Planetary-Scale Astronomical Bench
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Radio Astronomy & Radio Telescopes
Radio Astronomy & Radio Telescopes Tasso Tzioumis ([email protected]) Australia Telescope National Facility (ATNF) sms2020, Stellenbosch 2-6 March 2020 CSIRO ASTRONOMY AND SPACE SCIENCE Radio Astronomy – ITU definition 1.13 radio astronomy: Astronomy based on the reception of radio waves of cosmic origin. 1.5 radio waves or hertzian waves: Electromagnetic waves of frequencies arbitrarily lower than 3 000 GHz, propagated in space without artificial guide. • Astronomy covers the whole electromagnetic spectrum • Radio astronomy is the “low energy” part of the spectrum é 3 000 GHz Radioastronomy & Radio telescopes | Tasso Tzioumis Radio Astronomy “special” characteristics Technical challenges • Very faint signals – measured in 10-26 W/m2/Hz (-260 dBW) • “Power collected by all radiotelescopes since the start of radio astronomy would light a 1W bulb for less than 1 second” • à Need “sensitivity” i.e. large antennas and/or arrays of many antennas • à Very susceptible to intereference • Celestial structures at all scales: from very large to very small • à Need “spatial resolution” i.e. ability to see the details at all scales • à Need large antennas and/or arrays of many antennas • Astronomical events at all timescales(from < 1ms to > millions years) & and at all spectral resolutions (from < 1 Hz to GHz) • à Need very high time and frequency resolution • à Sensitive telescopes and arrays & extreme technical challenges Radioastronomy & Radio telescopes | Tasso Tzioumis Radio Astronomy “special” characteristics Scientific challenges • Radio -
Ty996i the Astronomical Journal Volume 71, Number
coPC THE ASTRONOMICAL JOURNAL VOLUME 71, NUMBER 6 AUGUST 1966 TY996I Observations of Comets, Minor Planets, and Satellites Elizabeth Roemer* and Richard E. Lloyd U. S. Naval Observatory, Flagstaff Station, Arizona (Received 10 May 1966) Accurate positions and descriptive notes are presented for 38 comets, 33 minor planets, 5 faint natural satellites, and Pluto, for which astrometric reduction of the series of Flagstaff observations has been completed. THE 1022 positions and descriptive notes presented reference star positions; therefore, she bears responsi- here supplement those given by Roemer (1965), bility for the accuracy of the results given here. who also described the program, the equipment used, Coma diameters and tail dimensions given in the and the procedures of observation and of reduction. Notes to Table I refer to the exposures taken for In this paper as in the earlier one, the participation astrometric purposes unless otherwise stated. In of those who shared in critical phases of the work is general, longer exposures show more extensive head and indicated in the Obs/Meas column of Table I according tail structure. to the following letters: For brighter comets the minimum exposure is determined by the necessity of recording measurable R=Elizabeth Roemer. images of 12th-13th magnitude reference stars. On Part-time assistants under contract Nonr-3342(00) such exposures the position of the nuclear condensation with Lowell Observatory: may be more or less obscured by the overexposed coma and be correspondingly difficult and uncertain to L = Richard E. Lloyd, measure. T = Maryanna Thomas, A colon has been used to indicate greater than normal S = Marjorie K. -
On the Accuracy of Restricted Three-Body Models for the Trojan Motion
