1 from Molecular Clouds to the Origin of Life
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Exploring Pulsars
High-energy astrophysics Explore the PUL SAR menagerie Astronomers are discovering many strange properties of compact stellar objects called pulsars. Here’s how they fit together. by Victoria M. Kaspi f you browse through an astronomy book published 25 years ago, you’d likely assume that astronomers understood extremely dense objects called neutron stars fairly well. The spectacular Crab Nebula’s central body has been a “poster child” for these objects for years. This specific neutron star is a pulsar that I rotates roughly 30 times per second, emitting regular appar- ent pulsations in Earth’s direction through a sort of “light- house” effect as the star rotates. While these textbook descriptions aren’t incorrect, research over roughly the past decade has shown that the picture they portray is fundamentally incomplete. Astrono- mers know that the simple scenario where neutron stars are all born “Crab-like” is not true. Experts in the field could not have imagined the variety of neutron stars they’ve recently observed. We’ve found that bizarre objects repre- sent a significant fraction of the neutron star population. With names like magnetars, anomalous X-ray pulsars, soft gamma repeaters, rotating radio transients, and compact Long the pulsar poster child, central objects, these bodies bear properties radically differ- the Crab Nebula’s central object is a fast-spinning neutron star ent from those of the Crab pulsar. Just how large a fraction that emits jets of radiation at its they represent is still hotly debated, but it’s at least 10 per- magnetic axis. Astronomers cent and maybe even the majority. -
Planetary Nebulae Jacob Arnold AY230, Fall 2008
Jacob Arnold Planetary Nebulae Jacob Arnold AY230, Fall 2008 1 PNe Formation Low mass stars (less than 8 M) will travel through the asymptotic giant branch (AGB) of the familiar HR-diagram. During this stage of evolution, energy generation is primarily relegated to a shell of helium just outside of the carbon-oxygen core. This thin shell of fusing He cannot expand against the outer layer of the star, and rapidly heats up while also quickly exhausting its reserves and transferring its head outwards. When the He is depleted, Hydrogen burning begins in a shell just a little farther out. Over time, helium builds up again, and very abruptly begins burning, leading to a shell-helium-flash (thermal pulse). During the thermal-pulse AGB phase, this process repeats itself, leading to mass loss at the extended outer envelope of the star. The pulsations extend the outer layers of the star, causing the temperature to drop below the condensation temperature for grain formation (Zijlstra 2006). Grains are driven off the star by radiation pressure, bringing gas with them through collisions. The mass loss from pulsating AGB stars is oftentimes referred to as a wind. For AGB stars, the surface gravity of the star is quite low, and wind speeds of ~10 km/s are more than sufficient to drive off mass. At some point, a super wind develops that removes the envelope entirely, a phenomenon not yet fully understood (Bernard-Salas 2003). The central, primarily carbon-oxygen core is thus exposed. These cores can have temperatures in the hundreds of thousands of Kelvin, leading to a very strong ionizing source. -
Introduction to Astronomy from Darkness to Blazing Glory
