Rotation Velocity Curve Measurement of SDSS-IV Manga Galaxies

Total Page:16

File Type:pdf, Size:1020Kb

Rotation Velocity Curve Measurement of SDSS-IV Manga Galaxies Rotation Velocity Curve Measurement of SDSS-IV MaNGA Galaxies 6th Survey Science Group Workshop 2017 June 30th, Ulleung Dae-A Resort Haeun Chung (SNU/KIAS) and Changbom Park (KIAS) Galaxy Rotation Curve Vera Rubin found flat rotation curve of M31 Corbelli and Salucci (1999) Rubin and Kent (1970) Dark Matter Star Gas Mass distribution of baryons can not explain this! 2017-07-03 6th Survey Science Group Workshop 2 MaNGA: Mapping Nearby Galaxies at APO . Multi-Integral Field Unit (Multi-IFUs) . 17 IFUs on 3° diameter plate – IFU diameters from 12” to 32” – Galaxy radius up to 1.5 – 2.5 Re . SDSS BOSS Spectrograph – 3600-10300Å, R~2000 . Project duration: 6 years – Launched on 2014 July 1 – Half of SDSS-IV dark time . Aim to observe ~ 10,000 galaxies . Data Release (July 2016) – SDSS DR13 – 1,390 MaNGA Galaxies (observed by June 2015) 2017-07-03 6th Survey Science Group Workshop 3 MaNGA: Mapping Nearby Galaxies at APO 2017-07-03 6th Survey Science Group Workshop 4 ~1,390 MaNGA Galaxies from SDSS DR13 Purpose of this Study . MaNGA is an excellent survey to study kinematics of nearby galaxies. – Especially stellar kinematics. Measure Rotation Curve from all MaNGA Galaxies, automatically! 2017-07-03 6th Survey Science Group Workshop 7 Galaxy Rotation Curve 휽 휽 ( , ) , = + ×′ sin′ × cos ↔ = sin × cos − First, we need to measure 2D line of sight velocity (VLOS) of galaxies 2017-07-03 6th Survey Science Group Workshop 8 2D Velocity Map . We use pPXF to measure LOSVD of each spaxel. – Penalized Pixel-Fitting (pPXF) is a SED model fitting code developed by Michele Cappellari (Cappellari+04) . We use Miles stellar libraries - Solar Metallicity, 2 ages . 1,390 All DR13 MaNGA galaxies: 400-2700 specs/IFU . Total 2.2M specs to measure LOSVD 3D Cube Data Run pPXF - Velocity - Velocity dispersion - High order kinematics - Steller population Cappellari+17 2017-07-03 6th Survey Science Group Workshop 9 2D Velocity Map Now we have 2D Vel Map of all DR13 1,390 MaNGA Galaxies 2017-07-03 6th Survey Science Group Workshop 10 Galaxy Rotation Curve Measurement . To measure RC, we need to know , , inclination angle , position angle . All MaNGA galaxies are observed before. So we already know above parameters. . Done…? 2017-07-03 6th Survey Science Group Workshop 11 Galaxy Rotation Curve Measurement . Incorrect photometric PA / Inclination Angle 2017-07-03 6th Survey Science Group Workshop 12 Galaxy Rotation Curve Measurement . Off center cases . We can not just use SDSS image data. we need to obtain Incl, PA, and center from 2D VelMap!! 2017-07-03 6th Survey Science Group Workshop 13 Galaxy Rotation Curve Measurement . How to measure geometrical parameters from 2D Vel Map? = + × sin × cos . If we have a good V(r), we can fit a 2D velocity model on to the data to get the geometrical parameters. Fortunately, we have a simple function which well approximate an actual RC. – Hyperbolic tangent function. = × tanh(r/R ) c R c Galaxy Rotation Curve Measurement . 2D model velocity map with different inclination angle / Rc Inclination Angle R c Galaxy Rotation Curve Measurement . We need one more step – We need a proper mask! . Now we have proper masks for model fitting. 