Orbital Period Analyses for the CVs Inside the Period Gap

Size: px
Start display at page:

Download "Orbital Period Analyses for the CVs Inside the Period Gap"

Transcription

1 Orbital Period Analyses for the CVs Inside the Period Gap YNAO Dai Zhibin Yunnan Astronomical Observatory, Chinese Academy of Sciences

2 OUTLINE What is the Period Gap? New orbital period distributions of CVs Orbital period analyses Summary

3 Part I. Period Gap

4 What is the Period Gap? Katysheva & Pavlenko (2003)

5 Why is there a gap? " Selection effect for observation (Rappaport et al., 1983) " CV Evolution A. The corresponding gap in white dwarf mass distribution (de Kool, 1992) M wd 0.46M Θ M wd 0. 56M Θ for the CVs below gap for the CVs above gap B. The similar gap has already been shown in the distribution of progenitors of CVs (Vojkhanskaja., 2007) Progenitors of CVs: White dwarf + red dwarf binary system / PCEBs C. Disrupted Magnetic Braking hypothesis (Robinson et al., 1981; McDermott & E. Taam, 1989) Sharp reduction in AML rate when secondary becomes fully convective

6 Standard paradigm of CV evolution A default argument: CVs evolution will shorten its Orbital period Evolution Above Gap Magnetic Wind With radiation core Below Gap Gravitational Radiation Full Convective

7 Part II. Investigation

8 Details of Orbital period distribution The distributions for different subtype of CVs a) Bimodality caused by DN and NL b) The shallower gap in MCV and DN c) No gap in NL and N&RN The pie diagram for the CVs inside below period gap a) MCV DN becomes is a significant a significant subtype subtype inside period below period gap gap b) The Over other 75% subtypes CVs below are gap nearly are DN equal and MCV New N&RN MCV DN NL!

9 A gradual rise branch near 2hr -- is it a result the whole caused gap by gravitational radiation? CVs have spread over The real minimum of gap is near 3hr-- is longer period it a possible evidence for the sudden decline of stellar wind? A small shift towards Smaller interval 10mins for histogram of orbital period distribution

10

11 Part III. Analyses

12 Eclipsing CVs inside gap Subtype MCV DN N & RN Eclipse CVs Orbital Period (hr) *HU Aqr (~15mag) (2.08h)!DD Cir (~20mag) (2.34h) *UZ For (~18mag) (2.11h) *V348 Pup (~15mag) (2.44h)!V597 Pup (>18mag) (2.6687h) *DV Uma (~19mag) (2.06h) *IR Com (~15mag) (2.09h)!SDSS J (~18mag) (2.40h)!CTCV J (~16mag) (2.13h)?TY Psa (~14mag) (2.02h)!V Per (~18mag) (2.57h)!DD Cir (~20mag) (2.34h)!V630 Sgr (~18mag) (2.83h)!QU Vul (~19mag) (2.68h)!V597 Pup (>18mag) (2.6687h)

13 Photometries for AM Her (Dai et al., 2012, in preparation) It locates at the upper edge of period gap. Its secular evolution state is a key factor to test the current evolution theory. Collected from AAVSO and our photometries

14 New O-C diagram of AM Her A typical period decrease rate ~ Low-state data just add the large scatters

15 The orbital period variations Cyclical Secular Log(P mod ) = -0.36(±0.10)Log(Ω) ² A combined masses of 0.78M sun (WD) M sun (RD) means that mass transfer E0/Emin<<1 in AM Her with an average mass transfer rate M sun yr -1 only induces the orbital period increase(gänsicke et al., 2001). ² This increase can be counteracted by the gravitational radiation. ² R 3 /a ~ 10 3 ² The magnetic braking may be suppressed ² in Mpolars 3 (min)/m (Cumming, 2 ~ ). Including Algol, RS CVn,WUMa and CVs (Lanza & Rodonò,1999)