Introduction to Astronomy From Darkness to Blazing Glory Published by JAS Educational Publications Copyright Pending 2010 JAS Educational Publications All rights reserved. Including the right of reproduction in whole or in part in any form. Second Edition Author: Jeffrey Wright Scott Photographs and Diagrams: Credit NASA, Jet Propulsion Laboratory, USGS, NOAA, Aames Research Center JAS Educational Publications 2601 Oakdale Road, H2 P.O. Box 197 Modesto California 95355 1-888-586-6252 Website: http://.Introastro.com Printing by Minuteman Press, Berkley, California ISBN 978-0-9827200-0-4 1 Introduction to Astronomy From Darkness to Blazing Glory The moon Titan is in the forefront with the moon Tethys behind it. These are two of many of Saturn’s moons Credit: Cassini Imaging Team, ISS, JPL, ESA, NASA 2 Introduction to Astronomy Contents in Brief Chapter 1: Astronomy Basics: Pages 1 – 6 Workbook Pages 1 - 2 Chapter 2: Time: Pages 7 - 10 Workbook Pages 3 - 4 Chapter 3: Solar System Overview: Pages 11 - 14 Workbook Pages 5 - 8 Chapter 4: Our Sun: Pages 15 - 20 Workbook Pages 9 - 16 Chapter 5: The Terrestrial Planets: Page 21 - 39 Workbook Pages 17 - 36 Mercury: Pages 22 - 23 Venus: Pages 24 - 25 Earth: Pages 25 - 34 Mars: Pages 34 - 39 Chapter 6: Outer, Dwarf and Exoplanets Pages: 41-54 Workbook Pages 37 - 48 Jupiter: Pages 41 - 42 Saturn: Pages 42 - 44 Uranus: Pages 44 - 45 Neptune: Pages 45 - 46 Dwarf Planets, Plutoids and Exoplanets: Pages 47 -54 3 Chapter 7: The Moons: Pages: 55 - 66 Workbook Pages 49 - 56 Chapter 8: Rocks and Ice: -
Lecture 3 - Minimum Mass Model of Solar Nebula
Lecture 3 - Minimum mass model of solar nebula o Topics to be covered: o Composition and condensation o Surface density profile o Minimum mass of solar nebula PY4A01 Solar System Science Minimum Mass Solar Nebula (MMSN) o MMSN is not a nebula, but a protoplanetary disc. Protoplanetary disk Nebula o Gives minimum mass of solid material to build the 8 planets. PY4A01 Solar System Science Minimum mass of the solar nebula o Can make approximation of minimum amount of solar nebula material that must have been present to form planets. Know: 1. Current masses, composition, location and radii of the planets. 2. Cosmic elemental abundances. 3. Condensation temperatures of material. o Given % of material that condenses, can calculate minimum mass of original nebula from which the planets formed. • Figure from Page 115 of “Physics & Chemistry of the Solar System” by Lewis o Steps 1-8: metals & rock, steps 9-13: ices PY4A01 Solar System Science Nebula composition o Assume solar/cosmic abundances: Representative Main nebular Fraction of elements Low-T material nebular mass H, He Gas 98.4 % H2, He C, N, O Volatiles (ices) 1.2 % H2O, CH4, NH3 Si, Mg, Fe Refractories 0.3 % (metals, silicates) PY4A01 Solar System Science Minimum mass for terrestrial planets o Mercury:~5.43 g cm-3 => complete condensation of Fe (~0.285% Mnebula). 0.285% Mnebula = 100 % Mmercury => Mnebula = (100/ 0.285) Mmercury = 350 Mmercury o Venus: ~5.24 g cm-3 => condensation from Fe and silicates (~0.37% Mnebula). =>(100% / 0.37% ) Mvenus = 270 Mvenus o Earth/Mars: 0.43% of material condensed at cooler temperatures. -
Impact of Supernovae on Molecular Cloud Evolution Dynamics and Structure
Impact of Supernovae on Molecular Cloud Evolution Dynamics and Structure Bastian K¨ortgen1, Daniel Seifried1, and Robi Banerjee1 1Hamburger Sternwarte, Gojenbergsweg 112, 21029 Hamburg, Germany [email protected] Introduction We perform numerical simulations of colliding streams of the WNM, including magnetic fields and self{gravity, to analyse the formation and evolution of molecular clouds subject to supernova feedback from massive stars. Simulation Setup The Supernova Subgrid Model The equations of MHD together with selfgravity and heating and cooling are evolved in time using the The supernova feedback is included into the model by means of a Sedov blast FLASH code [Fryxell et al., 2000]. We use a constant heating rate Γ and the cooling function Λ according to wave solution. We define a volume of radius R = 1 pc centered on the sink [Koyama and Inutsuka, 2000] and [V´azquez-Semadeni et al., 2007]. The table below lists the initial conditions. particle. Within this volume each grid cell is assigned a certain radial veloc- ity vc. This velocity