Jets from Spinning Black Holes in Active Galactic Nuclei

Total Page:16

File Type:pdf, Size:1020Kb

Jets from Spinning Black Holes in Active Galactic Nuclei Jets from Spinning Black Holes in Active Galactic Nuclei Dissertation zur Erlangung des Doktorgrades (Dr. rer. nat.) der Mathematisch-Naturwissenschaftlichen Fakult¨at der Rheinischen Friedrich-Wilhelms-Universit¨at Bonn vorgelegt von Ioana Dut¸an aus Bukarest, Rum¨anien Bonn, im Oktober 2010 Angefertigt mit Genehmigung der Mathematisch-Naturwissenschaftlichen Fakult¨at der Rheinischen Friedrich-Wilhelms-Universit¨at Bonn Promotionskommission: 1. Erstgutachter und Betreuer: Prof. Dr. Peter L. Biermann, Max Planck Institute for Radio Astronomy, Bonn 2. Zweitgutachter: Prof. Dr. Uli Klein, Argelander Institute for Astronomy, Bonn 3. Fachnahes Mitglied: PD Dr. J¨org Pretz, Institute of Physics, Bonn 4. Fachangrenzendes Mitglied: Prof. Dr. Jens Franke, Mathematical Institute of the University of Bonn Tag der Promotion: 31 Januar 2011 Diese Dissertation ist auf dem Hochschulschriftenserver der ULB Bonn http : //hss.ulb.uni bonn.de/diss−online − elektronisch publiziert. Das Erscheinungsjahr ist 2011. To my parents. iii iv . Acknowledgments This thesis could not have been completed without the generosity and assistance of a large number of people to whom I would like to express my gratitude. I am grateful to Peter L. Biermann, my thesis adviser, for the possibility he gave me to work on a subject I like and for his support that he made available in a number of ways. In particular, I would like to thank him for comprehensive and stimulating discussions, valuable suggestions and comments on this thesis and on my other manuscripts. I am also grateful to the second referee, Uli Klein, for reviewing this thesis. I also thank J¨org Pretz and Jens Franke, who kindly agreed to join the examination committee. I would like to thank my thesis committee (Peter L. Biermann, Uli Klein, Anton J. Zensus, and Frank Bertoldi) for offering suggestions to solve several problems encountered in my research. This work was supported by the International Max Planck Research School (IM- PRS) for Astronomy and Astrophysics at the Universities of Bonn and Cologne, being performed at the Max Planck Institute for Radio Astronomy, Bonn, in the Theory group. I am also grateful to Gerd Weigelt, the director of the Infrared Astronomy Department, for providing me with financial support during the final stage of this work. Furthermore, I would like to thank Ken-Ichi Nishikawa, Yosuke Mizuno, and Shinji Koide, my collaborators on General Relativistic Magnetohydrodynamic Simulations of Jet Formation, for providing me with their simulation code and for their scientific support and encouragement. The simulations were performed on a machine at the National Center for Supercomputing Applications at the University of Illinois at Urbana-Champaign, USA, through a research project whose principal investigator is Ken-Ichi Nishikawa. The results of this collaboration are presented in Chapter 4. I would like to thank Laurent¸iu Caramete, my office mate, for providing me with a complete sample of active galactic nuclei, which is a part of the work for his PhD thesis. This has made it possible for me to extend the application of the model for Ultra-high- energy Cosmic Rays developed in Chapter 3 to observational data. I also thank him for his friendship, patience, and help in ways too numerous to mention. I thank Alex Curut¸iu for his expertise whenever I was stuck with a problem in my programs, as well as for his friendship. I also thank Alan Roy, Iv´an Aguido, and Manuel Peruchio (from the VLBI group) for insights into observational research of active galactic nuclei. I am grateful to Michelle Fekety for proofreading this thesis and my other manu- scripts, as well as for her friendship and kind assistance in dealing with bureaucratic pro- cedures and many hassles. It is a pleasure to thank my colleagues and friends for a lot of help, for numerous discussions either related to science or just about life itself, and for creating a friendly atmosphere in which I could enjoy the work at this thesis. Beside those already mentioned, I thank Hyunjoo Kim, Laura G´omez, Sˆınziana Pˇaduroiu, Leonardo Casta˜neda, and Traian Popescu, with whom I spent a longer time in Bonn. There are Petru Ghenuche and Valeriu Tudose, abroad, who were there when I needed most. I would also like to thank my best friend back in Romania, Melania Chiciuc, for her never-ending support. I also acknowledge my Master’s thesis co-adviser at the University of Bucharest, Mircea Rusu, for his influence on my studies and more. It is quite difficult to catch in a few v vi Acknowledgments words his qualities as a professor, and as a person in general. It was a real privilege for me to have him as a mentor. At the end, I would like to thank my father especially for encouraging me in keeping my way and trying harder. I also thank my mother, in memoriam. Many of her words have been guiding me through life. Contents Abstract ........................................ ix Acronyms ....................................... xi Most Used Mathematical Symbols ....................... xii Preface ......................................... xiii 1 Introduction to Kerr Black Holes 1 1.1 Introduction.................................... 1 1.2 Kerrsolution ................................... 4 1.3 Kerr black holes in Boyer-Lindquist coordinates . .......... 5 1.4 OrbitsintheKerrmetric ........................... 8 1.5 Stretched horizon – membrane paradigm . ..... 10 2 Magnetic Connection Model for Launching Relativistic Jets from Kerr Black Holes 11 2.1 Introduction.................................... 12 2.2 Basicassumptions ................................ 17 2.3 Massflowrateintothejets .. .. .. .. .. .. .. .. 21 2.4 Angular momentum and energy conservation laws . ...... 24 2.5 Launchingpowerofthejets . 25 2.6 Rate of the disk angular momentum removed by the jets . ...... 32 2.7 Efficiencyofjetlaunching . 33 2.8 Spin evolution of the black hole . 34 2.9 Relevance to the observational data . ...... 36 2.9.1 Maximum lifetime of the AGN from the black hole spin-down power 36 2.9.2 On the relation between the spin-down power of a black hole and the particle maximum energy in the jets . 38 2.9.3 On the relation between the spin-down power of a black hole and the observed radio flux-density from flat-spectrum core source . ..... 39 2.10 Summaryandconclusions . 40 3 Ultra-High-Energy Cosmic Ray Contribution from the Spin-Down Power of Black Holes 45 3.1 Introduction.................................... 45 3.2 Modeldescription................................ 52 3.2.1 Modelconditions............................. 52 3.2.2 Magnetic field scaling along a steady jet . 52 3.2.3 Electron and proton number densities . 54 3.2.4 Particle energy distribution . 55 vii viii Contents 3.2.5 Self-absorbed synchrotron emission of the jets . ........ 56 3.3 Luminosity and flux of the ultra-high-energy cosmic rays ........... 61 3.4 Maximum particle energy of ultra-high-energy cosmic rays.......... 62 3.4.1 Spatiallimit ............................... 62 3.4.2 Synchrotronlosslimit . 63 3.5 ApplicationtoM87andCenA . 63 3.6 Predictions for nearby galaxies as ultra-high-energy cosmic ray sources . 65 3.7 Summaryandconclusions . 66 4 General Relativistic Magnetohydrodynamics Simulation of Jet Formation from Kerr Black Holes 69 4.1 Introduction.................................... 70 4.2 General relativistic magnetohydrodynamics equations in conservation form 75 4.2.1 3+1 decomposition of the space-time (in the Eulerean formulation) . 75 4.2.2 3+1 decomposition of the energy-momentum tensor . ..... 79 4.2.3 Perfectfluidapproximation . 80 4.2.4 Evolution of the electromagnetic fields . ..... 80 4.2.5 ConservationEquations . 82 4.3 General relativistic magnetohydrodynamics simulation code (Koide et al.) . 85 4.3.1 Metricandcoordinates ......................... 85 4.3.2 General relativistic magnetohydrodynamics equations in zero angular momentumobserver’sframe. 86 4.3.3 Descriptionofthecode ......................... 88 4.4 Simulation of jet formation from a Kerr black hole . ........ 94 4.4.1 Initialconditions . .. .. .. .. .. .. .. .. 94 4.4.2 Numericalresults............................. 95 4.4.3 Comparison with the RAISHIN simulation code (Mizuno et al.) . 108 4.4.4 Comparisonwithotherwork . 110 4.5 Summaryandconclusions . 111 Outlook ........................................ 113 References ....................................... 115 Appendix 1 ...................................... 127 Appendix 2 ...................................... 129 List of Publications ................................. 