16 Decreasing orbital period (Qian et al., MNRASL, 2011) (Qian et al., ApJL, 2008) HU Aqr(b) HU Aqr (c) Amplitude (d) (17) (14) Eccentricity (±0.15) Period (yr) 6.54(±0.01) 11.96(±1.41) Solar Titus-Bode relation Distance (au) 3.6(±0.8) 5.4(±0.9) Masses (Jup) 5.9(±0.6) HU Aqr 4.5(±0.5) HW Vir P cycle =15.7 yr A cycle = d A planetary system with three giant planets

17 Can we find the orbital period increase? λ( q) Rcr Porb q 1 In conservative case Normal CVs cannot sustain conservative mass transfer. It obviously conflicts with hypothesis of CV evolution We need to pay more attention to the increasing O-C diagrams

18 Possible increasing orbital period (Dai et al., in preparation) E0/Emin~4 (Dai et al., MNRAS, 2010) V348 Pup UZ For UZ For The more increase observations in a decrease long base It Different line should are necessary be model a substellar can for result checking object out for both this totally models increasing opposite (>90% trend variation probability) trend

19 Summary The orbital period distribution for different subtype exhibits the complication of gap. Part of the eclipsing CVs inside gap never give us definite secular evolutional information Most of modulations in O-Cs can be explained by light travel-time effect

20 Thanks for your attention!

Orbital period analyses for the CVs inside the period gap

Orbital period analyses for the CVs inside the period gap Mem. S.A.It. Vol. 83, 614 c SAIt 2012 Memorie della Orbital period analyses for the CVs inside the period gap Z.-B. Dai 1,2 and S.-B. Qian 1,2 1 National Astronomical Observatories/Yunnan Observatory,

More information

Orbital period analysis of eclipsing Z Cam-type Dwarf Nova EM Cygni: Evidence of magnetic braking and a third body

Orbital period analysis of eclipsing Z Cam-type Dwarf Nova EM Cygni: Evidence of magnetic braking and a third body Orbital period analysis of eclipsing Z Cam-type Dwarf Nova EM Cygni: Evidence of magnetic braking and a third body arxiv:1006.1206v2 [astro-ph.sr] 23 Jul 2010 Zhibin Dai 1,2, Shengbang Qian 1,2 July 26,

More information

PoS(SSC2015)051. Multi-tomography of polars from SALT spectroscopy

PoS(SSC2015)051. Multi-tomography of polars from SALT spectroscopy from SALT spectroscopy Stephen B. Potter 1 South African Astronomical Observatory Cape Town, South Africa E-mail: sbp@saao.ac.za Enrico J. Kotze South African Astronomical Observatory and Astrophysics,

More information

WANTED THE TRUE BOUNCE -BACK SYSTEMS

WANTED THE TRUE BOUNCE -BACK SYSTEMS WANTED THE TRUE BOUNCE -BACK SYSTEMS Paczynski, B. & Sienkiewicz, R., 1981, ApJ, 248, L27 Paczynski, 1981, AcA, 31, 1 After reach the period minimum the CVs should be evolving back toward longer periods

More information

Extrasolar Planets. Methods of detection Characterization Theoretical ideas Future prospects

Extrasolar Planets. Methods of detection Characterization Theoretical ideas Future prospects Extrasolar Planets Methods of detection Characterization Theoretical ideas Future prospects Methods of detection Methods of detection Methods of detection Pulsar timing Planetary motion around pulsar

More information

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS Main Categories of Compact Systems Formation of Compact Objects Mass and Angular Momentum Loss Evolutionary Links to Classes of Binary Systems Future Work

More information

Searching for Other Worlds

Searching for Other Worlds Searching for Other Worlds Lecture 32 1 In-Class Question What is the Greenhouse effect? a) Optical light from the Sun is reflected into space while infrared light passes through the atmosphere and heats

