Effect of Radiative Levitation on Calculations of Accretion Rates in White Dwarfs Pierre Chayer 1 and Jean Dupuis 2 1 STScI, 2 CSA 17 th European White.

Slides:



Advertisements
Similar presentations
Putting A Stars into Context: Evolution, Environment, and Related Stars, June 3-7, 2013, Moscow M.V. Lomonosov State University, Moscow, RUSSIA Abundance.
Advertisements

Fick’s Laws Combining the continuity equation with the first law, we obtain Fick’s second law:
% eff = (Wout / W in) *100 eff = (80 J / 100 J) * 100 = 80% W in = 75 N * 5 m = 375 J W out = 100 N * 3 m = 300 J eff = (300 J / 375 J) *100 = 80% W in.
Stellar Atmospheres: Hydrostatic Equilibrium 1 Hydrostatic Equilibrium Particle conservation.
White Dwarfs in the HET Dark Energy Experiment Bárbara G. Castanheira The University of Texas at Austin Universität Wien 17 th European White Dwarf Workshop.
Review for Quiz 2. Outline of Part 2 Properties of Stars  Distances, luminosities, spectral types, temperatures, sizes  Binary stars, methods of estimating.
Sylvie Vauclair Institut de Recherches en Astrophysique et Planétologie, OMP, CNRS, Université de Toulouse, Institut universitaire de France Séminaire.
Oct 17, Non-Equilibrium Ionization Orly Gnat (Caltech) with Amiel Sternberg (Tel-Aviv University) Gnat & Sternberg 2007, ApJS, 168, 213 in Post-Shock.
OPserver: opacities and radiative accelerations on demand C Mendoza (IVIC, Ven) LS Rodríguez (IVIC, Ven) MJ Seaton (UCL, UK) F Delahaye (OPM, France) P.
Average Atomic Mass Practice
João Pedro Marques Mário João Monteiro CESAM2K CoRoT/ESTA - Aarhus Workshop.
Post-AGB evolution. Learning outcome evolution from the tip of the AGB to the WD stage object types along the post-AGB evolution basics about planetary.
The Effects of Mass Loss on the Evolution of Chemical Abundances in Fm Stars Mathieu Vick 1,2 Georges Michaud 1 (1)Département de physique, Université.
Iron K Spectra from L-Shell Ions in Photoionized Plasmas Work in Progress Duane Liedahl Physics and Advanced Technologies Lawrence Livermore National Laboratory.
Dusty old star offers window to our future --- GD 362 Department of Physics National Tsing Hua University G.T. Chen 2005/10/20.
Institute for Astronomy and Astrophysics, University of Tübingen, Germany July 5, 2004Cool Stars, Stellar Systems and the Sun (Hamburg, Germany)1 Turning.
New Objective 6.5B Recognize that a limited number of elements make up the largest portion of solid Earth, living matter, oceans and the atmosphere.
Catalyst 1. Write down Dalton’s postulate that was proven wrong by the existence of isotopes. 2. How does the existence of isotopes disprove this component.
computer
Survey of the Universe Tom Burbine
Cataclysmic Variables in the UV D.de Martino INAF-Osservatorio Astronomico di Capodimonte Napoli & B.T. Gaensicke (Warwick), K.Long (STScI), T.R.Marsh.
Class Goals Familiarity with basic terms and definitions Physical insight for conditions, parameters, phenomena in stellar atmospheres Appreciation of.
The White Dwarf in SS Cygni: FUSE + HST Spectral Analysis Edward M. Sion, Patrick Godon, Janine Myszka Edward M. Sion, Patrick Godon, Janine Myszka Department.
Surface abundances of Am stars as a constraint on rotational mixing Olivier Richard 1,2, Suzanne Talon 2, Georges Michaud 2 1 GRAAL UMR5024, Université.
A Spectroscopic Survey of Bright DA(…) White Dwarfs Alexandros Gianninas, Pierre Bergeron Université de Montréal Jean Dupuis Canadian Space Agency Maria.
The theoretical understanding of Type Ia Supernovae Daniel Kasen.
New Model Atmospheres for Hydrogen-Deficient Stars May 3 rd, 2006 Natalie Behara Armagh Observatory.
A short review The basic equation of transfer for radiation passing through gas: the change in specific intensity I is equal to: -dI /d  = I - j /  =
Calculating the Average Atomic Mass. Steps for Calculating Average Atomic Mass (When given percentages of each isotope and each isotopes mass) 1. Convert.
Bisector analysis of RR Lyrae atmosphere dynamics at different pulsation and Blazhko phases Elisabeth Guggenberger – IAU Symposium 301, August 2013 Work.
Atomic Mass The Mole Atomic Weight Formula Weight Molarity of a Solution.
Institute for Astronomy and Astrophysics, University of Tübingen 16 Aug th European White Dwarf Workshop Tübingen, Germany 1 HST / COS Spectroscopy.
On the Stark broadening of Cr II spectral lines in atmospheres of DB white dwarfs Z. Simić 1, M. S. Dimitrijević 1,2, A. Kovačević 3, S. Sahal-Bréchot.
The Empirical Mass Distribution of Hot B Subdwarfs derived by asteroseismology and other means Valerie Van Grootel (1) G. Fontaine (2), P. Brassard (2),
Warm Absorbers: Are They Disk Outflows? Daniel Proga UNLV.
Investigations of the accretion disk structure in SS Cyg using the Doppler tomography technique D.A.Kononov Institute of Astronomy of the RAS Russia, Moscow.
The Stratification of Metals in Hot White Dwarf Atmospheres N.J. Dickinson, M.A. Barstow, I. Hubeny * * Steward Observatory, University of.
Warm-Up 1) Use log 3 5 = and log 3 6 = to approximate log ) Condense 7 log log 4 x + 3 log 4 y.
Fluorine in RCB and EHe Stars. ► RCB stars comprise a sequence of H-deficient supergiants with effective temperatures from about 3500 K, as represented.
Isotopic Abundance Pages Thinking question Why are there decimal places for atomic masses on the periodic table if protons and neutrons have amu.
ATOMIC DATA AND STARK BROADENING OF Nb III Zoran Simić Milan S. Dimitrijević Luka Č. Popović Astronomical Observatory Belgrade, 11060, Serbia.
Black Bodies Wien’s Law – Peak intensity Stefan-Boltzman Law – Luminosity Planck’s Law – Energy Distribution –Rayleigh-Jeans approximation –Wien approximation.
STELLAR EVOLUTION – THE STANDARD SOLAR MODEL AND SOLAR NEUTRINOS – MARIE ZECH.
Luminosity and Spectra of Young Jupiters Jonathan J. Fortney University of California, Santa Cruz Mark Marley (NASA Ames) Olenka Hubickyj (NASA Ames) Peter.
Average Atomic Mass Practice
The Future of White Dwarf Asteroseismology Travis Metcalfe (NCAR) NGC 1514 – Crystal Ball Nebula.
Exploring the diffusion induced nova scenario Marcelo Miguel Miller Bertolami Leandro Gabriel Althaus (FCAGLP-UNLP/IALP CONICET, Argentina) Exploring the.
Michael Langer Heinrich Bülthoff NEC Research Institute MPI for Biological Cybernetics Princeton, NJ Tübingen, Germany Shape from Shading under diffuse.
STARK BROADENING IN ASTROPHYSICS
The Transfer Equation The basic equation of transfer for radiation passing through gas: the change in specific intensity In is equal to: dIl = intensity.
Milan S. Dimitrijević and Nenad Milovanović
Exploring the diffusion induced nova scenario
The Elements – Part 2 Getting Specific.
Stellar Evolution Pressure vs. Gravity.
Mariko KATO (Keio Univ., Japan) collaboration with
Irregularities Of Mass In The Periodic Table
Starter - Calculate the P,N + E
Isotopes 436 Objectives: 5.2 Identify the advantages and disadvantages of using isotopes in industry, medical science, basic research, and in the environment.
Isotopes and RAM Learning Outcomes:
Dimensional Analysis If snow falls at 1.5 in/hour how many mm/minute is that? (1in=2.54 cm)
EXAMPLE 4 Check data for inverse variation
Bohr Model Lewis Structures
LECTURE 10.3 – ISOTOPES.
Silicon - Si - #14.
Unit 3 Review (Calculator)
Properties of Atoms and the Periodic Table
ON THE STARK BROADENING OF Si III SPECTRAL LINES IN STELLAR PLASMA
DA型脉动白矮星氢大气厚度主导脉动周期间隔弥散
Igneous Rocks Chapter 5.
Calculate 9 x 81 = x 3 3 x 3 x 3 x 3 3 x 3 x 3 x 3 x 3 x 3 x =
Presentation transcript:

Effect of Radiative Levitation on Calculations of Accretion Rates in White Dwarfs Pierre Chayer 1 and Jean Dupuis 2 1 STScI, 2 CSA 17 th European White Dwarf Workshop Tübingen, Germany August 16−20, 2010 Gemini Observatory Illustration by Jon Lomberg

Two methods exist for computing accretion rates 2 1)Steady state approximation 2)Time-dependent diffusion calculations

Silicon and aluminum are supported 3 Radiative acceleration as a function of depth T eff = 20,000 K, log g = 8.0

Silicon is supported in DA with T eff < 17,500 K 4 Radiative acceleration as a function of depth for Si Log g = 8.0

Evolution of Si in a DA in presence of accretion but without radiative levitation 5 Log [dM/dt] Si = 10 2 g/s, T eff = 20,000 K, log g = 8.0

Evolution of Si in a DA in presence of accretion and radiative levitation 6 Log [dM/dt] si = 10 2 g/s, T eff = 20,000 K, log g = 8.0

Evolution of Si in a DA in presence of accretion and radiative levitation 7 Log [dM/dt] si = 10 6 g/s, T eff = 20,000 K, log g = 8.0

The radiative levitation has an impact on the determination of accretion rates 8 Silicon abundance as a function of depth Teff = 20,000 K Log g = 8.0

In summary, the abundance of elements supported by the radiative levitation may not be related to the accretion rate 9 25,000 K 20,000 K 17,500 K 22,500 K Log g = 8.0