133 Abstract Relativistic jets are highly collimated plasma outflows that can be present in extra- galactic radio sources, which are associated with active galactic nuclei (AGN). Observations give strong support for the idea that a supermassive black hole (BH), surrounded by an accretion disk, is harbored in the center of an AGN. The jet power can be generally provided by the accretion disk, by the BH rotation, or both. Such powerful jets can also be sites of the origin of ultra-high-energy cosmic rays (UHECRs). In this work, we study the jet formation from rapidly-spinning BHs in the framework of General Relativity and General Relativistic Magnetohydrodynamics, as well as the acceleration of UHECRs in AGN jets. Magnetic connection model for launching relativistic jets from a Kerr black hole: Despite intense efforts to understand the processes responsible for formation of the AGN jets, we still face the problem of exactly how to explain them. Here, we present a model for launching relativistic jets in
Recommended publications
  • Infrared Spectroscopy of Nearby Radio Active Elliptical Galaxies
    The Astrophysical Journal Supplement Series, 203:14 (11pp), 2012 November doi:10.1088/0067-0049/203/1/14 C 2012. The American Astronomical Society. All rights reserved. Printed in the U.S.A. INFRARED SPECTROSCOPY OF NEARBY RADIO ACTIVE ELLIPTICAL GALAXIES Jeremy Mould1,2,9, Tristan Reynolds3, Tony Readhead4, David Floyd5, Buell Jannuzi6, Garret Cotter7, Laura Ferrarese8, Keith Matthews4, David Atlee6, and Michael Brown5 1 Centre for Astrophysics and Supercomputing Swinburne University, Hawthorn, Vic 3122, Australia; [email protected] 2 ARC Centre of Excellence for All-sky Astrophysics (CAASTRO) 3 School of Physics, University of Melbourne, Melbourne, Vic 3100, Australia 4 Palomar Observatory, California Institute of Technology 249-17, Pasadena, CA 91125 5 School of Physics, Monash University, Clayton, Vic 3800, Australia 6 Steward Observatory, University of Arizona (formerly at NOAO), Tucson, AZ 85719 7 Department of Physics, University of Oxford, Denys, Oxford, Keble Road, OX13RH, UK 8 Herzberg Institute of Astrophysics Herzberg, Saanich Road, Victoria V8X4M6, Canada Received 2012 June 6; accepted 2012 September 26; published 2012 November 1 ABSTRACT In preparation for a study of their circumnuclear gas we have surveyed 60% of a complete sample of elliptical galaxies within 75 Mpc that are radio sources. Some 20% of our nuclear spectra have infrared emission lines, mostly Paschen lines, Brackett γ , and [Fe ii]. We consider the influence of radio power and black hole mass in relation to the spectra. Access to the spectra is provided here as a community resource. Key words: galaxies: elliptical and lenticular, cD – galaxies: nuclei – infrared: general – radio continuum: galaxies ∼ 1. INTRODUCTION 30% of the most massive galaxies are radio continuum sources (e.g., Fabbiano et al.
    [Show full text]
  • And Ecclesiastical Cosmology
    GSJ: VOLUME 6, ISSUE 3, MARCH 2018 101 GSJ: Volume 6, Issue 3, March 2018, Online: ISSN 2320-9186 www.globalscientificjournal.com DEMOLITION HUBBLE'S LAW, BIG BANG THE BASIS OF "MODERN" AND ECCLESIASTICAL COSMOLOGY Author: Weitter Duckss (Slavko Sedic) Zadar Croatia Pусскй Croatian „If two objects are represented by ball bearings and space-time by the stretching of a rubber sheet, the Doppler effect is caused by the rolling of ball bearings over the rubber sheet in order to achieve a particular motion. A cosmological red shift occurs when ball bearings get stuck on the sheet, which is stretched.“ Wikipedia OK, let's check that on our local group of galaxies (the table from my article „Where did the blue spectral shift inside the universe come from?“) galaxies, local groups Redshift km/s Blueshift km/s Sextans B (4.44 ± 0.23 Mly) 300 ± 0 Sextans A 324 ± 2 NGC 3109 403 ± 1 Tucana Dwarf 130 ± ? Leo I 285 ± 2 NGC 6822 -57 ± 2 Andromeda Galaxy -301 ± 1 Leo II (about 690,000 ly) 79 ± 1 Phoenix Dwarf 60 ± 30 SagDIG -79 ± 1 Aquarius Dwarf -141 ± 2 Wolf–Lundmark–Melotte -122 ± 2 Pisces Dwarf -287 ± 0 Antlia Dwarf 362 ± 0 Leo A 0.000067 (z) Pegasus Dwarf Spheroidal -354 ± 3 IC 10 -348 ± 1 NGC 185 -202 ± 3 Canes Venatici I ~ 31 GSJ© 2018 www.globalscientificjournal.com GSJ: VOLUME 6, ISSUE 3, MARCH 2018 102 Andromeda III -351 ± 9 Andromeda II -188 ± 3 Triangulum Galaxy -179 ± 3 Messier 110 -241 ± 3 NGC 147 (2.53 ± 0.11 Mly) -193 ± 3 Small Magellanic Cloud 0.000527 Large Magellanic Cloud - - M32 -200 ± 6 NGC 205 -241 ± 3 IC 1613 -234 ± 1 Carina Dwarf 230 ± 60 Sextans Dwarf 224 ± 2 Ursa Minor Dwarf (200 ± 30 kly) -247 ± 1 Draco Dwarf -292 ± 21 Cassiopeia Dwarf -307 ± 2 Ursa Major II Dwarf - 116 Leo IV 130 Leo V ( 585 kly) 173 Leo T -60 Bootes II -120 Pegasus Dwarf -183 ± 0 Sculptor Dwarf 110 ± 1 Etc.
