of classes L, T, and Y are not included. -Classes are further divided by Arabic numerals (0-9), and then even further by half subtypes. The lower the number, the hotter (e.g. A0 is hotter than an A7 star) YERKES/MK SPECTRAL CLASSIFICATION (2-D!) -Groups stars based on both temperature and luminosity based on spectral lines. -
The Distance to NGC 5128 (Centaurus A)
CSIRO PUBLISHING www.publish.csiro.au/journals/pasa Publications of the Astronomical Society of Australia, 2010, 27, 457–462 The Distance to NGC 5128 (Centaurus A) Gretchen L. H. HarrisA,D, Marina RejkubaB, and William E. HarrisC A Department of Physics and Astronomy, University of Waterloo, Waterloo ON, N2L 3G1, Canada B European Southern Observatory, Karl-Schwarzschild-Strasse 2, D-85748 Garching, Germany C Department of Physics and Astronomy, McMaster University, Hamilton ON, L8P 2X7, Canada D Corresponding author. Email: [email protected] Received 2009 September 24, accepted 2010 February 26 Abstract: In this paper we review the various high precision methods that are now available to determine the distance to NGC 5128. These methods include: Cepheids, TRGB (tip of the red giant branch), PNLF (planetary nebula luminosity function), SBF (surface brightness fluctuations), and Long Period Variable (LPV) Mira stars. From an evaluation of these methods and their uncertainties, we derive a best-estimate distance of 3.8 Æ 0.1 Mpc to NGC 5128 and find that this mean is now well supported by the current data. We also discuss the role of NGC 5128 more generally for the extragalactic distance scale as a testbed for the most direct possible comparison among these key methods. Keywords: Galaxies: distances and redshifts — galaxies: individual (NGC 5128) — galaxies: stellar content 1 Introduction the planetary nebula luminosity function (PNLF); surface An issue arising frequently in the literature on NGC 5128 brightness fluctuations (SBF); and long period variables is a lack of consensus about the best distance to adopt for (LPV/Miras). Below we briefly describe these methods to this important nearby elliptical galaxy.