Phys 321: Lecture 13 the Big Bang Theory
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1 Lecture 26
PHYS 445 Lecture 26 - Black-body radiation I 26 - 1 Lecture 26 - Black-body radiation I What's Important: · number density · energy density Text: Reif In our previous discussion of photons, we established that the mean number of photons with energy i is 1 n = (26.1) i eß i - 1 Here, the questions that we want to address about photons are: · what is their number density · what is their energy density · what is their pressure? Number density n Eq. (26.1) is written in the language of discrete states. The first thing we need to do is replace the sum by an integral over photon momentum states: 3 S i ® ò d p Of course, it isn't quite this simple because the density-of-states issue that we introduced before: for every spin state there is one phase space state for every h 3, so the proper replacement more like 3 3 3 S i ® (1/h ) ò d p ò d r The units now work: the left hand side is a number, and so is the right hand side. But this expression ignores spin - it just deals with the states in phase space. For every photon momentum, there are two ways of arranging its polarization (i.e., the orientation of its electric or magnetic field vectors): where the photon momentum vector is perpendicular to the plane. Thus, we have 3 3 3 S i ® (2/h ) ò d p ò d r. (26.2) Assuming that our system is spatially uniform, the position integral can be replaced by the volume ò d 3r = V. -
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A&A 561, L12 (2014) Astronomy DOI: 10.1051/0004-6361/201323020 & c ESO 2014 Astrophysics Letter to the Editor Possible structure in the GRB sky distribution at redshift two István Horváth1, Jon Hakkila2, and Zsolt Bagoly1,3 1 National University of Public Service, 1093 Budapest, Hungary e-mail: [email protected] 2 College of Charleston, Charleston, SC, USA 3 Eötvös University, 1056 Budapest, Hungary Received 9 November 2013 / Accepted 24 December 2013 ABSTRACT Context. Research over the past three decades has revolutionized cosmology while supporting the standard cosmological model. However, the cosmological principle of Universal homogeneity and isotropy has always been in question, since structures as large as the survey size have always been found each time the survey size has increased. Until 2013, the largest known structure in our Universe was the Sloan Great Wall, which is more than 400 Mpc long located approximately one billion light years away. Aims. Gamma-ray bursts (GRBs) are the most energetic explosions in the Universe. As they are associated with the stellar endpoints of massive stars and are found in and near distant galaxies, they are viable indicators of the dense part of the Universe containing normal matter. The spatial distribution of GRBs can thus help expose the large scale structure of the Universe. Methods. As of July 2012, 283 GRB redshifts have been measured. Subdividing this sample into nine radial parts, each contain- ing 31 GRBs, indicates that the GRB sample having 1.6 < z < 2.1differs significantly from the others in that 14 of the 31 GRBs are concentrated in roughly 1/8 of the sky. -
Lecture 17 : the Cosmic Microwave Background
Let’s think about the early Universe… Lecture 17 : The Cosmic ! From Hubble’s observations, we know the Universe is Microwave Background expanding ! This can be understood theoretically in terms of solutions of GR equations !Discovery of the Cosmic Microwave ! Earlier in time, all the matter must have been Background (ch 14) squeezed more tightly together ! If crushed together at high enough density, the galaxies, stars, etc could not exist as we see them now -- everything must have been different! !The Hot Big Bang This week: read Chapter 12/14 in textbook 4/15/14 1 4/15/14 3 Let’s think about the early Universe… Let’s think about the early Universe… ! From Hubble’s observations, we know the Universe is ! From Hubble’s observations, we know the Universe is expanding expanding ! This can be understood theoretically in terms of solutions of ! This can be understood theoretically in terms of solutions of GR equations GR equations ! Earlier in time, all the matter must have been squeezed more tightly together ! If crushed together at high enough density, the galaxies, stars, etc could not exist as we see them now -- everything must have been different! ! What was the Universe like long, long ago? ! What were the original contents? ! What were the early conditions like? ! What physical processes occurred under those conditions? ! How did changes over time result in the contents and structure we see today? 4/15/14 2 4/15/14 4 The Poetic Version ! In a brilliant flash about fourteen billion years ago, time and matter were born in a single instant of creation. -
The Reionization of Cosmic Hydrogen by the First Galaxies Abstract 1