    [Show full text]
  • Arxiv:0811.1848V3 [Astro-Ph] 18 Dec 2008 Cieglci Uli Ore O Lr Iheeg Cosmi Energy High Biermann Ultra L
    Active Galactic Nuclei: Sources for ultra high energy cosmic rays? Peter L. Biermannabcde, Julia K. Beckerf g, Laurent¸iu Carametea h, Alex Curut¸iua, Ralph Engele, Heino Falckei j, L´aszl´o A.´ Gergelyk l, P. Gina Isare h, Ioana C. Mari¸se, Athina Melim, Karl-Heinz Kampertn, Todor Stanevo, Oana Ta¸sc˘aun, Christian Ziera p aMPI for Radioastronomy, Bonn, Germany bDept. of Phys. & Astron., Univ. of Bonn, Germany cDept. of Phys. & Astr., Univ. of Alabama, Tuscaloosa, AL, USA dDept. of Phys., Univ. of Alabama at Huntsville, AL, USA eInst. Nucl. Phys. FZ, Karlsruhe Inst. of Techn. (KIT), Germany f Institution f¨or Fysik, G¨oteborgs Univ., Sweden gDept. of Phys., Univ. Dortmund, Dortmund, Germany hInstitute for Space Studies, Bucharest, Romania iDept. of Astrophys., IMAP, Radboud Univ., Nijmegen, Netherlands jASTRON, Dwingeloo, Netherlands kDept. Appl. Sci., London South Bank University, UK lDept. of Theoret. & Exp. Phys., Univ. of Szeged, Szeged, Hungary mPhysik. Inst. Univ. Erlangen-N¨urnberg, Germany nPhys. Dept., Univ. Wuppertal, Germany oBartol Research Inst., Univ. of Delaware, Newark, DE, USA arXiv:0811.1848v3 [astro-ph] 18 Dec 2008 pRaman Res. Inst., Bangalore, India The origin of ultra high energy cosmic rays promises to lead us to a deeper understanding of the structure of matter. This is possible through the study of particle collisions at center-of-mass energies in interactions far larger than anything possible with the Large Hadron Collider, albeit at the substantial cost of no control over the sources and interaction sites. For the extreme energies we have to identify and understand the sources first, before trying to use them as physics laboratories.
