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The Ptolemaic System Claudius Ptolemy
Putting it All Together: The Ptolemaic System Claudius Ptolemy (c. 90 - c. 168 CE) • Librarian at Alexandria • “The Great Treatise” & “The Almagest” (to the 12th Century) The Ptolemaic System: Objectives Wanted: A Model to explain the observed apparent motions of the Sun, Moon, Planets, and the Celestial Sphere. The Model should explain related phenomena such as the lunar phases, eclipses, and planetary brightness variation. The Model should be capable of accurately predicting these phenomena. (When? Where? Details?) The Model is geostatic, geocentric, and uses only uniform circular motions. (cf., the Aristotelian doctrines and the Aristarchian heresy.) The Ptolemaic System Observations • The apparent rotation of the Celestial Sphere • The annual motion of the Sun along the ecliptic • The monthly motion of the Moon The lunar phases and the synodic month Lunar and Solar Eclipses • The motions of the planets on the celestial sphere Direct and retrograde motions Planetary brightness variations Periodicities: The synodic periods Assumptions • A Geostatic cosmology (The Earth does not move.) • Uniform Circular motions (It is a “perfect” universe.) Approaches • The offsets and epicycles introduced by Hipparchus The Ptolemaic System For Inferior Planets (Mercury Venus) Deferent Period is 1 Year; Epicyclic period is the Synodic Period For Superior Planets (Mars, Jupiter, Saturn) Deferent Period is the Synodic period; Epicyclic Period is 1 year The Ptolemaic System (“To Scale”) Note: Indicated motions are with respect to the Celestial Sphere AGAIN: Problems with the Ptolemaic System Recollect the assumptions • The Earth doesn’t move (“geostatic”) • The Earth is at the center of the universe (“geocentric”) • All motions are circular (... or combinations thereof) • All motions are uniform (.. -
Cosmology Slides
Inhomogeneous cosmologies George Ellis, University of Cape Town 27th Texas Symposium on Relativistic Astrophyiscs Dallas, Texas Thursday 12th December 9h00-9h45 • The universe is inhomogeneous on all scales except the largest • This conclusion has often been resisted by theorists who have said it could not be so (e.g. walls and large scale motions) • Most of the universe is almost empty space, punctuated by very small very high density objects (e.g. solar system) • Very non-linear: / = 1030 in this room. Models in cosmology • Static: Einstein (1917), de Sitter (1917) • Spatially homogeneous and isotropic, evolving: - Friedmann (1922), Lemaitre (1927), Robertson-Walker, Tolman, Guth • Spatially homogeneous anisotropic (Bianchi/ Kantowski-Sachs) models: - Gödel, Schücking, Thorne, Misner, Collins and Hawking,Wainwright, … • Perturbed FLRW: Lifschitz, Hawking, Sachs and Wolfe, Peebles, Bardeen, Ellis and Bruni: structure formation (linear), CMB anisotropies, lensing Spherically symmetric inhomogeneous: • LTB: Lemaître, Tolman, Bondi, Silk, Krasinski, Celerier , Bolejko,…, • Szekeres (no symmetries): Sussman, Hellaby, Ishak, … • Swiss cheese: Einstein and Strauss, Schücking, Kantowski, Dyer,… • Lindquist and Wheeler: Perreira, Clifton, … • Black holes: Schwarzschild, Kerr The key observational point is that we can only observe on the past light cone (Hoyle, Schücking, Sachs) See the diagrams of our past light cone by Mark Whittle (Virginia) 5 Expand the spatial distances to see the causal structure: light cones at ±45o. Observable Geo Data Start of universe Particle Horizon (Rindler) Spacelike singularity (Penrose). 6 The cosmological principle The CP is the foundational assumption that the Universe obeys a cosmological law: It is necessarily spatially homogeneous and isotropic (Milne 1935, Bondi 1960) Thus a priori: geometry is Robertson-Walker Weaker form: the Copernican Principle: We do not live in a special place (Weinberg 1973). -
The Big Bang