More information

GR VIRGINIS: A DEEP OVERCONTACT BINARY

GR VIRGINIS: A DEEP OVERCONTACT BINARY The Astronomical Journal, 128:2430 2434, 2004 November # 2004. The American Astronomical Society. All rights reserved. Printed in U.S.A. GR VIRGINIS: A DEEP OVERCONTACT BINARY S.-B. Qian and Y.-G. Yang

More information

Ay123 Set 1 solutions

Ay123 Set 1 solutions Ay13 Set 1 solutions Mia de los Reyes October 18 1. The scale of the Sun a Using the angular radius of the Sun and the radiant flux received at the top of the Earth s atmosphere, calculate the effective

More information

CATACLYSMIC VARIABLES. AND THE TYPE Ia PROGENITOR PROBLEM PROGENITOR PROBLEM

CATACLYSMIC VARIABLES. AND THE TYPE Ia PROGENITOR PROBLEM PROGENITOR PROBLEM CATACLYSMIC VARIABLES AND THE TYPE Ia PROGENITOR PROBLEM PROGENITOR PROBLEM Lorne Nelson SNOVAE07 Feb. 23, 2007 Cataclysmic Variables CVs are characterized by a low-mass star/bd (donor) losing mass to

More information

arxiv: v2 [astro-ph] 18 Dec 2008

arxiv: v2 [astro-ph] 18 Dec 2008 Planet influence on the shape of the hosting star - ellipsoidal variations of tau Bootis W. Dimitrov Astronomical Observatory of Adam Mickiewicz University ul. S loneczna 36, 60-286 Poznań, Poland dimitrov@amu.edu.pl

More information

Reanalysis of the Orbital Period Variations of Two DLMR Overcontact Binaries: FG Hya and GR Vir

Reanalysis of the Orbital Period Variations of Two DLMR Overcontact Binaries: FG Hya and GR Vir Research in Astron. Astrophys. Vol.0 (200x) No.0, 000 000 http://www.raa-journal.org http://www.iop.org/journals/raa Research in Astronomy and Astrophysics Reanalysis of the Orbital Period Variations of

More information

Star-planet interaction and planetary characterization methods

Star-planet interaction and planetary characterization methods Star-planet interaction and planetary characterization methods K. G. Kislyakova (1), H. Lammer (1), M. Holmström (2), C.P. Johnstone (3) P. Odert (4), N.V. Erkaev (5,6) (1) Space Research Institute (IWF),

More information

Monitoring orbital period variations in eclipsing white dwarf binaries

Monitoring orbital period variations in eclipsing white dwarf binaries Monitoring orbital period variations in eclipsing white dwarf binaries Madelon Bours Tom Marsh, Steven Parsons Astronomy & Astrophysics Group - University of Warwick - UK RAS Meeting London, January 11,

More information

arxiv: v1 [astro-ph.sr] 21 Nov 2018

arxiv: v1 [astro-ph.sr] 21 Nov 2018 DE CVn: an eclipsing post-common envelope binary with a circumbinary disk and a giant planet arxiv:1811.08625v1 [astro-ph.sr] 21 Nov 2018 Han Z.-T 1,2,3,4, Qian S.-B 1,2,3,4,5, Zhu L.-Y 1,3,4,5, Zhi Q.-J

More information

Mean-Motion Resonance and Formation of Kirkwood Gaps

Mean-Motion Resonance and Formation of Kirkwood Gaps Yan Wang Project 1 PHYS 527 October 13, 2008 Mean-Motion Resonance and Formation of Kirkwood Gaps Introduction A histogram of the number of asteroids versus their distance from the Sun shows some distinct

More information

Thermal-timescale mass transfer and magnetic CVs

Thermal-timescale mass transfer and magnetic CVs IAU Colloquium 190 on Magnetic Cataclysmic Variables ASP Conference Series, Vol. 315, 2004 Sonja Vrielmann & Mark Cropper, eds. Thermal-timescale mass transfer and magnetic CVs Klaus Schenker, Graham A.