DISCRETE AND CONTINUOUS Website: http://AIMsciences.org DYNAMICAL SYSTEMS Volume 11, Number 4, December 2004 pp. 843{854 ON THE ACCURACY OF RESTRICTED THREE-BODY MODELS FOR THE TROJAN MOTION Frederic Gabern1, Angel` Jorba1 and Philippe Robutel2 Departament de Matem`aticaAplicada i An`alisi Universitat de Barcelona Gran Via 585, 08007 Barcelona, Spain1 Astronomie et Syst`emesDynamiques IMCCE-Observatoire de Paris 77 Av. Denfert-Rochereau, 75014 Paris, France2 Abstract. In this note we compare the frequencies of the motion of the Trojan asteroids in the Restricted Three-Body Problem (RTBP), the Elliptic Restricted Three-Body Problem (ERTBP) and the Outer Solar System (OSS) model. The RTBP and ERTBP are well-known academic models for the motion of these asteroids, and the OSS is the standard model used for realistic simulations. Our results are based on a systematic frequency analysis of the motion of these asteroids. The main conclusion is that both the RTBP and ERTBP are not very accurate models for the long-term dynamics, although the level of accuracy strongly depends on the selected asteroid. 1. Introduction. The Restricted Three-Body Problem models the motion of a particle under the gravitational attraction of two point masses following a (Keple- rian) solution of the two-body problem (a general reference is [17]). The goal of this note is to discuss the degree of accuracy of such a model to study the real motion of an asteroid moving near the Lagrangian points of the Sun-Jupiter system. To this end, we have considered two restricted three-body problems, namely: i) the Circular RTBP, in which Sun and Jupiter describe a circular orbit around their centre of mass, and ii) the Elliptic RTBP, in which Sun and Jupiter move on an elliptic orbit. -
Astrocladistics of the Jovian Trojan Swarms
MNRAS 000,1–26 (2020) Preprint 23 March 2021 Compiled using MNRAS LATEX style file v3.0 Astrocladistics of the Jovian Trojan Swarms Timothy R. Holt,1,2¢ Jonathan Horner,1 David Nesvorný,2 Rachel King,1 Marcel Popescu,3 Brad D. Carter,1 and Christopher C. E. Tylor,1 1Centre for Astrophysics, University of Southern Queensland, Toowoomba, QLD, Australia 2Department of Space Studies, Southwest Research Institute, Boulder, CO. USA. 3Astronomical Institute of the Romanian Academy, Bucharest, Romania. Accepted XXX. Received YYY; in original form ZZZ ABSTRACT The Jovian Trojans are two swarms of small objects that share Jupiter’s orbit, clustered around the leading and trailing Lagrange points, L4 and L5. In this work, we investigate the Jovian Trojan population using the technique of astrocladistics, an adaptation of the ‘tree of life’ approach used in biology. We combine colour data from WISE, SDSS, Gaia DR2 and MOVIS surveys with knowledge of the physical and orbital characteristics of the Trojans, to generate a classification tree composed of clans with distinctive characteristics. We identify 48 clans, indicating groups of objects that possibly share a common origin. Amongst these are several that contain members of the known collisional families, though our work identifies subtleties in that classification that bear future investigation. Our clans are often broken into subclans, and most can be grouped into 10 superclans, reflecting the hierarchical nature of the population. Outcomes from this project include the identification of several high priority objects for additional observations and as well as providing context for the objects to be visited by the forthcoming Lucy mission. -
Interferometry and Aperture Synthesis in Order to Understand the Re
Summer Student Lecture Notes INTERFEROMETRY AND APERTURE SYNTHESIS Bruce Balick July 1973 The following pages are reprinted (with corrections) from Balick, B. 1972, thesis (Cornell University) CHAPTER II INTERFEROMETRY AND APERTURE SYNTHESIS Electromagnetic radiation is a wave phenomena, consequently in- struments used to observe this radiation are subject to diffraction limi- tations on their resolution. The angular limit, A, is given approxi- mately by AS6 D/A, where D is the aperture dimension and X is the obscwrving wavelcngth; for radio work - _____A - 140 B/cm) min -arc [D/feet] Thus the 300-foot telescope has a maximum resolution of 6' .arc at XAll cm, whereas a 10-cm aperture optical telescope has a diffraction limit of 1" are