The Big Bang • Review of Hubble expansion • Assumptions in cosmology • The Big Bang • Cosmic microwave background Hubble expansion v = H0d What would be the recession speed of a galaxy at a distance of 7 Mpc? A) 0.1 km/s B) 10 km/s C) 250 km/s D) 500 km/s E) 1000 km/s Speed = H0 distance H0 = 71 km/s/Mpc Receding galaxy 8 Speed = 500 km/s = 0.5 Mpc/Gyr 6 4 2 Distance (Mpc) 0 -2 -18 -16 -14 -12 -10 -8 -6 -4 -2 0 Time (Gyr) When was this galaxy in the same place as the Milky Way? time = distance / velocity = 7 Mpc/(0.5 Mpc/Gyr) = 14 Gyr ago If the Hubble constant were doubled, what would be the recession speed of a galaxy at a distance of 7 Mpc? A) 0.1 km/s B) 10 km/s C) 250 km/s D) 500 km/s E) 1000 km/s Speed = H distance H = 271 km/s/Mpc 0 0 Receding galaxy 8 Speed = 1000 km/s = 1.0 Mpc/Gyr 6 4 2 0 Distance (Mpc) -2 -4 -12 -10 -8 -6 -4 -2 0 Time (Gyr) When was this galaxy in the same place as the Milky Way? time = distance / velocity = 7 Mpc/(1.0 Mpc/Gyr) = 7 Gyr ago If Hubble's constant were twice as large as we now think it is, our estimate of the age of the universe would A) be unchanged B) increase by a factor of 2 C) increase by a factor of 4 D) decrease by a factor of 2 E) decrease by a factor of 4 Quasars are receding from us at high velocities because A) matter in black hole jets moves at close to the speed of light B) matter moves rapidly when close to a black hole C) quasars are at large distances D) we smell bad The variety of different active galaxies can be explained as due to A) different orientations of the accretion disk B) different forms of matter being accreted C) different shapes of black holes D) different velocities of black holes Assumptions in Cosmology Copernican principle: – We do not occupy a special place. -
Thinking Outside the Sphere Views of the Stars from Aristotle to Herschel Thinking Outside the Sphere
Thinking Outside the Sphere Views of the Stars from Aristotle to Herschel Thinking Outside the Sphere A Constellation of Rare Books from the History of Science Collection The exhibition was made possible by generous support from Mr. & Mrs. James B. Hebenstreit and Mrs. Lathrop M. Gates. CATALOG OF THE EXHIBITION Linda Hall Library Linda Hall Library of Science, Engineering and Technology Cynthia J. Rogers, Curator 5109 Cherry Street Kansas City MO 64110 1 Thinking Outside the Sphere is held in copyright by the Linda Hall Library, 2010, and any reproduction of text or images requires permission. The Linda Hall Library is an independently funded library devoted to science, engineering and technology which is used extensively by The exhibition opened at the Linda Hall Library April 22 and closed companies, academic institutions and individuals throughout the world. September 18, 2010. The Library was established by the wills of Herbert and Linda Hall and opened in 1946. It is located on a 14 acre arboretum in Kansas City, Missouri, the site of the former home of Herbert and Linda Hall. Sources of images on preliminary pages: Page 1, cover left: Peter Apian. Cosmographia, 1550. We invite you to visit the Library or our website at www.lindahlll.org. Page 1, right: Camille Flammarion. L'atmosphère météorologie populaire, 1888. Page 3, Table of contents: Leonhard Euler. Theoria motuum planetarum et cometarum, 1744. 2 Table of Contents Introduction Section1 The Ancient Universe Section2 The Enduring Earth-Centered System Section3 The Sun Takes -
A Democratic Cosmos? Arxiv:1910.00481V1 [Physics.Hist-Ph] 1 Oct 2019
A democratic Cosmos? Guilherme Franzmann1 and Yigit Yargic2 1Department of Physics, McGill University, Montréal, QC, H3A 2T8, Canada 2Perimeter Institute for Theoretical Physics, 31 Caroline St. N., Waterloo ON, N2L 2Y5, Canada Abstract Despite the success of our best models in Theoretical Physics, especially concerning Cosmology and Particle Physics, we still face persistent challenges. Among them we have the cosmological singularity problem, understanding the late-time acceleration of the Universe, and comprehending the fundamental na- ture of time. We believe relevant new insights to tackle each of these issues may be found in the Philosophy of Cosmology. We elaborate on three philosophical principles that shall guide us on how to improve our current theories. They are the Copernican Principle for Scales, the Cosmological Heterarchical Principle and the Cosmological Principle of Irreversibility. Following these principles, and using some of our current physical theories as a proxy to implement them, we consider a new assessment of each of these challenges, and show how they may be either explained away, hinting towards new physics, or summarized in a new philosophical principle. Essay written for the 2019 Essay Prize in Philosophy of Cosmology1. arXiv:1910.00481v1 [physics.hist-ph] 1 Oct 2019 1http://www.rotman.uwo.ca/2019-essay-prize-in-philosophy-of-cosmology/ 1 Contents 1 The Cosmic Pnyka 3 2 The Copernican Principle for Scales 5 3 The Cosmological Heterarchical Principle 8 4 The landscape of scales 10 5 The Very Early Universe 12 5.1 T-duality . 12 6 Λ-theory: GR’s unknown heir in the deep IR 15 6.1 Inspirations from MOND . -