    [Show full text]
  • 190 Index of Names
    Index of names Ancora Leonis 389 NGC 3664, Arp 005 Andriscus Centauri 879 IC 3290 Anemodes Ceti 85 NGC 0864 Name CMG Identification Angelica Canum Venaticorum 659 NGC 5377 Accola Leonis 367 NGC 3489 Angulatus Ursae Majoris 247 NGC 2654 Acer Leonis 411 NGC 3832 Angulosus Virginis 450 NGC 4123, Mrk 1466 Acritobrachius Camelopardalis 833 IC 0356, Arp 213 Angusticlavia Ceti 102 NGC 1032 Actenista Apodis 891 IC 4633 Anomalus Piscis 804 NGC 7603, Arp 092, Mrk 0530 Actuosus Arietis 95 NGC 0972 Ansatus Antliae 303 NGC 3084 Aculeatus Canum Venaticorum 460 NGC 4183 Antarctica Mensae 865 IC 2051 Aculeus Piscium 9 NGC 0100 Antenna Australis Corvi 437 NGC 4039, Caldwell 61, Antennae, Arp 244 Acutifolium Canum Venaticorum 650 NGC 5297 Antenna Borealis Corvi 436 NGC 4038, Caldwell 60, Antennae, Arp 244 Adelus Ursae Majoris 668 NGC 5473 Anthemodes Cassiopeiae 34 NGC 0278 Adversus Comae Berenices 484 NGC 4298 Anticampe Centauri 550 NGC 4622 Aeluropus Lyncis 231 NGC 2445, Arp 143 Antirrhopus Virginis 532 NGC 4550 Aeola Canum Venaticorum 469 NGC 4220 Anulifera Carinae 226 NGC 2381 Aequanimus Draconis 705 NGC 5905 Anulus Grahamianus Volantis 955 ESO 034-IG011, AM0644-741, Graham's Ring Aequilibrata Eridani 122 NGC 1172 Aphenges Virginis 654 NGC 5334, IC 4338 Affinis Canum Venaticorum 449 NGC 4111 Apostrophus Fornac 159 NGC 1406 Agiton Aquarii 812 NGC 7721 Aquilops Gruis 911 IC 5267 Aglaea Comae Berenices 489 NGC 4314 Araneosus Camelopardalis 223 NGC 2336 Agrius Virginis 975 MCG -01-30-033, Arp 248, Wild's Triplet Aratrum Leonis 323 NGC 3239, Arp 263 Ahenea
    [Show full text]
  • Active Galactic Nuclei: Sources for Ultra High Energy Cosmic Rays!
    ACTIVE GALACTIC NUCLEI: SOURCES FOR ULTRA HIGH ENERGY COSMIC RAYS! Peter L. Biermann1,2,3,4, Laurent¸iu Caramete1,5, Alex Curut¸iu1, Ioana Dut¸an1, Ioana C. Mari¸s6, Oana Ta¸sc˘au7, Julia Becker8,9, Ralph Engel6, Heino Falcke10, Karl-Heinz Kampert7, & Todor Stanev11 1 MPI for Radioastronomy, Bonn, Germany 2 Dept. of Phys. & Astron., Univ. of Bonn, Germany 3 Dept. of Phys. & Astr., Univ. of Alabama, Tuscaloosa, AL, USA 4 Dept. of Phys., Univ. of Alabama at Huntsville, AL, USA 1 5 Institute for Space Studies, Bucharest, Romania 6 FZ Karlsruhe, and Phys. Dept., Univ. Karlsruhe, Germany 7 Phys. Dept., Univ. Wuppertal, Germany 8 Institution f¨orFysik, G¨oteborgs Univ., Sweden 9 Dept. of Phys., Univ. Dortmund, Dortmund, Germany 10 Dept. of Astrophys., IMAP, Radboud Univ., Nijmegen, Netherlands 11 Bartol Research Inst., Univ. of Delaware, Newark, DE, USA www.mpifr-bonn.mpg.de/div/theory 2 Abstract: Ultra high energy cosmic rays were discovered over forty years ago (Linsley 1963). The first prediction has been that due to in- teraction with the microwave background their spectrum should show a turn-down near 5 1019 eV (Greisen 1966, Zatsepin & Kuzmin 1966): this has now been confirmed by both HiRes and Auger (ICRC Mexico 2007). While many sites of origin have been proposed, only one argument demonstrated that protons of order 1021 eV are required in a source region to ex- plain observations, specifically the ubiquitous turnoff in the optical synchrotron spectrum near 3 1014 Hz (Biermann & Strittmatter 1987); this argument led to the second prediction that radio galaxies are sources of ultra high en- ergy cosmic rays, one rare and specific class of active galactic nuclei (AGN).