at optical wavelengths. (The same high resolution would require ap- ertures 1-1000 km in diameter at radio wavelengths.) To obtain high resolution at radio wavelengths, partially fill- ed apertures of large diameter can be synthesized. For this, two tele- scopes separated by a baseline B can be used to simulate the response of a nearly circular annulus of diameter IB. The telescope pair is con- figured in such a manner that it is best described as an interferometer in the ordinary optical sense. By moving the telescopes to obtain inter- ferometers of different spacings, annuli of different sizes can be simu- lated. The results obtained on the various spacings can be added appropriately to synthesize the response of a single telescope of very large diameter, and thereby yield maps of high resolution. For example, the interferometer of the National Radio Astronomy Observatory (NRAO) can 10 S. -
Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing
THESIS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing ERIK RYMAN Division of Computer Engineering Department of Computer Science and Engineering CHALMERS UNIVERSITY OF TECHNOLOGY Göteborg, Sweden 2018 Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing Erik Ryman ISBN 978-91-7597-751-5 Copyright © Erik Ryman, 2018. Doktorsavhandlingar vid Chalmers tekniska högskola Ny serie Nr 4432 ISSN 0346-718X Technical report No. 156D Department of Computer Science and Engineering VLSI Research Group Department of Computer Science and Engineering Chalmers University of Technology SE-412 96 GÖTEBORG, Sweden Phone: +46 (0)31-772 10 00 Author e-mail: [email protected] Cover: A 64-channel cross-correlator unit, including chip photos of digital correlator and analog-to-digital converter. Printed by Chalmers Reproservice Göteborg, Sweden 2018 Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing Erik Ryman Department of Computer Science and Engineering, Chalmers University of Technology ABSTRACT An ever-increasing demand for weather prediction and high climate modelling ac- curacy drives the need for better atmospheric data collection. These demands in- clude better spatial and temporal coverage of mainly humidity and temperature distributions in the atmosphere. A new type of remote sensing satellite technol- ogy is emerging, originating in the field of radio astronomy where telescope aper- ture upscaling could not keep up with the increasing demand for higher resolution. Aperture synthesis imaging takes an array of receivers and emulates apertures ex- tending way beyond what is possible with any single antenna. In the field of Earth remote sensing, the same idea could be used to construct satellites observing in the microwave region at a high resolution with foldable antenna arrays. -
Book of Abstracts
Dissecting the Universe - Workshop on Results from High-Resolution VLBI Monday 30 November 2015 - Wednesday 02 December 2015 Max-Planck-Institut für Radioastronomie, Bonn, Germany Book of Abstracts Contents GMVA Observations of M87 and Status Report of the GLT Project . 1 Water megamasers at high resolution . 1 Millimeter VLBI Observations of the Twin-Jet-System in NGC1052 . 1 First 3mm-VLBI imaging of the two-sided jet in Cygnus A: zooming into the launching region . 2 New insight into AGN-jets: they are alive! . 2 The connection between the mm VLBI jet and the gamma-ray emission in the blazar CTA102 and the radio galaxy 3C120 . 2 New Developments with the Event Horizon Telescope . 3 Dissecting TeV blazars: Space VLBI study of the BL Lac source Markarian 501 . 3 VLBI Studies of Star Forming Regions using Molecular Masers . 4 The farthest view with overterrestrial baselines . 4 Probing the innermost regions of AGN jets and their magnetic fields with RadioAstron 4 What has VLBI at the highest resolutions taught us about the VLBI "core"? . 5 The most compact H2O maser spots and their locations in W3 IRS5 . 5 A physical model for the radio and GeV emission from the microquasar LS I +61◦303 6 Detection and Implications of Horizon-Scale Polarization in Sgr A* . 7 The Discovery and Implications of Refractive Substructure for VLBI at the Highest Angular Resolutions . 7 Microarcsecond Structure of the Parsec Scale Jet of the Quasar 3C454.3 . 7 Jets from Water-Disk-Megamaser Galaxies . 8 Unlocking the secrets of PKS 1502+106. Synergies between mm-VLBI and single-dish monitoring . -