David Goodstein’s Cosmology Book The Reionization of Cosmic Hydrogen by the First Galaxies Abraham Loeb Department of Astronomy, Harvard University, 60 Garden St., Cambridge MA, 02138 Abstract Cosmology is by now a mature experimental science. We are privileged to live at a time when the story of genesis (how the Universe started and developed) can be critically explored by direct observations. Looking deep into the Universe through powerful telescopes, we can see images of the Universe when it was younger because of the finite time it takes light to travel to us from distant sources. Existing data sets include an image of the Universe when it was 0.4 million years old (in the form of the cosmic microwave background), as well as images of individual galaxies when the Universe was older than a billion years. But there is a serious challenge: in between these two epochs was a period when the Universe was dark, stars had not yet formed, and the cosmic microwave background no longer traced the distribution of matter. And this is precisely the most interesting period, when the primordial soup evolved into the rich zoo of objects we now see. The observers are moving ahead along several fronts. The first involves the construction of large infrared telescopes on the ground and in space, that will provide us with new photos of the first galaxies. Current plans include ground-based telescopes which are 24-42 meter in diameter, and NASA’s successor to the Hubble Space Telescope, called the James Webb Space Telescope. In addition, several observational groups around the globe are constructing radio arrays that will be capable of mapping the three-dimensional distribution of cosmic hydrogen in the infant Universe. -
Measurement of the Cosmic Microwave Background Radiation at 19 Ghz
Measurement of the Cosmic Microwave Background Radiation at 19 GHz 1 Introduction Measurements of the Cosmic Microwave Background (CMB) radiation dominate modern experimental cosmology: there is no greater source of information about the early universe, and no other single discovery has had a greater impact on the theories of the formation of the cosmos. Observation of the CMB confirmed the Big Bang model of the origin of our universe and gave us a look into the distant past, long before the formation of the very first stars and galaxies. In this lab, we seek to recreate this founding pillar of modern physics. The experiment consists of a temperature measurement of the CMB, which is actually “light” left over from the Big Bang. A radiometer is used to measure the intensity of the sky signal at 19 GHz from the roof of the physics building. A specially designed horn antenna allows you to observe microwave noise from isolated patches of sky, without interference from the relatively hot (and high noise) ground. The radiometer amplifies the power from the horn by a factor of a billion. You will calibrate the radiometer to reduce systematic effects: a cryogenically cooled reference load is periodically measured to catch changes in the gain of the amplifier circuit over time. 2 Overview 2.1 History The first observation of the CMB occurred at the Crawford Hill NJ location of Bell Labs in 1965. Arno Penzias and Robert Wilson, intending to do research in radio astronomy at 21 cm wavelength using a special horn antenna designed for satellite communications, noticed a background noise signal in all of their radiometric measurements. -
Black Body Radiation
BLACK BODY RADIATION hemispherical Stefan-Boltzmann law This law states that the energy radiated from a black body is proportional to the fourth power of the absolute temperature. Wien Displacement Law FormulaThe Wien's Displacement Law provides the wavelength where the spectral radiance has maximum value. This law states that the black body radiation curve for different temperatures peaks at a wavelength inversely proportional to the temperature. Maximum wavelength = Wien's displacement constant / Temperature The equation is: λmax= b/T Where: λmax: The peak of the wavelength b: Wien's displacement constant. (2.9*10(−3) m K) T: Absolute Temperature in Kelvin. Emissive power The value of the Stefan-Boltzmann constant is approximately 5.67 x 10 -8 watt per meter squared per kelvin to the fourth (W · m -2 · K -4 ). If the radiation emitted normal to the surface and the energy density of radiation is u, then emissive power of the surface E=c u If the radiation is diffuse Emitted uniformly in all directions 1 E= 푐푢 4 Thermal radiation exerts pressure on the surface on which they are Incident. If the intensity of directed beam of radiations incident normally to The surface is I 퐼 Then Pressure P=u= 푐 If the radiation is diffused 1 P= 푢 3 The value of the constant is approximately 1.366 kilowatts per square metre. When the emissivity of non-black surface is constant at all temperatures and throughout the entire range of wavelength, the surface is called Gray Body. PROBLEMS 1. The temperature of a person’s skin is 350 C. -