    [Show full text]
  • Ngc Catalogue Ngc Catalogue
    NGC CATALOGUE NGC CATALOGUE 1 NGC CATALOGUE Object # Common Name Type Constellation Magnitude RA Dec NGC 1 - Galaxy Pegasus 12.9 00:07:16 27:42:32 NGC 2 - Galaxy Pegasus 14.2 00:07:17 27:40:43 NGC 3 - Galaxy Pisces 13.3 00:07:17 08:18:05 NGC 4 - Galaxy Pisces 15.8 00:07:24 08:22:26 NGC 5 - Galaxy Andromeda 13.3 00:07:49 35:21:46 NGC 6 NGC 20 Galaxy Andromeda 13.1 00:09:33 33:18:32 NGC 7 - Galaxy Sculptor 13.9 00:08:21 -29:54:59 NGC 8 - Double Star Pegasus - 00:08:45 23:50:19 NGC 9 - Galaxy Pegasus 13.5 00:08:54 23:49:04 NGC 10 - Galaxy Sculptor 12.5 00:08:34 -33:51:28 NGC 11 - Galaxy Andromeda 13.7 00:08:42 37:26:53 NGC 12 - Galaxy Pisces 13.1 00:08:45 04:36:44 NGC 13 - Galaxy Andromeda 13.2 00:08:48 33:25:59 NGC 14 - Galaxy Pegasus 12.1 00:08:46 15:48:57 NGC 15 - Galaxy Pegasus 13.8 00:09:02 21:37:30 NGC 16 - Galaxy Pegasus 12.0 00:09:04 27:43:48 NGC 17 NGC 34 Galaxy Cetus 14.4 00:11:07 -12:06:28 NGC 18 - Double Star Pegasus - 00:09:23 27:43:56 NGC 19 - Galaxy Andromeda 13.3 00:10:41 32:58:58 NGC 20 See NGC 6 Galaxy Andromeda 13.1 00:09:33 33:18:32 NGC 21 NGC 29 Galaxy Andromeda 12.7 00:10:47 33:21:07 NGC 22 - Galaxy Pegasus 13.6 00:09:48 27:49:58 NGC 23 - Galaxy Pegasus 12.0 00:09:53 25:55:26 NGC 24 - Galaxy Sculptor 11.6 00:09:56 -24:57:52 NGC 25 - Galaxy Phoenix 13.0 00:09:59 -57:01:13 NGC 26 - Galaxy Pegasus 12.9 00:10:26 25:49:56 NGC 27 - Galaxy Andromeda 13.5 00:10:33 28:59:49 NGC 28 - Galaxy Phoenix 13.8 00:10:25 -56:59:20 NGC 29 See NGC 21 Galaxy Andromeda 12.7 00:10:47 33:21:07 NGC 30 - Double Star Pegasus - 00:10:51 21:58:39
    [Show full text]
  • The Duty Cycle of Radio-Mode Feedback in Complete Samples of Clusters
    Mon. Not. R. Astron. Soc. 427, 3468–3488 (2012) doi:10.1111/j.1365-2966.2012.22083.x The duty cycle of radio-mode feedback in complete samples of clusters L. Bˆırzan,1 D. A. Rafferty,1 P. E. J. Nulsen,2 B. R. McNamara,2,3,4 H. J. A. Rottgering,¨ 1 M. W. Wise5 and R. Mittal6 1Leiden Observatory, Leiden University, Oort Gebouw, PO Box 9513, 2300 RA Leiden, the Netherlands 2Harvard–Smithsonian Centre for Astrophysics, 60 Garden St., Cambridge, MA 02138, USA 3Department of Physics and Astronomy, University of Waterloo, Waterloo, ON N2L 2G1, Canada 4Perimeter Institute for Theoretical Physics, Waterloo, ON N2L 2Y5, Canada 5Netherlands Institute for Radio Astronomy (ASTRON), PO Box 2, 7990 AA Dwingeloo, the Netherlands 6Chester F. Carlson centre for Imaging Science, Rochester Institute of Technology, Rochester, NY 14623, USA Accepted 2012 September 7. Received 2012 September 6; in original form 2012 June 30 Downloaded from ABSTRACT The Chandra X-ray Observatory has revealed X-ray bubbles in the intracluster medium (ICM) of many nearby cooling-flow clusters. The bubbles trace feedback that is thought to couple http://mnras.oxfordjournals.org/ the central active galactic nucleus (AGN) to the ICM, helping to stabilize cooling flows and govern the evolution of massive galaxies. However, the prevalence and duty cycle of such AGN outbursts is not well understood. To this end, we study how cooling is balanced by bubble heating for complete samples of clusters (the Brightest 55 clusters of galaxies, hereafter B55, and the HIghest X-ray FLUx Galaxy Cluster Sample, HIFLUGCS). We find that the radio luminosity of the central galaxy only exceeds 2.5 × 1030 erg s−1 Hz−1 in cooling-flow clusters.