2017-07-03 6th Survey Science Group Workshop 16 2D Velocity Model Fitting . We fit 7 parameters simultaneously + Xcent , Ycent = + × tanh(r/ ) × sin × cos . Due to limitation of MPFIT, fitting result is very sensitive to the initial parameters. . Two solutions – Do Monte Carlo – Provide good initial value . Fit the model with good initial value. Use known SDSS photometric data. Use photometric data during mask generation . First fit on smoothed 2D vel map, second fit on original 2D vel map. -> Smoothed vel map image 2017-07-03 6th Survey Science Group Workshop 17 Fitting Results 2D Velocity Map Results . Success ratio: – Out of 1,390 MaNGA galaxies: – 996 galaxies shows good results – 71.6% . We are working on increasing success rate 2017-07-03 6th Survey Science Group Workshop 22 Limitation of MaNGA 3D Cube . MaNGA 3D Cube is quite blurred, due to IFU sampling size and seeing. SDSS Camera Pixel Size SDSS gri 2” 0.4” MaNGA gri MaNGA fiber size 2017-07-03 6th Survey Science Group Workshop 23 Limitation of MaNGA 3D Cube . Since size of PSF (point spread function) is large, (~2.5” in FWHM) it would affect to the shape of the measured 2D velocity map. Convolution Original Galaxy MaNGA PSF Observed Galaxy 2017-07-03 6th Survey Science Group Workshop 24 Deconvolution . If we know the PSF which made observed galaxy, we can (mathematically, theoretically) reverse the convolution process and make original galaxy! Deconvolution Observed Galaxy MaNGA PSF Original Galaxy 2017-07-03 6th Survey Science Group Workshop 25 3D Cube Deconvolution y Deconvolution with known Gaussian PSF x Original 2D Image 2D Image Deconvolved MaNGA 3DCube @each wavelength After deconvolution MaNGA 3DCube 3D Cube Deconvolution . MaNGA provides FWHM at 4 wavelengths (griz) – About 2.5” . Deconvolution algorithm – Simple inversion – Lucy-Richardson (Poisson max likelihood) – Frieden (Friden max entrophy) Original – Gaussian (Gaussian max likelihood) MaNGA gri – Jansson-van Cittert . Noise? – From original 3D cube. (1st order approximation) Fitting Results Fitting Results Compare Before / After Deconvolution 2017-07-03 6th Survey Science Group Workshop 30 Compare Before / After Deconvolution 2017-07-03 6th Survey Science Group Workshop 31 Inclination Degeneracy 2017-07-03 6th Survey Science Group Workshop 32 Summary . We measure velocity rotation curves from original / deconvolved MaNGA 3D Cubes. – Measure 2D VLOS map from 3D Cube – Generate proper mask – Fit tanh 2D VLOS map to get geometrical parameters . Deconvolved 3D Cube show small scale structures as well as true rotation curve. We work on developing science cases using these data, including analysis on abnormal cases. 2017-07-03 6th Survey Science Group Workshop 33.
Recommended publications
  • (Dark) Matter! Luminous Matter Is Concentrated at the Center
    Cosmology Two Mysteries and then How we got here Dark Matter Orbital velocity law Derivable from Kepler's 3rd law and Newton's Law of gravity r v2 M = r G M : mass lying within stellar orbit r r: radius from the Galactic center v: orbital velocity From Sun's r and v: there are about 100 billion solar masses inside the Sun's orbit! 4 Rotation curve of the Milky Way: Speed of stars and clouds of gas (from Doppler shift) vs distance from center Galaxy: rotation curve flattens out with distance Indicates much more mass in the Galaxy than observed as stars and gas! Mass not concentrated at center5 From the rotation curve, inferred distribution of dark matter: The Milky Way is surrounded by an enormous halo of non-luminous (dark) matter! Luminous matter is concentrated at the center 6 We can make measurements for other galaxies Weighing spiral galaxies C Compare shifts of spectral lines (in atomic H gas clouds) as a function of distance from the center 7 Rotation curves for various spiral galaxies First measured in 1960's by Vera Rubin They all flatten out with increasing radius, implying that all spiral galaxies have vast haloes of dark matter – luminous matter 1/6th of mass 8 This mass is the DARK MATTER: It's some substance that interacts gravitationally (equivalent to saying that it has mass)... It neither emits nor absorbs light in any form (equivalent to saying that it does not interact electromagnetically) Dark matter might conceivably have 'weak' (radioactive force) interactions 9 Gaggles of Galaxies • Galaxy groups > The Local group