More information

AP Physics C Textbook Problems

AP Physics C Textbook Problems AP Physics C Textbook Problems Chapter 13 Pages 412 416 HW-16: 03. A 200-kg object and a 500-kg object are separated by 0.400 m. Find the net gravitational force exerted by these objects on a 50.0-kg object

More information

Name Period Date Earth and Space Science. Solar System Review

Name Period Date Earth and Space Science. Solar System Review Name Period Date Earth and Space Science Solar System Review 1. is the spinning a planetary object on its axis. 2. is the backward motion of planets. 3. The is a unit less number between 0 and 1 that describes

More information

Binary Stars (continued) ASTR 2120 Sarazin. γ Caeli - Binary Star System

Binary Stars (continued) ASTR 2120 Sarazin. γ Caeli - Binary Star System Binary Stars (continued) ASTR 2120 Sarazin γ Caeli - Binary Star System Visual Binaries: Types of Binary Stars Spectroscopic Binaries: Eclipsing Binaries: Periodic changes in brightness, stars block one

More information

Distribution of X-ray binary stars in the Galaxy (RXTE) High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars

Distribution of X-ray binary stars in the Galaxy (RXTE) High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars Distribution of X-ray binary stars in the Galaxy (RXTE) Robert Laing Primary Compact accreting binary systems Compact star WD NS BH

More information

University of Central Florida Department of Physics, PSB 132, 4000 University Blvd., Orlando, FL, USA

University of Central Florida Department of Physics, PSB 132, 4000 University Blvd., Orlando, FL, USA University of Central Florida Department of Physics, PSB 132, 4000 University Blvd., Orlando, FL, USA E-mail: montgomery@physics.ucf.edul In this work, we review the evolutionary sequence of close binary

More information

Planets around evolved stellar systems. Tom Marsh, Department of Physics, University of Warwick

Planets around evolved stellar systems. Tom Marsh, Department of Physics, University of Warwick Planets around evolved stellar systems Tom Marsh Department of Physics, University of Warwick Tom Marsh, Department of Physics, University of Warwick Slide 1 / 35 Tom Marsh, Department of Physics, University

More information

Starspot Magnetic Fields

Starspot Magnetic Fields Starspot Magnetic Fields Adriana (Silva) Valio CRAAM Universidade Presbiteriana Mackenzie Precision Spectroscopy: Toward Earth 2.0 01-04/08/2017 Spot detection during transit Very likely, all cool stars

More information

DEPARTMENT OF PHYSICS AND ASTRONOMY. Planets around white dwarfs Matt Burleigh

DEPARTMENT OF PHYSICS AND ASTRONOMY. Planets around white dwarfs Matt Burleigh DEPARTMENT OF PHYSICS AND ASTRONOMY Planets around white dwarfs Matt Burleigh Contents Original motivation DODO - results from our direct imaging survey Where do we go next? The role for E-ELT Direct imaging

More information

Fundamental (Sub)stellar Parameters: Surface Gravity. PHY 688, Lecture 11

Fundamental (Sub)stellar Parameters: Surface Gravity. PHY 688, Lecture 11 Fundamental (Sub)stellar Parameters: Surface Gravity PHY 688, Lecture 11 Outline Review of previous lecture binary stars and brown dwarfs (sub)stellar dynamical masses and radii Surface gravity stars,

More information

6 th lecture of Compact Object and Accretion, Master Programme at Leiden Observatory

6 th lecture of Compact Object and Accretion, Master Programme at Leiden Observatory 6 th lecture of Compact Object and Accretion, Master Programme at Leiden Observatory Accretion 1st class study material: Chapter 1 & 4, accretion power in astrophysics these slides at http://home.strw.leidenuniv.nl/~emr/coa/

More information

A period investigation of the overcontact binary system V417 Aquilae. Qian Shengbang 1,2. Min.I = ḍ E (1)