Living in a Void: Testing the Copernican Principle with Distant Supernovae
Living in a Void: Testing the Copernican Principle with Distant Supernovae Timothy Clifton,∗ Pedro G. Ferreira, and Kate Land Oxford Astrophysics, Physics, DWB, Keble Road, Oxford, OX1 3RH, UK A fundamental presupposition of modern cosmology is the Copernican Principle; that we are not in a central, or otherwise special region of the Universe. Studies of Type Ia supernovae, together with the Copernican Principle, have led to the inference that the Universe is accelerating in its expansion. The usual explanation for this is that there must exist a ‘Dark Energy’, to drive the acceleration. Alternatively, it could be the case that the Copernican Principle is invalid, and that the data has been interpreted within an inappropriate theoretical frame-work. If we were to live in a special place in the Universe, near the centre of a void where the local matter density is low, then the supernovae observations could be accounted for without the addition of dark energy. We show that the local redshift dependence of the luminosity distance can be used as a clear discriminant between these two paradigms. Future surveys of Type Ia supernovae that focus on a redshift range of ∼ 0.1 − 0.4 will be ideally suited to test this hypothesis, and hence to observationally determine the validity of the Copernican Principle on new scales, as well as probing the degree to which dark energy must be considered a necessary ingredient in the Universe. The concordance model of the Universe combines two An alternative to admitting the existence of dark en- fundamental assumptions. The first is that space-time ergy is to review the postulates that necessitate its intro- is dynamical, obeying Einstein’s Equations. -
Nicolaus Copernicus: the Loss of Centrality
I Nicolaus Copernicus: The Loss of Centrality The mathematician who studies the motions of the stars is surely like a blind man who, with only a staff to guide him, must make a great, endless, hazardous journey that winds through innumerable desolate places. [Rheticus, Narratio Prima (1540), 163] 1 Ptolemy and Copernicus The German playwright Bertold Brecht wrote his play Life of Galileo in exile in 1938–9. It was first performed in Zurich in 1943. In Brecht’s play two worldviews collide. There is the geocentric worldview, which holds that the Earth is at the center of a closed universe. Among its many proponents were Aristotle (384–322 BC), Ptolemy (AD 85–165), and Martin Luther (1483–1546). Opposed to geocentrism is the heliocentric worldview. Heliocentrism teaches that the sun occupies the center of an open universe. Among its many proponents were Copernicus (1473–1543), Kepler (1571–1630), Galileo (1564–1642), and Newton (1643–1727). In Act One the Italian mathematician and physicist Galileo Galilei shows his assistant Andrea a model of the Ptolemaic system. In the middle sits the Earth, sur- rounded by eight rings. The rings represent the crystal spheres, which carry the planets and the fixed stars. Galileo scowls at this model. “Yes, walls and spheres and immobility,” he complains. “For two thousand years people have believed that the sun and all the stars of heaven rotate around mankind.” And everybody believed that “they were sitting motionless inside this crystal sphere.” The Earth was motionless, everything else rotated around it. “But now we are breaking out of it,” Galileo assures his assistant. -
OR GREAT BOOK. Figure 10 Explains the Cosmographic System of The