Aperture Synthesis James Di Francesco National Research Council of Canada North American ALMA Regional Center – Victoria
A Crash Course in ! Radio Astronomy and Interferometry:! 2. Aperture Synthesis James Di Francesco National Research Council of Canada North American ALMA Regional Center – Victoria (thanks to S. Dougherty, C. Chandler, D. Wilner & C. Brogan) Aperture Synthesis Output of a Filled Aperture • Signals at each point in the aperture are brought together in phase at the antenna output (the focus) • Imagine the aperture to be subdivided into N smaller elementary areas; the voltage, V(t), at the output is the sum of the contributions ΔVi(t) from the N individual aperture elements: V(t) = ∑ΔVi (t) € Aperture Synthesis Aperture Synthesis: Basic Concept • The radio power measured by a receiver attached to the telescope is proportional to a running time average of the square of the output voltage: 2 P V V V ∝ (∑Δ i ) = ∑∑ (Δ iΔ k ) 2 = ∑ ΔVi + ∑∑ ΔViΔVk i≠k • Any€ measurement with the large filled-aperture telescope can be written as a sum, in which each term depends on contributions from only two of the N aperture€ elements • Each term 〈ΔViΔVk〉 can be measured with two small antennas, if we place them at locations i and k and measure the average product of their output voltages with a correlation (multiplying) receiver Aperture Synthesis Aperture Synthesis: Basic Concept • If the source emission is unchanging, there is no need to measure all the pairs at one time • One could imagine sequentially combining pairs of signals. For N sub-apertures there will be N(N-1)/2 pairs to combine • Adding together all the terms effectively “synthesizes” one measurement -
Appendix 1 1311 Discoverers in Alphabetical Order
Appendix 1 1311 Discoverers in Alphabetical Order Abe, H. 28 (8) 1993-1999 Bernstein, G. 1 1998 Abe, M. 1 (1) 1994 Bettelheim, E. 1 (1) 2000 Abraham, M. 3 (3) 1999 Bickel, W. 443 1995-2010 Aikman, G. C. L. 4 1994-1998 Biggs, J. 1 2001 Akiyama, M. 16 (10) 1989-1999 Bigourdan, G. 1 1894 Albitskij, V. A. 10 1923-1925 Billings, G. W. 6 1999 Aldering, G. 4 1982 Binzel, R. P. 3 1987-1990 Alikoski, H. 13 1938-1953 Birkle, K. 8 (8) 1989-1993 Allen, E. J. 1 2004 Birtwhistle, P. 56 2003-2009 Allen, L. 2 2004 Blasco, M. 5 (1) 1996-2000 Alu, J. 24 (13) 1987-1993 Block, A. 1 2000 Amburgey, L. L. 2 1997-2000 Boattini, A. 237 (224) 1977-2006 Andrews, A. D. 1 1965 Boehnhardt, H. 1 (1) 1993 Antal, M. 17 1971-1988 Boeker, A. 1 (1) 2002 Antolini, P. 4 (3) 1994-1996 Boeuf, M. 12 1998-2000 Antonini, P. 35 1997-1999 Boffin, H. M. J. 10 (2) 1999-2001 Aoki, M. 2 1996-1997 Bohrmann, A. 9 1936-1938 Apitzsch, R. 43 2004-2009 Boles, T. 1 2002 Arai, M. 45 (45) 1988-1991 Bonomi, R. 1 (1) 1995 Araki, H. 2 (2) 1994 Borgman, D. 1 (1) 2004 Arend, S. 51 1929-1961 B¨orngen, F. 535 (231) 1961-1995 Armstrong, C. 1 (1) 1997 Borrelly, A. 19 1866-1894 Armstrong, M. 2 (1) 1997-1998 Bourban, G. 1 (1) 2005 Asami, A. 7 1997-1999 Bourgeois, P. 1 1929 Asher, D. -
H I Observations of Two New Dwarf Galaxies: Pisces a and B with the SKA Pathfinder KAT-7? C