    [Show full text]
  • A Case for Alternate Theories of Gravity C Sivaram Indian Institute Of
    Preprints (www.preprints.org) | NOT PEER-REVIEWED | Posted: 19 June 2020 doi:10.20944/preprints202006.0239.v1 Non-detection of Dark Matter particles: A case for alternate theories of gravity C Sivaram Indian Institute of Astrophysics, Bangalore, 560 034, India e-mail: [email protected] Kenath Arun Christ Junior College, Bangalore, 560 029, India e-mail: [email protected] A Prasad Center for Space Plasma & Aeronomic Research, The University of Alabama in Huntsville, Huntsville, Alabama 35899 email: [email protected] Louise Rebecca Christ Junior College, Bangalore - 560 029, India e-mail: [email protected] Abstract: While there is overwhelming evidence for dark matter (DM) in galaxies and galaxy clusters, all searches for DM particles have so far proved negative. It is not even clear whether only one particle is involved or a combination or particles, their masses not precisely predicted. This non-detectability raises the possible relevance of modified gravity theories – MOND, MONG, etc. Here we consider a specific modification of Newtonian gravity (MONG) which involves gravitational self-energy, leading to modified equations whose solutions imply flat rotation curves and limitations of sizes of clusters. The results are consistent with current observations including that involving large spirals. This modification could also explain the current Hubble tension. We also consider effects of dark energy (DE) in terms of a cosmological constant. 1 © 2020 by the author(s). Distributed under a Creative Commons CC BY license. Preprints (www.preprints.org) | NOT PEER-REVIEWED | Posted: 19 June 2020 doi:10.20944/preprints202006.0239.v1 Over the past few decades there have been a plethora of sophisticated experiments involving massive sensitive detectors trying to catch faint traces of the elusive Dark Matter (DM) particles.
    [Show full text]
  • Disk Galaxy Rotation Curves and Dark Matter Distribution
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Disk galaxy rotation curves and dark matter distribution by Dilip G. Banhatti School of Physics, Madurai-Kamaraj University, Madurai 625021, India [Based on a pedagogic / didactic seminar given by DGB at the Graduate College “High Energy & Particle Astrophysics” at Karlsruhe in Germany on Friday the 20 th January 2006] Abstract . After explaining the motivation for this article, we briefly recapitulate the methods used to determine the rotation curves of our Galaxy and other spiral galaxies in their outer parts, and the results of applying these methods. We then present the essential Newtonian theory of (disk) galaxy rotation curves. The next two sections present two numerical simulation schemes and brief results. Finally, attempts to apply Einsteinian general relativity to the dynamics are described. The article ends with a summary and prospects for further work in this area. Recent observations and models of the very inner central parts of galaxian rotation curves are omitted, as also attempts to apply modified Newtonian dynamics to the outer parts. Motivation . Extensive radio observations determined the detailed rotation curve of our Milky Way Galaxy as well as other (spiral) disk galaxies to be flat much beyond their extent as seen in the optical band. Assuming a balance between the gravitational and centrifugal forces within Newtonian mechanics, the orbital speed V is expected to fall with the galactocentric distance r as V 2 = GM/r beyond the physical extent of the galaxy of mass M, G being the gravitational constant.