    [Show full text]
  • Hydrodynamical Simulations of Colliding Jets: Modeling 3C 75 S
    Draft version June 17, 2021 Preprint typeset using LATEX style emulateapj v. 5/2/11 HYDRODYNAMICAL SIMULATIONS OF COLLIDING JETS: MODELING 3C 75 S. M. Molnar1, H.-Y. Schive2, M. Birkinshaw3, T. Chiueh4,5 G. Musoke3, and A. J. Young3 Draft version June 17, 2021 ABSTRACT Radio observations suggest that 3C 75, located in the dumbbell shaped galaxy NGC 1128 at the center of Abell 400, hosts two colliding jets. Motivated by this source, we perform three- dimensional hydrodynamical simulations using a modified version of the GPU-accelerated Adaptive- MEsh-Refinement hydrodynamical parallel code (GAMER) to study colliding extragalactic jets. We find that colliding jets can be cast into two categories: 1) bouncing jets, in which case the jets bounce off each other keeping their identities, and 2) merging jets, when only one jet emerges from the col- lision. Under some conditions the interaction causes the jets to break up into oscillating filaments of opposite helicity, with consequences for their downstream stability. When one jet is significantly faster than the other and the impact parameter is small, the jets merge; the faster jet takes over the slower one. In the case of merging jets, the oscillations of the filaments, in projection, may show a feature which resembles a double helix, similar to the radio image of 3C 75. Thus we interpret the morphology of 3C 75 as a consequence of the collision of two jets with distinctly different speeds at a small impact parameter, with the faster jet breaking up into two oscillating filaments. Subject headings: galaxies: clusters: general { galaxies: clusters: individual (Abell 400) { galaxies: clusters: intracluster medium { methods: numerical { extragalactic jets 1.
    [Show full text]
  • The Electromagnetic Radiation Field
    The electromagnetic radiation field A In this appendix, we will briefly review the most important The flux is measured in units of erg cm2 s1 Hz1.Ifthe properties of a radiation field. We thereby assume that the radiation field is isotropic, F vanishes. In this case, the same reader has encountered these quantities already in a different amount of radiation passes through the surface element in context. both directions. The mean specific intensity J is defined as the average of I over all angles, A.1 Parameters of the radiation field Z 1 J D d!I ; (A.3) The electromagnetic radiation field is described by the spe- 4 cific intensity I, which is defined as follows. Consider a D surface element of area dA. The radiation energy which so that, for an isotropic radiation field, I J.Thespecific passes through this area per time interval dt from within a energy density u is related to J according to solid angle element d! around a direction described by the n 4 unit vector , with frequency in the range between and u D J ; (A.4) C d,is c where u is the energy of the radiation field per D dE I dA cos dt d! d; (A.1) volume element and frequency interval, thus measured in erg cm3 Hz1. The total energy density of the radiation is where describes the angle between the direction n of the obtained by integrating u over frequency. In the same way, light and the normal vector of the surface element. Then, the intensity of the radiation is obtained by integrating the dA cos is the area projected in the direction of the infalling specific intensity I over .
    [Show full text]
  • The Duty Cycle of Radiomode Feedback in Complete
    Mon. Not. R. Astron. Soc. 427, 3468–3488 (2012) doi:10.1111/j.1365-2966.2012.22083.x The duty cycle of radio-mode feedback in complete samples of clusters L. Bˆırzan,1 D. A. Rafferty,1 P. E. J. Nulsen,2 B. R. McNamara,2,3,4 H. J. A. Rottgering,¨ 1 M. W. Wise5 and R. Mittal6 1Leiden Observatory, Leiden University, Oort Gebouw, PO Box 9513, 2300 RA Leiden, the Netherlands 2Harvard–Smithsonian Centre for Astrophysics, 60 Garden St., Cambridge, MA 02138, USA 3Department of Physics and Astronomy, University of Waterloo, Waterloo, ON N2L 2G1, Canada 4Perimeter Institute for Theoretical Physics, Waterloo, ON N2L 2Y5, Canada 5Netherlands Institute for Radio Astronomy (ASTRON), PO Box 2, 7990 AA Dwingeloo, the Netherlands 6Chester F. Carlson centre for Imaging Science, Rochester Institute of Technology, Rochester, NY 14623, USA Accepted 2012 September 7. Received 2012 September 6; in original form 2012 June 30 ABSTRACT The Chandra X-ray Observatory has revealed X-ray bubbles in the intracluster medium (ICM) of many nearby cooling-flow clusters. The bubbles trace feedback that is thought to couple the central active galactic nucleus (AGN) to the ICM, helping to stabilize cooling flows and govern the evolution of massive galaxies. However, the prevalence and duty cycle of such AGN outbursts is not well understood. To this end, we study how cooling is balanced by bubble heating for complete samples of clusters (the Brightest 55 clusters of galaxies, hereafter B55, and the HIghest X-ray FLUx Galaxy Cluster Sample, HIFLUGCS). We find that the radio luminosity of the central galaxy only exceeds 2.5 × 1030 erg s−1 Hz−1 in cooling-flow clusters.