A&A 587, L3 (2016) Astronomy DOI: 10.1051/0004-6361/201527910 & c ESO 2016 Astrophysics Letter to the Editor H I observations of two new dwarf galaxies: Pisces A and B with the SKA Pathfinder KAT-7? C. Carignan1;2, Y. Libert1, D. M. Lucero1;4, T. H. Randriamampandry1, T. H. Jarrett1, T. A. Oosterloo3;4, and E. J. Tollerud5 1 Department of Astronomy, University of Cape Town, Private Bag X3, 7701 Rondebosch, South Africa e-mail: [email protected] 2 Observatoire d’Astrophysique de l’Université de Ouagadougou, BP 7021, Ouagadougou 03, Burkina Faso 3 Netherlands Institute for Radio Astronomy (ASTRON), Postbus 2, 7990 AA Dwingeloo, The Netherlands 4 Kapteyn Astronomical Institute, University of Groningen, PO Box 800, 9700 AV Groningen, The Netherlands 5 Space Telescope Science Institute, 3700 San Martin Dr, Baltimore, MD 21218, USA Received 7 December 2015 / Accepted 3 January 2016 ABSTRACT Context. Pisces A and Pisces B are the only two galaxies found via optical imaging and spectroscopy out of 22 Hi clouds identified in the GALFAHI survey as dwarf galaxy candidates. Aims. We derive the Hi content and kinematics of Pisces A and B. Methods. Our aperture synthesis Hi observations used the seven-dish Karoo Array Telescope (KAT-7), which is a pathfinder instru- ment for MeerKAT, the South African precursor to the mid-frequency Square Kilometre Array (SKA-MID). Results. The low rotation velocities of ∼5 km s−1 and ∼10 km s−1 in Pisces A and B, respectively, and their Hi content show that they are really dwarf irregular galaxies (dIrr). -
First Results from the Event Horizon Telescope
First results from the Event Horizon Telescope Dom Pesce On behalf of the Event Horizon Telescope collaboration March 10, 2020 EDSU conference The goal (ca. 2017) The goal is to take a picture of a black hole The goal (ca. 2017) Subrahmanyan Chandrasekhar The goal is to take a picture of a black hole • General relativity makes a prediction for the apparent shape of a black hole “It is conceptually interesting, if not astrophysically very important, to calculate the precise apparent shape of the black hole… Unfortunately, there seems to be no hope of observing this effect.” - James Bardeen, 1973 James Bardeen Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend event horizon b photon orbit Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend The closer these trajectories get to a critical impact parameter, the more tightly wound they become Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend The closer these trajectories get to a critical impact parameter, the more tightly wound they become Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend The closer these trajectories get to a critical impact parameter, the more tightly wound they become The trajectories interior to this critical impact parameter intersect the horizon, and these collectively form the black hole “shadow” (Falcke, Melia, & Agol 2000) while the bright surrounding region constitutes the “photon ring” Adapted from: Asada et al. -
Appendix 1 897 Discoverers in Alphabetical Order
Appendix 1 897 Discoverers in Alphabetical Order Abe, H. 22 (7) 1993-1999 Bohrmann, A. 9 1936-1938 Abraham, M. 3 (3) 1999 Bonomi, R. 1 (1) 1995 Aikman, G. C. L. 3 1994-1997 B¨orngen, F. 437 (161) 1961-1995 Akiyama, M. 14 (10) 1989-1999 Borrelly, A. 19 1866-1894 Albitskij, V. A. 10 1923-1925 Bourgeois, P. 1 1929 Aldering, G. 3 1982 Bowell, E. 563 (6) 1977-1994 Alikoski, H. 13 1938-1953 Boyer, L. 40 1930-1952 Alu, J. 20 (11) 1987-1993 Brady, J. L. 1 1952 Amburgey, L. L. 1 1997 Brady, N. 1 2000 Andrews, A. D. 1 1965 Brady, S. 1 1999 Antal, M. 17 1971-1988 Brandeker, A. 1 2000 Antonini, P. 25 (1) 1996-1999 Brcic, V. 2 (2) 1995 Aoki, M. 1 1996 Broughton, J. 179 1997-2002 Arai, M. 43 (43) 1988-1991 Brown, J. A. 1 (1) 1990 Arend, S. 51 1929-1961 Brown, M. E. 1 (1) 2002 Armstrong, C. 1 (1) 1997 Broˇzek, L. 23 1979-1982 Armstrong, M. 2 (1) 1997-1998 Bruton, J. 1 1997 Asami, A. 5 1997-1999 Bruton, W. D. 2 (2) 1999-2000 Asher, D. J. 9 1994-1995 Bruwer, J. A. 4 1953-1970 Augustesen, K. 26 (26) 1982-1987 Buchar, E. 1 1925 Buie, M. W. 13 (1) 1997-2001 Baade, W. 10 1920-1949 Buil, C. 4 1997 Babiakov´a, U. 4 (4) 1998-2000 Burleigh, M. R. 1 (1) 1998 Bailey, S. I. 1 1902 Burnasheva, B. A. 13 1969-1971 Balam, D.