    [Show full text]
  • Rotation and Mass in the Milky Way and Spiral Galaxies
    Publ. Astron. Soc. Japan (2014) 00(0), 1–34 1 doi: 10.1093/pasj/xxx000 Rotation and Mass in the Milky Way and Spiral Galaxies Yoshiaki SOFUE1 1Institute of Astronomy, The University of Tokyo, Mitaka, 181-0015 Tokyo ∗E-mail: [email protected] Received ; Accepted Abstract Rotation curves are the basic tool for deriving the distribution of mass in spiral galaxies. In this review, we describe various methods to measure rotation curves in the Milky Way and spiral galaxies. We then describe two major methods to calculate the mass distribution using the rotation curve. By the direct method, the mass is calculated from rotation velocities without employing mass models. By the decomposition method, the rotation curve is deconvolved into multiple mass components by model fitting assuming a black hole, bulge, exponential disk and dark halo. The decomposition is useful for statistical correlation analyses among the dynamical parameters of the mass components. We also review recent observations and derived results. Full resolution copy is available at URL: http://www.ioa.s.u-tokyo.ac.jp/∼sofue/htdocs/PASJreview2016/ Key words: Galaxy: fundamental parameters – Galaxy: kinematics and dynamics – Galaxy: structure – galaxies: fundamental parameters – galaxies: kinematics and dynamics – galaxies: structure – dark matter 1 INTRODUCTION rotation curves of the Milky Way and spiral galaxies, respec- tively, and describe the general characteristics of observed rota- tion curves. The progress in the rotation curve studies will be Rotation of spiral galaxies is measured by spectroscopic ob- also reviewed briefly. In section 4 we review the methods to de- arXiv:1608.08350v1 [astro-ph.GA] 30 Aug 2016 servations of emission lines such as Hα, HI and CO lines from termine the mass distributions in disk galaxies using the rotation disk objects, namely population I objects and interstellar gases.
    [Show full text]
  • Was 49B: an Overmassive AGN in a Merging Dwarf Galaxy?
    A Preprint typeset using LTEX style emulateapj v. 5/2/11 WAS 49B: AN OVERMASSIVE AGN IN A MERGING DWARF GALAXY? Nathan J. Secrest1,5, Henrique R. Schmitt2, Laura Blecha3, Barry Rothberg4,5, and Jacqueline Fischer2 1National Academy of Sciences NRC Research Associate, resident at Naval Research Laboratory; [email protected] 2Naval Research Laboratory, Remote Sensing Division, 4555 Overlook Ave. SW, Washington, DC 20375, USA 3University of Maryland Dept. of Astronomy, 1113 PSC, Bldg. 415, College Park, MD 20742, USA 4LBT Observatory, University of Arizona, 933 N. Cherry Ave., Tuscan, AZ 85721, USA and 5Department of Physics & Astronomy, George Mason University, MS 3F3, 4400 University Drive, Fairfax, VA 22030, USA ABSTRACT We present a combined morphological and X-ray analysis of Was 49, an isolated, dual AGN system notable for the presence of a dominant AGN Was 49b in the disk of the primary galaxy Was 49a, at a projected radial distance of 8 kpc from the nucleus. Using X-ray data from Chandra, NuSTAR, and 45 −1 Swift, we find that this AGN has a bolometric luminosity of Lbol ∼ 2 × 10 erg s , with a black +2.9 8 hole mass of MBH =1.3−0.9 × 10 M⊙. Despite its large mass, our analysis of optical data from the Discovery Channel Telescope shows that the supermassive black hole is hosted by a stellar counterpart +4.9 9 with a mass of only 5.6−2.6 ×10 M⊙, making the SMBH potentially larger than expected from SMBH- galaxy scaling relations, and the stellar counterpart exhibits a morphology that is consistent with dwarf elliptical galaxies.