depends on the kinetic energy input. Additionally we U Sink Particle Parameter Value Parameter Value inject thermal energy, which then gives the total amount of injected energy of E = 1051 erg with 65 % thermal and 35 % kinetic energy according to the Flow Mach number Mf 2.0 Alfv´en velocity va [km/s] 5.8 sn Sedov solution. The cell velocity is Turbulent Mach number Ms 0.5 Alfv´enic Mach number Ma 1.96 r vc = Ush Temperature [K] 5000 Plasma Beta β = Pth=PB 1.93 R Number density n cm−3 1.0 Flow Length [pc] 112 Figure 1: Schematic of the where U is the shock velocity, depending on the kinetic energy input. -
The MUSE View of the Planetary Nebula NGC 3132? Ana Monreal-Ibero1,2 and Jeremy R
A&A 634, A47 (2020) Astronomy https://doi.org/10.1051/0004-6361/201936845 & © ESO 2020 Astrophysics The MUSE view of the planetary nebula NGC 3132? Ana Monreal-Ibero1,2 and Jeremy R. Walsh3,?? 1 Instituto de Astrofísica de Canarias (IAC), 38205 La Laguna, Tenerife, Spain e-mail: [email protected] 2 Universidad de La Laguna, Dpto. Astrofísica, 38206 La Laguna, Tenerife, Spain 3 European Southern Observatory, Karl-Schwarzschild Strasse 2, 85748 Garching, Germany Received 4 October 2019 / Accepted 6 December 2019 ABSTRACT Aims. Two-dimensional spectroscopic data for the whole extent of the NGC 3132 planetary nebula have been obtained. We deliver a reduced data-cube and high-quality maps on a spaxel-by-spaxel basis for the many emission lines falling within the Multi-Unit Spectroscopic Explorer (MUSE) spectral coverage over a range in surface brightness >1000. Physical diagnostics derived from the emission line images, opening up a variety of scientific applications, are discussed. Methods. Data were obtained during MUSE commissioning on the European Southern Observatory (ESO) Very Large Telescope and reduced with the standard ESO pipeline. Emission lines were fitted by Gaussian profiles. The dust extinction, electron densities, and temperatures of the ionised gas and abundances were determined using Python and PyNeb routines. 2 Results. The delivered datacube has a spatial size of 6300 12300, corresponding to 0:26 0:51 pc for the adopted distance, and ∼ × ∼ 1 × a contiguous wavelength coverage of 4750–9300 Å at a spectral sampling of 1.25 Å pix− . The nebula presents a complex reddening structure with high values (c(Hβ) 0:4) at the rim. -
1 the XMM-NEWTON SURVEY of the TAURUS MOLECULAR CLOUD: ACCRETION, JETS, and FLUORESCENCE M. Audard1, Manuel Güdel2, Kevin Brigg
1 THE XMM-NEWTON SURVEY OF THE TAURUS MOLECULAR CLOUD: ACCRETION, JETS, AND FLUORESCENCE M. Audard1, Manuel G¨udel2, Kevin Briggs2, and the XEST Team3 1Columbia Astrophysics Laboratory, 550 West 120th Street, NC 5247, New York, NY 10027, USA 2Paul Scherrer Institut, 5232 Villigen PSI, Switzerland ABSTRACT 1031 The Taurus Molecular Cloud (TMC) is one of the best studied star forming regions. It is close (140 pc) and represents the mode of isolated, non-clustered star for- mation. XMM-Newton has surveyed the richer 5 square degrees of the TMC in X-rays and has obtained high- 30 quality photometric and spectroscopic data of young stars 10 LX and brown dwarfs in their early stages of formation. We present results of the X-ray Emission Survey of TMC (XEST) on the following topics: i) Accretion. The ori- gin of X-rays in young, accreting stars is controversial, as accretion appears to be the dominant emission mech- 1029 anism in some classical T Tauri stars, whereas magnetic activity is the preferred explanation for others. The TMC 10-10 10-9 10-8 10-7 10-6 10-5 Mdot contains several accreting stars whose spectra help us un- derstand the importance of accretion for the production of X-rays. ii) Jets. Young, accreting stars display jets detected in the optical, near-infrared, and radio domains. There is now evidencethat jets are also detected in X-rays in some TMC targets. iii) Fluorescence. The detection of 7.5 an emission feature at 6.4 keV indicates that fluorescence of Fe in a cool environment,e.g., the accretion disk, takes place due to photoionization by hard X-rays or collisions logTav with electron beams. -