A period investigation of the overcontact binary system V417 Aquilae. Qian Shengbang 1,2. Min.I = ḍ E (1) A&A 400, 649 653 (2003) DOI: 10.1051/0004-6361:20030018 c ESO 2003 Astronomy & Astrophysics A period investigation of the overcontact binary system V417 Aquilae Qian Shengbang 1,2 1 National Astronomical

More information

arxiv:astro-ph/ v1 10 May 2006

arxiv:astro-ph/ v1 10 May 2006 **FULL TITLE** ASP Conference Series, Vol. **VOLUME**, **YEAR OF PUBLICATION** **NAMES OF EDITORS** Newly arising problems in the research of SU UMa-type dwarf novae from VSNET collaborations arxiv:astro-ph/0605246v1

More information

Thermal pressure vs. magnetic pressure

Thermal pressure vs. magnetic pressure Thermal pressure vs. magnetic pressure The Earth The auroral oval: bremsstrahlung and lines induced by electrons precipitating through the Earth s magnetic field (LX ~ 10 14 erg/s ~ 2 kg TNT equivalent/s)

More information

The role of SW Sex stars in the evolution of CVs

The role of SW Sex stars in the evolution of CVs European Southern Observatory Chile Wild Stars in the West II, Tucson 2009 The orbital period distribution SW Sextantis stars in a nutshell Original definition (Thorstensen et al. 1991, AJ 102, 272): novalike

More information

Exoplanet Search Techniques: Overview. PHY 688, Lecture 28 April 3, 2009

Exoplanet Search Techniques: Overview. PHY 688, Lecture 28 April 3, 2009 Exoplanet Search Techniques: Overview PHY 688, Lecture 28 April 3, 2009 Course administration final presentations Outline see me for paper recommendations 2 3 weeks before talk see me with draft of presentation

More information

Variable Stars South. Who we are What we do. 2

Variable Stars South. Who we are What we do.   2 Who we are What we do www.variablestarssouth.org 2 We are a group of amateur astronomers. Mainly from Australia New Zealand with a few from other parts of the globe We study stars that vary in brightness

More information

10/16/ Detecting Planets Around Other Stars. Chapter 10: Other Planetary Systems The New Science of Distant Worlds

10/16/ Detecting Planets Around Other Stars. Chapter 10: Other Planetary Systems The New Science of Distant Worlds 10/16/17 Lecture Outline 10.1 Detecting Planets Around Other Stars Chapter 10: Other Planetary Systems The New Science of Distant Worlds Our goals for learning: How do we detect planets around other stars?

More information

Cataclysmic variables

Cataclysmic variables Cataclysmic variables Sander Bus Kapteyn Astronomical Institute Groningen October 6, 2011 Overview Types of cataclysmic stars How to form a cataclysmic variable X-ray production Variation in outburst lightcurve,

More information

Names: Team: Team Number:

Names: Team: Team Number: Astronomy C Michigan Region 8 March 11, 2017 Names: Team: Team Number: Directions 1. There is a separate answer sheet. Answers written elsewhere (e.g. on the test) will not be considered. 2. You may take

More information

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies?

Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies? Components of Galaxies Stars What Properties of Stars are Important for Understanding Galaxies? Temperature Determines the λ range over which the radiation is emitted Chemical Composition metallicities

More information

10/25/2010. Stars, Galaxies & the Universe Announcements. Stars, Galaxies & the Universe Lecture Outline. Reading Quiz #9 Wednesday (10/27)

10/25/2010. Stars, Galaxies & the Universe Announcements. Stars, Galaxies & the Universe Lecture Outline. Reading Quiz #9 Wednesday (10/27) Stars, Galaxies & the Universe Announcements Reading Quiz #9 Wednesday (10/27) HW#8 in ICON due Friday (10/29) by 5 pm - available Wednesday 1 Stars, Galaxies & the Universe Lecture Outline 1. Black Holes