    [Show full text]
  • Hands-On Radio Astronomy Mapping the Milky Way
    Hands-On Radio Astronomy Mapping the Milky Way Cathy Horellou & Daniel Johansson Onsala Space Observatory Chalmers University of Technology Date of last revision: 2010 October 4, CH SE-439 92 Onsala Sweden Contents Abstract 3 1 Welcome to the Galaxy 4 1.1 WhereareweintheMilkyWay? . 5 1.1.1 Galactic longitude and latitude . ..... 5 1.1.2 Notations ................................... 5 1.2 Lookingforhydrogen.............................. ... 6 1.3 TheDopplereffect ................................. 7 2 The theory behind the Milky Way 9 2.1 Preliminarycalculations . ...... 9 2.2 Howdoesthegasrotate?............................ 10 2.3 Whereisthegas?................................... 11 2.4 EstimatingthemassofourGalaxy . ..... 13 3 Observing with Such A Lovely Small Antenna (SALSA) 14 3.1 SALSA-Onsala .................................... 14 3.2 Beforetheobservations. ..... 14 3.3 HowtoobservewithSALSA-Onsala. ..... 14 3.3.1 NX....................................... 15 3.3.2 qradio ..................................... 15 3.3.3 kstars: A planetarium program to control the radio telescope . 17 4 After the observations – my first maps of the Milky Way 19 4.1 Software........................................ 19 4.2 Dataprocessing.................................. 19 4.3 Dataanalysis .................................... 20 4.3.1 Rotationcurve ................................ 20 4.3.2 MapoftheMilkyWay ............................ 22 Appendices 24 A Rotation curves 25 A.1 Solid-bodyrotation .............................. 25 A.2 Keplerianrotation: theSolarsystem
    [Show full text]
  • Dark Matter Halos of Spiral Galaxies
    Dark Matter Halos of Spiral Galaxies Arunima Banerjee National Centre for Radio Astrophysics Tata Institute of Fundamental Research Pune, India email: [email protected] Web: http://www.ncra.tifr.res.in/~arunima PLAN OF THE TALK • Spiral Galaxies: An Overview • Dark Matter: A Brief History • LCDM model: Success & Failure • Tracking DM halos using HI Rotation Curve & Scale height data • Application & Results • Summary Spiral Galaxies: An Overview OUR MILKY WAY OTHER SPIRAL GALAXIES NGC 891 NGC 628 THE GALAXY CLASSIFICATION SCHEME NGC 628 FACE-ON SPIRAL GALAXY NGC 891 M87 EDGE-ON SPIRAL GALAXY ELLIPTICAL GALAXY BASIC BUILDING BLOCKS OF A SPIRAL GALAXY σ MASS ∆R ∆Z (km/s) (Msun ) (KPC) (KPC) Differential Rotation DM 10 12 200 200 STARS 10 11 10 0.350 18 Caveat: Not to Scale! GAS(HI) 10 10 30 0.15 - 1 7-9 R A MULTI-WAVELENGTH VIEW OF THE MILKY WAY GALAXY ENVIRONMENT: CLUSTER, GROUP, FIELD Cluster Group Abell 1689 Field Robert’s Quartet NGC 891 Dark Matter: A Brief History DARK MATTER: CLUSTER KINEMATICS (1933) Fritz Zwicky From Virial Theorem, Coma Cluster (Abell 1669) T + V = 0 Estimable from the Doppler Shifts of the i.e. V = -T galaxy spectra Hints at the existence of Dark Matter! But Estimable from the lumininosities of the V >> Vobs !! galaxies DARK MATTER: GALAXY ROTATION CURVE (1980) Vera Rubin Observed M(R) ~ R !! VROT =(GM/R)½ R Vrot (km/s) R(kpc) DARK MATTER: LARGE SCALE STRUCTURE AND COSMOLOGY Observed Large Scale Structure (SDSS) Ansotropies in the Cosmic Microwave Background (WMAP) Abundance of H, He, Li ΛCDM: STANDARD MODEL OF COSMOLOGY ORDINARY MATTER! Matter-energy budget in the LCDM universe which consists of dark energy and cold, dissipationless and collisionless dark matter LCDM Model: Success & Failure DARK MATTER DISTRIBUTION IN THE UNIVERSE AT PRESENT TIME Millenium Simulation LCDM HALOS: A ONE-SLIDE PRIMER Bett et al.