The Role of State-Of-The-Art Quantum-Chemical Calculations in Astrochemistry: Formation Route and Spectroscopy of Ethanimine As a Paradigmatic Case
molecules Article The Role of State-of-the-Art Quantum-Chemical Calculations in Astrochemistry: Formation Route and Spectroscopy of Ethanimine as a Paradigmatic Case Carmen Baiano 1 , Jacopo Lupi 1 , Nicola Tasinato 1 , Cristina Puzzarini 2,∗ and Vincenzo Barone 1,∗ 1 Scuola Normale Superiore, Piazza dei Cavalieri 7, 56126 Pisa, Italy; [email protected] (C.B.); [email protected] (J.L.); [email protected] (N.T.); 2 Dipartimento di Chimica “Giacomo Ciamician”, Università di Bologna, Via F. Selmi 2, 40126 Bologna, Italy * Correspondence: [email protected] (C.P.); [email protected] (V.B.) Received: 31 May 2020; Accepted: 18 June 2020; Published: 22 June 2020 Abstract: The gas-phase formation and spectroscopic characteristics of ethanimine have been re-investigated as a paradigmatic case illustrating the accuracy of state-of-the-art quantum-chemical (QC) methodologies in the field of astrochemistry. According to our computations, the reaction between the amidogen, NH, and ethyl, C2H5, radicals is very fast, close to the gas-kinetics limit. Although the main reaction channel under conditions typical of the interstellar medium leads to methanimine and the methyl radical, the predicted amount of the two E,Z stereoisomers of ethanimine is around 10%. State-of-the-art QC and kinetic models lead to a [E-CH3CHNH]/[Z-CH3CHNH] ratio of ca. 1.4, slightly higher than the previous computations, but still far from the value determined from astronomical observations (ca. 3). An accurate computational characterization of the molecular structure, energetics, and spectroscopic properties of the E and Z isomers of ethanimine combined with millimeter-wave measurements up to 300 GHz, allows for predicting the rotational spectrum of both isomers up to 500 GHz, thus opening the way toward new astronomical observations. -
Ghost Supernova Remnants: Evidence for Pulsar Reactivation in Dusty Molecular Clouds?
Notas de Rsica NOTAS DE FÍSICA é uma pré-publicaçáo de trabalhos em Física do CBPF NOTAS DE FÍSICA is a series of preprints from CBPF Pedidos de cópias desta publicaçáfo devem ser enviados aos autores ou à: Requests for free copies of these reports should be addressed to: Divisão de Publicações do CBPF-CNPq Av. Wenceslau Braz, 71 • Fundos 22.290 - Rk> de Janeiro - RJ. Brasil CBPF-NF-034/83 GHOST SUPERNOVA RE WANTS: EVIDENCE FOR PULSAR REACTIVATION IN DUSTY MOLECULAR CLOUDS? by H.Heintzmann1 and M.Novello Centro Brasileiro de Pesquisas Físicas - CBPF/CNPq Rua Xavier Sigaud, 150 22290 - R1o de Janeiro, RJ - Brasil Mnstitut fOr Theoretische Physik der UniversUlt zu K0Tn, 5000 K01n 41, FRG Alemanha GHOST SUPERNOVA REMNANTS: EVIDENCE FOR PULSAR REACTIVATION IN DUSTY MOLECULAR CLOUDS? There is ample albeit ambiguous evidence in favour of a new model for pulsar evolution, according to which pulsars aay only function as regularly pulsed emitters if an accretion disc provides a sufficiently continuous return-current to the radio pulsar (neutron star). On its way through the galaxy the pulsar will consume the disc within some My and travel further (away from the galactic plane) some 100 My without functioning as a pulsar. Back to the galactic plane it may collide with a dense molecular cloud and turn-on for some ten thousand years as a RSntgen source through accretion. The response of the dusty cloud to the collision with the pulsar should resemble a super- nova remnant ("ghost supernova remnant") whereas the pulsar will have been endowed with a new disc, new angular momentum and a new magnetic field . -