Class 12 I : Blackbody Spectra
Class 12 Spectra and the structure of atoms Blackbody spectra and Wien’s law Emission and absorption lines Structure of atoms and the Bohr model I : Blackbody spectra Definition : The spectrum of an object is the distribution of its observed electromagnetic radiation as a function of wavelength or frequency Particularly important example… A blackbody spectrum is that emitted from an idealized dense object in “thermal equilibrium” You don’t have to memorize this! h=6.626x10-34 J/s -23 kB=1.38x10 J/K c=speed of light T=temperature 1 2 Actual spectrum of the Sun compared to a black body 3 Properties of blackbody radiation… The spectrum peaks at Wien’s law The total power emitted per unit surface area of the emitting body is given by finding the area under the blackbody curve… answer is Stephan-Boltzmann Law σ =5.67X10-8 W/m2/K4 (Stephan-Boltzmann constant) II : Emission and absorption line spectra A blackbody spectrum is an example of a continuum spectrum… it is smooth as a function of wavelength Line spectra: An absorption line is a sharp dip in a (continuum) spectrum An emission line is a sharp spike in a spectrum Both phenomena are caused by the interaction of photons with atoms… each atoms imprints a distinct set of lines in a spectrum The precise pattern of emission/absorption lines tells you about the mix of elements as well as temperature and density 4 Solar spectrum… lots of absorption lines 5 Kirchhoffs laws: A solid, liquid or dense gas produces a continuous (blackbody) spectrum A tenuous gas seen against a hot -
Peter Scicluna – Systematic Effects in Dust-Mass Determinations
The other side of the equation Systematic effects in the determination of dust masses Peter Scicluna ASIAA JCMT Users’ Meeting, Nanjing, 13th February 2017 Peter Scicluna JCMT Users’ Meeting, Nanjing, 13th February 2017 1 / 9 Done for LMC (Reibel+ 2012), SMC (Srinivasan+2016) Total dust mass ∼ integrated dust production over Hubble time What about dust destruction? Dust growth in the ISM? Are the masses really correct? The dust budget crisis: locally Measure dust masses in FIR/sub-mm Measure dust production in MIR Gordon et al., 2014 Peter Scicluna JCMT Users’ Meeting, Nanjing, 13th February 2017 2 / 9 What about dust destruction? Dust growth in the ISM? Are the masses really correct? The dust budget crisis: locally Measure dust masses in FIR/sub-mm Measure dust production in MIR Done for LMC (Reibel+ 2012), SMC (Srinivasan+2016) Total dust mass ∼ integrated dust production over Hubble time Gordon et al., 2014 Peter Scicluna JCMT Users’ Meeting, Nanjing, 13th February 2017 2 / 9 Dust growth in the ISM? Are the masses really correct? The dust budget crisis: locally Measure dust masses in FIR/sub-mm Measure dust production in MIR Done for LMC (Reibel+ 2012), SMC (Srinivasan+2016) Total dust mass ∼ integrated dust production over Hubble time What about dust destruction? Gordon et al., 2014 Peter Scicluna JCMT Users’ Meeting, Nanjing, 13th February 2017 2 / 9 How important are supernovae? Are there even enough metals yet? Dust growth in the ISM? Are the masses really correct? The dust budget crisis: at high redshift Rowlands et al., 2014 Measure -
The High Redshift Universe: Galaxies and the Intergalactic Medium
The High Redshift Universe: Galaxies and the Intergalactic Medium Koki Kakiichi M¨unchen2016 The High Redshift Universe: Galaxies and the Intergalactic Medium Koki Kakiichi Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Koki Kakiichi aus Komono, Mie, Japan M¨unchen, den 15 Juni 2016 Erstgutachter: Prof. Dr. Simon White Zweitgutachter: Prof. Dr. Jochen Weller Tag der m¨undlichen Pr¨ufung:Juli 2016 Contents Summary xiii 1 Extragalactic Astrophysics and Cosmology 1 1.1 Prologue . 1 1.2 Briefly Story about Reionization . 3 1.3 Foundation of Observational Cosmology . 3 1.4 Hierarchical Structure Formation . 5 1.5 Cosmological probes . 8 1.5.1 H0 measurement and the extragalactic distance scale . 8 1.5.2 Cosmic Microwave Background (CMB) . 10 1.5.3 Large-Scale Structure: galaxy surveys and Lyα forests . 11 1.6 Astrophysics of Galaxies and the IGM . 13 1.6.1 Physical processes in galaxies . 14 1.6.2 Physical processes in the IGM . 17 1.6.3 Radiation Hydrodynamics of Galaxies and the IGM . 20 1.7 Bridging theory and observations . 23 1.8 Observations of the High-Redshift Universe . 23 1.8.1 General demographics of galaxies . 23 1.8.2 Lyman-break galaxies, Lyα emitters, Lyα emitting galaxies . 26 1.8.3 Luminosity functions of LBGs and LAEs . 26 1.8.4 Lyα emission and absorption in LBGs: the physical state of high-z star forming galaxies . 27 1.8.5 Clustering properties of LBGs and LAEs: host dark matter haloes and galaxy environment . 30 1.8.6 Circum-/intergalactic gas environment of LBGs and LAEs . -
Blackbody Radiation