    [Show full text]
  • Kinematics and Dynamics of the Luminous Infrared Galaxy Pair NGC 5257/58 (Arp 240)? I
    A&A 621, A25 (2019) Astronomy https://doi.org/10.1051/0004-6361/201834159 & c ESO 2018 Astrophysics Kinematics and dynamics of the luminous infrared galaxy pair NGC 5257/58 (Arp 240)? I. Fuentes-Carrera1, M. Rosado2, P. Amram3, E. Laurikainen4, H. Salo4, J. A. Gómez-López3, H. O. Castañeda1, A. Bernal2, and C. Balkowski5 1 Escuela Superior de Física y Matemáticas, Instituto Politécnico Nacional (ESFM-IPN), U.P. Adolfo López Mateos, edificio 9, Zacatenco, 07730 Mexico City, Mexico e-mail: [email protected], [email protected] 2 Instituto de Astronomía, Universidad Nacional Autónoma de México (UNAM), Apdo. Postal 70-264, 04510 Mexico City, Mexico 3 Aix-Marseille Université, CNRS, LAM (Laboratoire d’Astrophysique de Marseille), 13388 Marseille, France 4 Department of Physical Sciences, Division of Astronomy, University of Oulu, 90570 Oulu, Finland 5 GEPI, Observatoire de Paris, CNRS, Université Paris Diderot, 5 Place Jules Janssen, 92190 Meudon, France Received 29 August 2018 / Accepted 19 October 2018 ABSTRACT Context. Encounters between galaxies modify their morphology, kinematics, and star formation history. The relation between these changes and external perturbations is not straightforward. The great number of parameters involved requires both the study of large samples and individual encounters where particular features, motions, and perturbations can be traced and analysed in detail. Aims. We analysed the morphology, kinematics, and dynamics of two luminous infrared spiral galaxies of almost equal mass, NGC 5257 and NGC 5258, in which star formation is mostly confined to the spiral arms, in order to understand interactions be- tween galaxies of equivalent masses and star-forming processes during the encounter.
    [Show full text]
  • Constraining Spiral Galaxy Mass Distributions with the Rss Imaging Spectroscopy Nearby Galaxy Survey
    CONSTRAINING SPIRAL GALAXY MASS DISTRIBUTIONS WITH THE RSS IMAGING SPECTROSCOPY NEARBY GALAXY SURVEY By CARL J. MITCHELL A dissertation submitted to the Graduate School|New Brunswick Rutgers, The State University of New Jersey in partial fulfillment of the requirements for the degree of Doctor of Philosophy Graduate Program in Physics and Astronomy written under the direction of J. A. Sellwood and approved by New Brunswick, New Jersey October, 2017 ABSTRACT OF THE DISSERTATION Constraining Spiral Galaxy Mass Distributions with the RSS Imaging Spectroscopy Nearby Galaxy Survey By CARL J. MITCHELL Dissertation Director: J. A. Sellwood Kinematic measurements of galaxies provide a way to trace their mass distributions. The RSS Imaging spectroscopy Nearby Galaxy Survey (RINGS) was designed to probe the mass distributions of 19 spiral galaxies on small spatial scales by obtaining a suite of multi-wavelength kinematic and photometric data. In this dissertation, I introduce the high-spatial-resolution, medium-spectral-resolution Hα kinematic portion of the survey, and detail the process which has been used to convert the raw Fabry-P´erotobservations into useful kinematic data and models. These Hα kinematic data were obtained with the Robert Stobie Spectrograph (RSS) at the Southern African Large Telescope (SALT). I then demon- strate how these Hα kinematic data can be combined with the other types of observations in RINGS, H I radio interferometry and broadband photometric imaging, to probe these galaxies' mass distributions. ii Acknowledgments This work would not have been possible without the contributions of a number of other people. First and foremost, I must thank Jerry Sellwood for providing me with his support and insight over the last several years.
    [Show full text]
  • Arxiv:1710.10630V1 [Astro-Ph.GA] 29 Oct 2017
    Zasov A.V., Saburova A.S., Khoperskov A.V., Khoperskov S.A. Dark matter in galaxies. Physics- Uspekhi (Advances in Physical Sciences), 2017, v.60, no.1, pp. 3-39 DOI: 10.3367/UFNe.2016.03.037751 A.V. Zasov, A.S. Saburova, A.V. Khoperskov, S.A. Khoperskov Dark matter in galaxies УДК 524.6 PACS: 95.35.+d Dark matter; 98.62.Dm Kinematics, dynamics, and rotation; 98.62.Gq Galactic halos Dark matter in galaxies, its abundance, and its distribution remain a subject of long- standing discussion, especially in view of the fact that neither dark matter particles nor dark matter bodies have yet been found. Experts’ opinions range from ‘a very large number of completely dark galaxies exist’ to ‘nonbaryonic dark matter does not exist at all in any significant amounts’. We discuss astronomical evidence for the existence of dark matter and its connection with visible matter and examine attempts to estimate its mass and distribution in galaxies from photometry, dynamics, gravitational lensing, and other observations (the cosmological aspects arXiv:1710.10630v1 [astro-ph.GA] 29 Oct 2017 of the existence of dark matter are not considered in this review). In our view, the presence of dark matter in and around galaxies is a well-established fact. We conclude with an overview of mechanisms by which a dark halo can influence intragalactic processes. 1 1 Introduction Dark matter (DM) is one of the fundamental problems of modern astrophysics. It remains unsolved because the nature of DM is unknown and there is no clear understanding of DM relation with observed astronomical objects.
