On the origin of Microturbulence in hot stars

Slides:



Advertisements
Similar presentations
Disk Structure and Evolution (the so-called model of disk viscosity) Ge/Ay 133.
Advertisements

Proto-Planetary Disk and Planetary Formation
Magnetars in Supernova Remnants & Magnetar Formation Jacco Vink Isolated NSs, London, April, 2006 Magnetars in Supernova Remnants & Magnetar Formation.
Estimate of physical parameters of molecular clouds Observables: T MB (or F ν ), ν, Ω S Unknowns: V, T K, N X, M H 2, n H 2 –V velocity field –T K kinetic.
September 2005 Magnetic field excitation in galaxies.
Turbulent Convection in Stars Kwing Lam Chan Hong Kong University of Science and Technology “A Birthday Celebration of the Contribution of Bernard Jones.
August 22, 2006IAU Symposium 239 Observing Convection in Stellar Atmospheres John Landstreet London, Canada.
Angular momentum evolution of low-mass stars The critical role of the magnetic field Jérôme Bouvier.
The evolution and collapse of BH forming stars Chris Fryer (LANL/UA)  Formation scenarios – If we form them, they will form BHs.  Stellar evolution:
T Tauri Stars: An Overview Colette Salyk Ge132. What is a T Tauri star? 1st Answer: Observational –Hydrogen Balmer and Ca II H and K emission –Often emission.
A Multiphase, Sticky Particle, Star Formation Recipe for Cosmology
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.
CDM cusps in LSB galaxies by means of stellar kinematics A.Pizzella, E.M.Corsini, F. Bertola Università di Padova And J. Magorrian, M. Sarzi University.
Analysis of Doppler-Broadened X-ray Emission Line Profiles from Hot Stars David Cohen - Swarthmore College with Roban Kramer - Swarthmore College Stanley.
Marc Pinsonneault (OSU).  New Era in Astronomy  Seismology  Large Surveys  We can now measure things which have been assumed in stellar modeling 
Interacting Winds: Theory Overview Stan Owocki Bartol Research Institute University of Delaware with thanks for web slides from: D. Folini, K. Gayley,
Stellar Winds and Mass Loss Brian Baptista. Summary Observations of mass loss Mass loss parameters for different types of stars Winds colliding with the.
Spring School of Spectroscopic Data Analyses 8-12 April 2013 Astronomical Institute of the University of Wroclaw Wroclaw, Poland.
Resonance scattering in the X-ray emission line profiles of  Pup Maurice Leutenegger With David Cohen, Steve Kahn, Stan Owocki, and Frits Paerels.
ROTATING MASSIVE STARS as Long Gamma-Ray Burst progenitors Matteo Cantiello - Sterrekundig Instituut Utrecht as Long Gamma-Ray Burst progenitors Matteo.
Qingkang Li Department of Astronomy Beijing Normal University The Third Workshop of SONG, April, 2010 Disks of Be Stars & Their Pulsations &
A few Challenges in massive star evolution ROTATIONMAGNETIC FIELD MULTIPLICITY How do these distributions vary with metallicity? How do these distributions.
From an evolutionary point of view Selma de Mink Utrecht University Lorentz Center Workshop “Stellar Mergers” Ines Brott (Utrecht), Matteo Cantiello (Utrecht),
1 Observations of Convection in A-type Stars Barry Smalley Keele University Staffordshire United Kingdom.
Linear spectropolarimetry Jorick Vink (Armagh Observatory)
Rotational Line Broadening Gray Chapter 18 Geometry and Doppler Shift Profile as a Convolution Rotational Broadening Function Observed Stellar Rotation.
The Physical Properties of Red Supergiants Emily Levesque IfA, University of Hawaii/SAO, Harvard Hot Massive Stars: A Lifetime of Influence Lowell Observatory.
PHYSICS UNDER THE BONNET OF A STELLAR EVOLUTION CODE Richard J. Stancliffe Argelander Institut für Astronomie, Universität Bonn.
First Attempt of Modelling of the COROT Main Target HD Workshop: "gamma Doradus stars in the COROT fields" /05/ Nice Mehdi – Pierre.
Why do globular clusters have more than one main sequence? Ref: Gratton et al. 2012, A&ARv, 20, 50.
L 3 - Stellar Evolution I: November-December, L 3: Collapse phase – theoretical models Background image: courtesy ESO - B68 with.
Padova, October Padova, October 1980 Padova, October 1980.
Julie Hollek and Chris Lindner.  Background on HK II  Stellar Analysis in Reality  Methodology  Results  Future Work Overview.
Rotation Among High Mass Stars: A Link to the Star Formation Process? S. Wolff and S. Strom National Optical Astronomy Observatory.
Magneto-hydrodynamic Simulations of Collapsars Shin-ichiro Fujimoto (Kumamoto National College of Technology), Collaborators: Kei Kotake(NAOJ), Sho-ichi.
联 合 天 体 物 理 中 心 Joint Center for Astrophysics The half-light radius distribution of LBGs and their stellar mass function Chenggang Shu Joint Center for.
AGN Outflows: Part II Outflow Generation Mechanisms: Models and Observations Leah Simon May 4, 2006.
FIRST LIGHT A selection of future facilities relevant to the formation and evolution of galaxies Wavelength Sensitivity Spatial resolution.
Resolved X-ray Line Profiles from O Stars as a Diagnostic of Wind Mass Loss David Cohen Department of Physics & Astronomy Swarthmore College Jon Sundqvist.
Hunting Very Massive Metal-poor Stars Danny Lennon (ESA-STScI) Acknowledgements: Miriam Garcia (IAC), Artemio Herrero (IAC), Alex Fullerton (STScI), Joachim.
Massive Star Evolution: Plain and Fancy J. Craig Wheeler Department of Astronomy. University of Texas at Austin MESA Summer School, August 11, 2015.
Star Formation Triggered By First Supernovae Fumitaka Nakamura (Niigata Univ.)
Matteo Cantiello Astronomical Institute Utrecht Binary star progenitors of long GRBs M. Cantiello, S.-C. Yoon, N. Langer, and M. Livio A&A 465, L29-L33.
Convective Core Overshoot Lars Bildsten (Lecturer) & Jared Brooks (TA) Convective overshoot is a phenomenon of convection carrying material beyond an unstable.
The formation of the Local Group
Modern cosmology 1: The Hubble Constant
Single versus Binary Star Progenitors of Type IIb Supernovae
Numerical Simulations of Solar Magneto-Convection
Angular momentum transport and mixing in rotating stars
RR Lyrae variable stars
The effect of magnetic fields on the survival of high-velocity clouds
Long GRB rate in the binary merger model
October 14, Wednesday 12. Solar Convection
CO mass-loss rate of red-supergiants at low metallicity
Progenitors of long GRBs
Joleen Carlberg July 12, 2017 Abstract:
The Evolution of Supermassive Pop III stars
Pre-Main-Sequence of A stars
Spectrally-polarized features of ε Aurigae: In and out of eclipse
Atmospheres of Cool Stars
Outflows from Clusters of Massive Stars
Evolution of the circumstellar medium around massive stars
Single Vs binary star progenitors of Type Iib Sne
西华师范大学 China West Normal University
A Search for Quiet Massive X-Ray Binaries
Midwest Workshop on SUPernovae and TRansients Niharika Sravan
Pair Instability Supernovae
Convection John Crooke 3/26/2019.
Rotational Line Broadening Gray Chapter 18
Presentation transcript:

On the origin of Microturbulence in hot stars Matteo Cantiello Utrecht University (N.Langer, A.de Koter, J.Vink, A.Voegler, S.N.Shore, I.Brott, S.C.Yoon)

Outline of the talk Convection in hot stars Microturbulence in hot stars Implications for wind clumping Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Convection in hot stars Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Stellar structure Low Mass stars Massive stars e.g 1MSun e.g 20 MSun Radiative core Convective envelope Convective core Radiative envelope Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Opacity Inside a massive star Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Subsurface convection (e.g. Cantiello et al. ’08, Maeder et al. ‘08) Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Microturbulence in hot stars Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Microturbulence Is the additional broadening coming from nonthermal motions varying on a small scale in the region of line formation. Observed line profile Intrinsic line profile Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Microturbulence vs Macroturbulence L = Size of line forming region D= Scale on which non-thermal velocity varies D L D D < L Microturbulence D > L Macroturbulence non radial pulsation, granules motion... ? See next talk Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Origin of microturbulence? To fit stellar spectra of hot stars microturbulence (~0-20 km/s) is needed Used as a free parameter. Unknown physical origin We look for a correlation between subsurface convection and microturbulence Convection microturbulence clumping ? Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

The physical mechanism (e.g. Lighthill ‘52, Stein ‘67, Edmunds ’78, de Jager et al. ’91) Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Method We use a 1D-hydrodynamic stellar evolution code (Langer et al., Heger et al.) Convection: Ledoux criterion and Mixing length theory (Bohm-Vitense ‘58) Opacity: OPAL ‘96 (Rogers & Iglesias ‘96) Grids of models from 5 to 120 MSun at MW, LMC and SMC metallicities Observations of microturbulence in hot stars (ESO Flames, Hunter et al. 2007, Trundle et al. 2007) Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Results Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Results (LMC) Models + FLAMES observations of microturbulence Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Results II (Metallicity) Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Wind clumping Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Wind clumping Evidences that winds of massive stars are clumped (e.g. Puls at al. ‘06) Inner wind seems to be more clumped (Puls at al. ‘06) Line-driven instability prediction not confirmed (Runacres & Owocki ’02,’05) Correlation between clumping at the base of the wind and subsurface convection (hence microturbulence)? Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Inner wind clumping in ~ 1.05...2 R* (Data from Puls et al. ’06) Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Summary Most hot stars have subsurface convection Convection increases with Z , T, L Subsurface convection correlates with microturbulent velocities Similar prediction for wind clumping Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

The future ? Microturbulence, once a fudge factor, could become a physical phenomenon which plays an important role in the evolution of massive stars! Need for hydro simulations of the atmosphere of hot stars. Magnetic fields: dynamo from subsurface convection? Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

The End Thanks! Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Rotation and Microturbulence Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Small magellanic cloud Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008

Milky Way Matteo Cantiello On the origin of Microturbulence in hot stars Liège - July 2008