36 THE "ALMAGEST" OR GREAT BOOK. Figure 10 explains the cosmographic system of the same astronomer. In the centre we see the Earth, externally surrounded by fire [which is precisely opposite to the truth, according to the fundamental principles of modern geology; but the reader will understand that we are not attempting here to expose the errors of Ptolemaus; we confine ourselves to a description of his system]. Above the Earth spreads the first crystalline heaven, which carries and conveys the Moon. In the second and third crystal heavens the planets Mercury and Venus respectively describe their epicycles. The fourth heaven belongs to the Sun ; wherein it traverses the circle known as the ecliptic. The three last celestial spheres include Mars, Jupiter, and Saturn. Beyond these planets shines the heaven of the fixed stars. It rotates upon itself from east to west, with an inconceivable rapidity and an incalculable force of impulsion, for it is this which sets in motion all the fabulous machine. Ptolemaus places on the extreme confines of his vast Whole the eternal abode of the blessed. Thrice happy they in having no further cause to concern themselves %I c r ~NT about so terrible a system ; a system far from transparent, notwithstand ing all its crystal! S The treatise in which the Greek SU N X astronomer summed up his labours r _N_U remained for generations in high ( favour with the learned, and especi r F; r ally with the Arabs, whose privilegp and renown it is to have preserved intact the precious deposit of the sciences, when the Europe of the N - twelfth and thirteenth centuries was plunged in the night-shadows of the profoundest ignorance. -
The Planetary Increase of Brightness During Retrograde Motion: an Explanandum Constructed Ad Explanantem
Studies in History and Philosophy of Science 54 (2015) 90e101 Contents lists available at ScienceDirect Studies in History and Philosophy of Science journal homepage: www.elsevier.com/locate/shpsa The planetary increase of brightness during retrograde motion: An explanandum constructed ad explanantem Christián Carlos Carman National University of Quilmes/CONICET, Roque Sáenz Peña 352, B1876BXD Bernal, Buenos Aires, Argentina article info abstract Article history: In Ancient Greek two models were proposed for explaining the planetary motion: the homocentric Received 5 May 2015 spheres of Eudoxus and the Epicycle and Deferent System. At least in a qualitative way, both models Received in revised form could explain the retrograde motion, the most challenging phenomenon to be explained using circular 17 September 2015 motions. Nevertheless, there is another explanandum: during retrograde motion the planets increase their brightness. It is natural to interpret a change of brightness, i.e., of apparent size, as a change in Keywords: distance. Now, while according to the Eudoxian model the planet is always equidistant from the earth, Epicycle; according to the epicycle and deferent system, the planet changes its distance from the earth, Deferent; fi Homocentric spheres; approaching to it during retrograde motion, just as observed. So, it is usually af rmed that the main ’ Brightness change reason for the rejection of Eudoxus homocentric spheres in favor of the epicycle and deferent system was that the first cannot explain the manifest planetary increase of brightness during retrograde motion, while the second can. In this paper I will show that this historical hypothesis is not as firmly founded as it is usually believed to be. -
The Copernican Revolution: Observational Tests
The Copernican Revolution: Observational Tests The Trigonometric (Geometric) Parallax Aristotle’s missing Stellar Parallax: The Earth has moved! Parallactic ellipse has (angular) semi major axis p = a/d (radians) ... where a is the Earth’s orbital “radius” and d is the distance to the star. For d in parsecs (pc), and p in arc-seconds (“): (pc) = 1/p(“) aEarth = 1 au = 1.50 x 108 km and 1 pc = 206,265 au First Measurement of a Stellar Parallax by Bessel (1838) ... 