    [Show full text]
  • Appendix: Swift's Deep Sky Catalogs
    Appendix: Swift’s Deep Sky Catalogs © Springer International Publishing AG 2017 233 G.W. Kronk, Lewis Swift, Historical & Cultural Astronomy, DOI 10.1007/978-3-319-63721-1 Catalog 1 (Warner observatory) Equinox 1885.0 Equinox 2000.0 Swift object Date Original V no. of disc RA DEC Description RA DEC NGC/IC discoverer Type Mag Size Remarks h m s ° ′ ″ h m s ° ′ ″ S1–1 1884 0 4 32 +28 21 5 vvF; vS; E; B * 0 10 32.8 +28 59 46 NGC 27 L. Swift GX 13.5 1.2′ × 0.5′ PGC 742 Aug 3 nr S1–2 1884 2 2 35 +7 25 0 vF; pS; vvE; 2 8 56.3 +7 58 17 NGC 827 W. Herschel GX 12.7 2.2′ × 0.8′ PGC 8196* Oct 9 spindle; cannot (1784) be G. C. 493 [NGC 827], is not “am st”, nearest * is 5′ distant. Did not see [GC] 493 [NGC 827], but saw [GC] 5223 [NGC 840]. H. description must apply to some other nebula. S1–3 1884 2 27 22 +9 13 46 vF; cE. 2 33 22.7 +9 36 6 NGC 975 L. Swift GX 13.1 1.1′ × 0.8′ PGC 9735* Nov 9 S1–4 1884 2 45 2 −2 13 6 F; vE. 2 50 39.2 −1 44 3 NGC 1121 L. Swift GX 12.9 0.9′ × 0.4′ PGC 10789 Nov 9 S1–5 1884 3 1 31 +40 27 0 S; R; vvF. Right 3 9 42.2 +40 53 35 NGC L.
    [Show full text]
  • Apparent Magnitude = 10.5 11.5 ± 0.8 Million Light- Years (3.5 ± 0.3 Megaparsecs )
    1 2018 Div. C (High School) Astronomy Help Session Sunday, Feb. 17th, 2019 Stellar Evolution in normal and star burst galaxies Scott Jackson Mt. Cuba Astronomical Observatory • SO competition on March 2nd . • Resources – two computers or two 3 ring binder or one laptop plus one 3 ring binder – Programmable calculator – Connection to the internet is not allowed! – Help session before competition at Mt. Cuba Astronomical Observatory 2 3 4 Study aid -1 • Google each object, – Know what they look like in different parts of the spectrum. For example, the IR, optical, UV and Xray – Understand what each part of the spectrum means – Have a good qualitative feel for what the object is doing or has done within the astrophysical concepts that the student is being asked to know. 5 Study aid - 2 • Know the algebra behind the physics – Just because you think you have the right “equation” to use does not mean you know how to use it!!! – Hint for math problems: Solve equations symbolically BEFORE you put in numbers. Things tend to cancel out including parameters you do not need to have values for. – Know how to use scientific notation. 6 The test – 2 parts • Part 1 – multiple choice and a couple fill in the blanks • Part 2 – word problems for astrophysics there will be some algebra Solve the equations symbolically first then put in numbers!!!! Hint: most problems will not need a calculator if done this way Stellar evolution 7 stellar classification, spectral features and chemical composition, luminosity, blackbody radiation, color index H-R diagram transitions, star formation, Topics Cepheids, Emphasis from rules RR Lyrae stars, Type Ia & Type II supernovas, neutron stars, pulsars, stellar mass black holes, supermassive black holes, X-ray & gamma-ray binary systems, ultraluminous X-ray sources (ULXs), globular clusters, stellar populations, normal & starburst galaxies, galactic structure and interactions, gravitational waves.
    [Show full text]