More information

7. BINARY STARS (ZG: 12; CO: 7, 17)

7. BINARY STARS (ZG: 12; CO: 7, 17) 7. BINARY STARS (ZG: 12; CO: 7, 17) most stars are members of binary systems or multiple systems (triples, quadruples, quintuplets,...) orbital period distribution: P orb = 11 min to 10 6 yr the majority

More information

Observed Properties of Stars - 2 ASTR 2110 Sarazin

Observed Properties of Stars - 2 ASTR 2110 Sarazin Observed Properties of Stars - 2 ASTR 2110 Sarazin Properties Location Distance Speed Radial velocity Proper motion Luminosity, Flux Magnitudes Magnitudes Stellar Colors Stellar Colors Stellar Colors Stars

More information

Exoplanetary Atmospheres: Atmospheric Dynamics of Irradiated Planets. PHY 688, Lecture 24 Mar 23, 2009

Exoplanetary Atmospheres: Atmospheric Dynamics of Irradiated Planets. PHY 688, Lecture 24 Mar 23, 2009 Exoplanetary Atmospheres: Atmospheric Dynamics of Irradiated Planets PHY 688, Lecture 24 Mar 23, 2009 Outline Review of previous lecture: atmospheric temperature structure of irradiated planets isothermal

More information

Ay101 Set 1 solutions

Ay101 Set 1 solutions Ay11 Set 1 solutions Ge Chen Jan. 1 19 1. The scale of the Sun a 3 points Venus has an orbital period of 5 days. Using Kepler s laws, what is its semi-major axis in units of AU Start with Kepler s third

More information

Surface and Circumstellar Structures in Early-Type Interacting Binaries

Surface and Circumstellar Structures in Early-Type Interacting Binaries Surface and Circumstellar Structures in Early-Type Interacting Binaries Geraldine J. Peters Space Sciences Center & Department of Physics and Astronomy University of Southern California Los Angeles, CA

More information

Lecture 13: Binary evolution

Lecture 13: Binary evolution Lecture 13: Binary evolution Senior Astrophysics 2017-04-12 Senior Astrophysics Lecture 13: Binary evolution 2017-04-12 1 / 37 Outline 1 Conservative mass transfer 2 Non-conservative mass transfer 3 Cataclysmic

More information

Origins of Gas Giant Planets

Origins of Gas Giant Planets Origins of Gas Giant Planets Ruth Murray-Clay Harvard-Smithsonian Center for Astrophysics Image Credit: NASA Graduate Students Piso Tripathi Dawson Undergraduates Wolff Lau Alpert Mukherjee Wolansky Jackson

More information

arxiv:astro-ph/ v1 23 Oct 2002

arxiv:astro-ph/ v1 23 Oct 2002 Evolution of the symbiotic nova RX Puppis J. Mikołajewska, E. Brandi, L. Garcia, O. Ferrer, C. Quiroga and G.C. Anupama arxiv:astro-ph/0210505v1 23 Oct 2002 N. Copernicus Astronomical Center, Bartycka

More information

The Hertzprung-Russell Diagram. The Hertzprung-Russell Diagram. Question

The Hertzprung-Russell Diagram. The Hertzprung-Russell Diagram. Question Key Concepts: Lecture 21: Measuring the properties of stars (cont.) The Hertzsprung-Russell (HR) Diagram (L versus T) The Hertzprung-Russell Diagram The Stefan-Boltzmann Law: flux emitted by a black body

More information

Space Science Jeopardy!

Space Science Jeopardy! Space Science Jeopardy! Structure of the Universe Stars & HR Diagram Seasons, Tides, Phases, Eclipses Astronomical Bodies The Sun & Gravity 10 10 10 10 10 20 20 20 20 20 30 30 30 30 30 40 40 40 40 40 50

More information

Lines of Hydrogen. Most prominent lines in many astronomical objects: Balmer lines of hydrogen

Lines of Hydrogen. Most prominent lines in many astronomical objects: Balmer lines of hydrogen The Family of Stars Lines of Hydrogen Most prominent lines in many astronomical objects: Balmer lines of hydrogen The Balmer Thermometer Balmer line strength is sensitive to temperature: Most hydrogen

More information

Two projects without apparent connection?