61 Cygni, also know as “Piazzi’s Flying Star”, with p = 0.287”, d = 3.48 pc (The largest stellar parallax is that of α Centauri with p = 0.75”) There are 206,265 arc-seconds (“) in a radian: 180°= π radians; 1°= 60’= 3,600” One astronomical unit is 23,455 Earth radii. The Aberration of Starlight The Earth is moving! The Earth’s orbital speed is v = 30 km s-1 The speed of light is c = 3 x 105 km s-1 Therefore, the maximum aberration angle is v/c = 10-4 radian = 21” (Note that the semi major axes of all annual aberration ellipses are 21”) History Roemer (1675) measures the velocity of light Observations of eclipses of the satellites of Jupiter. (Io, P = 1.76d) (His value for the speed of light was about 75% of the true value.) Note: Light travels 1 astronomical unit in about 500 seconds. Picard (1680) observes “puzzling parallax” of Polaris (~20”) d (parsecs) = 1/p(“) .... but the motion was in the wrong direction for parallactic motion! ... and was seen with the same amplitude in all directions on the sky! Bradley (1728) explains the phemomenon (and provides observations of γ Draconis) Note that this was over a century before Bessel successfully measured the trigonometric parallax of 61 Cygni in 1838. -
Historical Astronomy
Historical Astronomy (Neolithic record of Moon Phases) Introduction Arguably the history of astronomy IS the history of science. Many cultures carried out astronomical observations. However, very few formed mathematical or physical models based on their observations. It is those that did that we will focus on here, primarily the Babylonians and Greeks. Other Examples At the same time, that focus should not cause us to forget the impressive accomplishments of other cultures. Other Examples ∼ 2300 year old Chankillo Big Horn Medicine Wheel, Observatory, near Lima, Wyoming Peru Other Examples Chinese Star Map - Chinese records go back over 4000 Stonehenge, England years Babylonian Astronomy The story we will follow in more detail begins with the Babylonians / Mesopotamians / Sumerians, the cultures that inhabited the “fertile crescent.” Babylonian Astronomy Their observations and mathematics was instrumental to the development of Greek astronomy and continues to influence science today. They were the first to provide a mathematical description of astronomical events, recognize that astronomical events were periodic, and to devise a theory of the planets. Babylonian Astronomy Some accomplishments: • The accurate prediction of solar and lunar eclipses. • They developed mathematical models to predict the motions of the planets. • Accurate star charts. • Recognized the changing apparent speed of the Sun’s motion. • Developed models to account for the changing speed of the Sun and Moon. • Gave us the idea of 360◦ in a circle, 600 in a degree, 6000 in a minute. Alas, only very fragmentary records of their work survives. Early Greek The conquests of Alexander the Great are oen credited with bringing knowl- edge of the Babylonians science and mathematics to the Greeks. -
“Point at Infinity Hape of the World
“Point at Infinity hape of the World Last week, we began a series of posts dedicated to thinking about immortality. If we want to even pretend to think precisely about immortality, we will have to consider some fundamental questions. What does it mean to be immortal? What does it mean to live forever? Are these the same thing? And since immortality is inextricably tied up in one’s relationship with time, we must think about the nature of time itself. Is there a difference between external time and personal time? What is the shape of time? Is time linear? Circular? Finite? Infinite? Of course, we exist not just across time but across space as well, so the same questions become relevant when asked about space. What is the shape of space? Is it finite? Infinite? It is not hard to see how this question would have a significant bearing on our thinking about immortality. In a finite universe (or, more precisely, a universe in which only finitely many different configurations of maer are possible), an immortal being would encounter the same situations over and over again, would think the same thoughts over and over again, would have the same conversations over and over again. Would such a life be desirable? (It is not clear that this repetition would be avoidable even in an infinite universe, but more on that later.) Today, we are going to take a lile historical detour to look at the shape of the universe, a trip that will take us from Ptolemy to Dante to Einstein, a trip that will uncover a remarkable confluence of poetry and physics.