    [Show full text]
  • Survey of Astrophysics A110 Galaxies
    Galaxies Survey of Astrophysics A110 Galaxies Survey of Astrophysics A110 Galaxies • Goals: – To determine the types and distributions of galaxies? – How do we measure the mass of galaxies and what comprises this mass? – How do we measure distances to galaxies and what does this tell us about their formation? • Nebulae and Galaxies – In 1845 Parsons discovered that many nebulae had spiral structures. • Most astronomers believed that the nebulae were local phenomenon (in our Galaxy). • In 1920 there was the “Great Debate” between Shapley (believed spiral nebulae were local) and Curtis (believed they were external galaxies). • Hubble solved the issue using Cepheids to measure the distances of galaxies. Galaxies Survey of Astrophysics A110 Galaxies Survey of Astrophysics A110 • Galaxy Types – The Hubble Classification Scheme Figure 26-10 • Four basic types of galaxies, Elliptical, Spiral, Barred Spiral and Irregular. • Each type of galaxy reflect their differences in shape, star formation and dynamical histories. • The sequence of galaxy types is called the “Hubble tuning fork”. • In general elliptical galaxies contain an old (cool and red) population of stars while spirals contain old (in the nucleus) and young (in the spiral arms). – Spiral Galaxies Figure 26-5 • Spiral galaxies are further subdivided according to the relative size of the central bulge and the winding of the spiral arms. Sa: Large nucleus (bulge), small disk Sb: Smaller nucleus, tight spiral arms Sc: Almost no nucleus, wide spiral arms Galaxies Survey of Astrophysics A110 Galaxies Survey of Astrophysics A110 – Spiral Galaxies • Disk is supported by rotational velocity. • Light profile in spirals falls off exponentially with distance from the center of the galaxy.
    [Show full text]
  • Newtonian Explanation of Galaxy Rotation Curves Based on Distribution of Baryonic Matter Konstantin Pavlovich, Alex Pavlovich & Alan Sipols June 9, 2014
    Newtonian explanation of galaxy rotation curves based on distribution of baryonic matter Konstantin Pavlovich, Alex Pavlovich & Alan Sipols June 9, 2014 360 W Illinois St., 8F, Chicago IL 60654, USA email: [email protected] ABSTRACT Circular velocities of stars and gas in galaxies generally do not decline in accordance with widely expected Keplerian fall-off in velocities further from the galactic nucleus. Two main groups of theories were proposed to explain the supposed discrepancy—first, the most commonly accepted, is the suggestion of the existence of large non-baryonic dark matter halo, and, second are theories advocating some modification to the law of gravity. So far however, there is no empirical evidence for either dark matter or modified gravity. Here we show that a broad range of galaxy rotation curves can be explained solely in accordance with Newton’s law of gravity by modeling the distribution of baryonic matter in a galaxy. We demonstrate that the expectation of Keplerian fall-off is incorrect, and that a large number of likely galaxy mass distribution profiles should in fact produce flat or accelerating rotation curves similar to those observed in reality. We further support our theoretical findings with the model fit of 47 real galaxies’ rotation curves, representing a broad range of galactic types and sizes, and achieving correlation of expected and observed velocities of over 0.995 for all cases. Our results make theories of exotic dark matter or modified gravity unnecessary for the explanation of galaxy rotation curves. INTRODUCTION Since Fritz Zwicky’s observations 1 of galaxy rotation curves in 1930s astronomers were puzzled by the fact that circular velocities of stars and gas further from the nucleus of the galaxy generally do not decline in accordance with widely expected Keplerian fall-off, similar to the decline in the Solar system 2.
    [Show full text]