The Physics and Chemistry of Nebular Evolution 209
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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. -
Chemical Equilibrium Chemistry (H) 1St Year SEM-II, Dated: 7Th April 2020
Remarks of Assignment 2: Chemical Equilibrium Chemistry (H) 1st Year SEM-II, Dated: 7th April 2020 Grades: A (Excellent); B+ (Very good); B (Good) and C (Poor) S. NAME Roll No. Grade Remarks No. 1. Sejal Jain 1931210 Resubmission: Not submitted or misplaced 2. Harshita 1931206 A In Q.6. no need to discuss the situations, according to figure 1 it is NO and Q.8. Try to write concisely 3. Yogesh Kumar 1931152 B+ Q. 6. Not correct 4. Pooja 1931132 B+ Q. 6. Not correct 5. Riddhima 120 A Excellent 6. Jyoti 112 B+ Q. 6. Not correct 7. Vivek 146 B+ Q. 6. Not correct 8. Vikash 154 B+ Q. 6. Not correct 9. Nidhi 150 A Excellent 10. Mehak Vaish 136 B+ Q. 6. Not correct 11. Rinka* 122 B+ Q. 6. Not correct 12. Sheenu 202 A Excellent 13. Bhupendra 104 B+ Q. 6. Not correct Maurya 14. Deepanshu 142 B+ Q. 6. Not correct 15. Diksha Rathi 204 A Excellent 16. Khushboo Mittal 256 A Q. 6. Not correct 17. Amit Patwa 252 B+ Q. 6. Not correct 18. Aman Tomar 246 A Excellent 19. Vinay Sharma 176 B+ Q. 6. Not correct 20. Garima Nveen 128 B+ Q. 6. Not correct and Q. 8. Answer in terms of number of moles, 21. Yatin Kumar 254 B+ Q. 6. Not correct 22. Ajay Kumar 238 B+ Q. 6. Not correct 23. Divya Yadav 214 A Excellent, Kindly check Q.6. not properly scanned but I think you want to say NO 24. Kushagra Malik 174 B+ Q. -
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 Co2 Chemistry in Sea Water
INTRODUCTION TO CO2 CHEMISTRY IN SEA WATER Andrew G. Dickson Scripps Institution of Oceanography, UC San Diego Mauna Loa Observatory, Hawaii Monthly Average Carbon Dioxide Concentration Data from Scripps CO Program Last updated August 2016 2 ? 410 400 390 380 370 2008; ~385 ppm 360 350 Concentration (ppm) 2 340 CO 330 1974; ~330 ppm 320 310 1960 1965 1970 1975 1980 1985 1990 1995 2000 2005 2010 2015 Year EFFECT OF ADDING CO2 TO SEA WATER 2− − CO2 + CO3 +H2O ! 2HCO3 O C O CO2 1. Dissolves in the ocean increase in decreases increases dissolved CO2 carbonate bicarbonate − HCO3 H O O also hydrogen ion concentration increases C H H 2. Reacts with water O O + H2O to form bicarbonate ion i.e., pH = –lg [H ] decreases H+ and hydrogen ion − HCO3 and saturation state of calcium carbonate decreases H+ 2− O O CO + 2− 3 3. Nearly all of that hydrogen [Ca ][CO ] C C H saturation Ω = 3 O O ion reacts with carbonate O O state K ion to form more bicarbonate sp (a measure of how “easy” it is to form a shell) M u l t i p l e o b s e r v e d indicators of a changing global carbon cycle: (a) atmospheric concentrations of carbon dioxide (CO2) from Mauna Loa (19°32´N, 155°34´W – red) and South Pole (89°59´S, 24°48´W – black) since 1958; (b) partial pressure of dissolved CO2 at the ocean surface (blue curves) and in situ pH (green curves), a measure of the acidity of ocean water. -
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. -
3-D Surface Visualization of Ph Titration “Topos”: Equivalence Point Cliffs, Dilution Ramps and Buffer Plateaus
University of Montana ScholarWorks at University of Montana Water Topos: A 3-D Trend Surface Approach to Viewing and Teaching Aqueous Equilibrium Open Educational Resources (OER) Chemistry 11-2020 Chapter 1.1: 3-D Surface Visualization of pH Titration “Topos”: Equivalence Point Cliffs, Dilution Ramps and Buffer Plateaus Garon C. Smith University of Montana, Missoula Md Mainul Hossain North South University, Bangladesh Patrick MacCarthy Colorado School of Mines Follow this and additional works at: https://scholarworks.umt.edu/topos Part of the Chemistry Commons Let us know how access to this document benefits ou.y Recommended Citation Smith, Garon C.; Hossain, Md Mainul; and MacCarthy, Patrick, "Chapter 1.1: 3-D Surface Visualization of pH Titration “Topos”: Equivalence Point Cliffs, Dilution Ramps and Buffer Plateaus" (2020). Water Topos: A 3-D Trend Surface Approach to Viewing and Teaching Aqueous Equilibrium Chemistry. 