Blackbody Radiation PHY293, PHY324 - TWO WEIGHTS PHY294 - ONE WEIGHT RECOMENDED READINGS 1) R. Harris: Modern Physics, Ch.3, pp. 74-75; Ch.9, pp.384-85. Addison Wesley, 2008. 2) Daniel V. Schroeder: Introduction to Thermal Physics, Ch.7. Addison Wesley Longman Publishing, 2000. 3) PASCO Instruction Manual and Experiment Guide for the Blackbody Radiation at https://www.pasco.com/file_downloads/Downloads_Manuals/Black-Body-Light-Source- Basic-Optics-Manual-OS-8542.pdf 4) Marcello Carla: “Stefan–Boltzmann law for the tungsten filament of a light bulb: Revisiting the experiment”. Am. J. Phys. V. 81 (7), 2013. http://studenti.fisica.unifi.it/~carla/varie/Stefan-Boltzmann_law_in_a_light_bulb.pdf INTRODUCTION All material objects emit electromagnetic radiation at a temperature above absolute zero. The radiation represents a conversion of a body's thermal energy into electromagnetic energy, and is therefore called thermal radiation. Conversely all matter absorbs electromagnetic radiation to some degree. An object that absorbs all radiation falling on it at all wavelengths is called a blackbody. It is well known that when an object, such as a lump of metal, is heated, it glows; first a dull red, then as it becomes hotter, a brighter red, then bright orange, then a brilliant white. Although the brightness varies from one material to another, the color (strictly spectral distribution) of the glow is essentially universal for all materials, and depends only on the temperature. In the idealized case, this is known as blackbody, or cavity, radiation. At low temperatures, the wavelengths of thermal radiation are mainly in infrared. As temperature increases, objects begin to glow red. -
19. Big-Bang Cosmology 1 19
19. Big-Bang cosmology 1 19. BIG-BANG COSMOLOGY Revised September 2009 by K.A. Olive (University of Minnesota) and J.A. Peacock (University of Edinburgh). 19.1. Introduction to Standard Big-Bang Model The observed expansion of the Universe [1,2,3] is a natural (almost inevitable) result of any homogeneous and isotropic cosmological model based on general relativity. However, by itself, the Hubble expansion does not provide sufficient evidence for what we generally refer to as the Big-Bang model of cosmology. While general relativity is in principle capable of describing the cosmology of any given distribution of matter, it is extremely fortunate that our Universe appears to be homogeneous and isotropic on large scales. Together, homogeneity and isotropy allow us to extend the Copernican Principle to the Cosmological Principle, stating that all spatial positions in the Universe are essentially equivalent. The formulation of the Big-Bang model began in the 1940s with the work of George Gamow and his collaborators, Alpher and Herman. In order to account for the possibility that the abundances of the elements had a cosmological origin, they proposed that the early Universe which was once very hot and dense (enough so as to allow for the nucleosynthetic processing of hydrogen), and has expanded and cooled to its present state [4,5]. In 1948, Alpher and Herman predicted that a direct consequence of this model is the presence of a relic background radiation with a temperature of order a few K [6,7]. Of course this radiation was observed 16 years later as the microwave background radiation [8]. -
Lecture Notes 6 BLACK-BODY RADIATION and the EARLY HISTORY of the UNIVERSE
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.286: The Early Universe October 25, 2018 Prof. Alan Guth Lecture Notes 6 BLACK-BODY RADIATION AND THE EARLY HISTORY OF THE UNIVERSE INTRODUCTION: In Lecture Notes 3 and 4 we discussed the dynamics of Newtonian cosmology under the assumption that mass is conserved as the universe expands. In that case, since the physical volume is proportional to a3(t), the mass density ρ(t) is proportional to 1=a3(t). In these lecture notes we will extend our understanding to include the dynamical effects of electromagnetic and other forms of radiation. Electromagnetic radiation is intrinsically relativistic (v ≡ c!), so we need to begin by discussing the concepts of mass and energy in the context of relativity. According to special relativity, mass and energy are equivalent, with the conversion of units given by the famous formula, E = mc2 : (6.1) When one says that mass and energy are equivalent, one is saying that they are just two different ways of expressing precisely the same thing. The total energy of any system is equal to the total mass of the system | sometimes called the relativistic mass | times c2, the square of the speed of light. Although c2 is a large number in conventional units, one can still think of it concep- tually as being merely a unit conversion factor. For example, one can imagine measuring the mass/energy of an object in either grams or ergs, with 1 gram = 8:9876 × 1020 erg ; (6.2) where c2 = 8:9876 × 1020 cm2/s2. So one gram is a huge number of ergs.