2. https://scholarworks.umt.edu/topos/2 This Book is brought to you for free and open access by the Open Educational Resources (OER) at ScholarWorks at University of Montana. It has been accepted for inclusion in Water Topos: A 3-D Trend Surface Approach to Viewing and Teaching Aqueous Equilibrium Chemistry by an authorized administrator of ScholarWorks at University of Montana. For more information, please contact [email protected]. Part 1: Acid-Base Equilibrium Chapter 1.1 3-D Surface Visualization of pH Titration “Topos”: Equivalence Point Cliffs, Dilution Ramps and Buffer Plateaus Garon C. Smith1, Md Mainul Hossain2 and Patrick MacCarthy3 1Department of Chemistry and Biochemistry, The University of Montana, Missoula, MT 59812, Department of Biochemistry and Microbiology, North South University, Dhaka, Bangladesh, and 2Department of Chemistry and Geochemistry, Colorado School of Mines, Golden, CO 80401 Abstract 3-D topographic surfaces (“topos”) can be generated to visualize how pH behaves during titration and dilution procedures. -
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. -
Kuchner, M. & Seager, S., Extrasolar Carbon Planets, Arxiv:Astro-Ph
Extrasolar Carbon Planets Marc J. Kuchner1 Princeton University Department of Astrophysical Sciences Peyton Hall, Princeton, NJ 08544 S. Seager Carnegie Institution of Washington, 5241 Broad Branch Rd. NW, Washington DC 20015 [email protected] ABSTRACT We suggest that some extrasolar planets . 60 ML will form substantially from silicon carbide and other carbon compounds. Pulsar planets and low-mass white dwarf planets are especially good candidate members of this new class of planets, but these objects could also conceivably form around stars like the Sun. This planet-formation pathway requires only a factor of two local enhancement of the protoplanetary disk’s C/O ratio above solar, a condition that pileups of carbonaceous grains may create in ordinary protoplanetary disks. Hot, Neptune- mass carbon planets should show a significant paucity of water vapor in their spectra compared to hot planets with solar abundances. Cooler, less massive carbon planets may show hydrocarbon-rich spectra and tar-covered surfaces. The high sublimation temperatures of diamond, SiC, and other carbon compounds could protect these planets from carbon depletion at high temperatures. arXiv:astro-ph/0504214v2 2 May 2005 Subject headings: astrobiology — planets and satellites, individual (Mercury, Jupiter) — planetary systems: formation — pulsars, individual (PSR 1257+12) — white dwarfs 1. INTRODUCTION The recent discoveries of Neptune-mass extrasolar planets by the radial velocity method (Santos et al. 2004; McArthur et al. 2004; Butler et al. 2004) and the rapid development 1Hubble Fellow –2– of new technologies to study the compositions of low-mass extrasolar planets (see, e.g., the review by Kuchner & Spergel 2003) have compelled several authors to consider planets with chemistries unlike those found in the solar system (Stevenson 2004) such as water planets (Kuchner 2003; Leger et al. -
Atmospheric Chemistry
Atmospheric Chemistry John Lee Grenfell Technische Universität Berlin Atmospheres and Habitability (Earthlike) Atmospheres: -support complex life (respiration) -stabilise temperature -maintain liquid water -we can measure their spectra hence life-signs Modern Atmospheric Composition CO2 Modern Atmospheric Composition O2 CO2 N2 CO2 N2 CO2 Modern Atmospheric Composition O2 CO2 N2 CO2 N2 P 93bar 1bar 6mb 1.5bar surface CO2 Tsurface 735K 288K 220K 94K Early Earth Atmospheric Compositions Magma Hadean Archaean Proterozoic Snowball CO2 Early Earth Atmospheric Compositions Magma Hadean Archaean Proterozoic Snowball Silicate CO2 CO2 N2 N2 Steam H2ON2 O2 O2 CO2 Additional terrestrial-type atmospheres Jurassic Earth Early Mars Early Venus Jungleworld Desertworld Waterworld Superearth Modern Atmospheric Composition Today we will talk about these CO2 Reading List Yuk Yung (Caltech) and William DeMore “Photochemistry of Planetary Atmospheres” Richard P. Wayne (Oxford) “Chemistry of Atmospheres” T. Gredel and Paul Crutzen (Mainz) “Chemie der Atmosphäre” Processes influencing Photochemistry Photons Protection Delivery Escape Clouds Photochemistry Surface OCEAN Biology Volcanism Some fundamentals… ALKALI METALS The Periodic Table NOBLE GASES One outer electron Increasing atomic number 8 outer electrons: reactive Rows called PERIODS unreactive GROUPS: similar Halogens chemical C, Si etc. have 4 outer electrons properties SO CAN FORM STABLE CHAINS Chemical Structure and Reactivity s and p orbitals d orbitals The Aufbau Method works OK for the first 18 elements -
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 .