Two projects without apparent connection? Two projects without apparent connection? SW Sextantis stars SW Sextantis stars The golden age of surveys, Gänsicke 2005, Strassbourg SW Sextantis stars an introduction Original definition (Thorstensen

More information

Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION

Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION Accretion Discs Mathematical Tripos, Part III Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION 0.1. Accretion If a particle of mass m falls from infinity and comes to rest on the surface of a star of mass

More information

Symbiotic stars: challenges to binary evolution theory. Joanna Mikołajewska Copernicus Astronomical Center, Warsaw

Symbiotic stars: challenges to binary evolution theory. Joanna Mikołajewska Copernicus Astronomical Center, Warsaw Symbiotic stars: challenges to binary evolution theory Joanna Mikołajewska Copernicus Astronomical Center, Warsaw Symbiotic stars S(stellar) normal giant 80% M g ~10-7 M sun /yr P orb ~ 1-15 yr Accreting

More information

Revision: Sun, Stars (and Planets) See web slides of Dr Clements for Planets revision. Juliet Pickering Office: Huxley 706

Revision: Sun, Stars (and Planets) See web slides of Dr Clements for Planets revision. Juliet Pickering Office: Huxley 706 Revision: Sun, Stars (and Planets) See web slides of Dr Clements for Planets revision Juliet Pickering Office: Huxley 706 Office hour (Pickering): Thursday 22nd May 12-11 pm Outline overview of first part

More information

UV Observations of Cataclysmic Variables and their role in multiband studies

UV Observations of Cataclysmic Variables and their role in multiband studies UV Observations of Cataclysmic Variables and their role in multiband studies D.de Martino INAF-Osservatorio Astronomico di Capodimonte Napoli & B.T. Gaensicke; K.Long, T.R.Marsh, E. Sion, P. Szkody Outline

More information

Exoplanets: a dynamic field

Exoplanets: a dynamic field Exoplanets: a dynamic field Alexander James Mustill Amy Bonsor, Melvyn B. Davies, Boris Gänsicke, Anders Johansen, Dimitri Veras, Eva Villaver The (transiting) exoplanet population Solar System Hot Jupiters:

More information

Extrasolar Planets: Ushering in the Era of Comparative Exoplanetology

Extrasolar Planets: Ushering in the Era of Comparative Exoplanetology Extrasolar Planets: Ushering in the Era of Comparative Exoplanetology A. Sozzetti INAF Osservatorio Astrofisico di Torino Detection/Characterization Detection (Visible): - Doppler spectroscopy (95%) -

More information

Actuality of Exoplanets Search. François Bouchy OHP - IAP

Actuality of Exoplanets Search. François Bouchy OHP - IAP Actuality of Exoplanets Search François Bouchy OHP - IAP How detect extrasolar planets? Two main difficulties : 1 A tiny angular separation 0.75 arcsec Sun Jupiter at 4 light years 4 Sun Jupiter at 100

More information

A Survey of Stellar Families Multiplicity of Solar-type Stars

A Survey of Stellar Families Multiplicity of Solar-type Stars A Survey of Stellar Families Multiplicity of Solar-type Stars Advisor: Dr. Hal McAlister GSU Committee members: Dr. Doug Gies GSU Deepak Raghavan Ph.D. Dissertation Talk March 17, 2009 Dr. Todd Henry GSU

More information

Spectroscopy, the Doppler Shift and Masses of Binary Stars

Spectroscopy, the Doppler Shift and Masses of Binary Stars Doppler Shift At each point the emitter is at the center of a circular wavefront extending out from its present location. Spectroscopy, the Doppler Shift and Masses of Binary Stars http://apod.nasa.gov/apod/astropix.html

More information

arxiv:astro-ph/ v1 8 May 2002

arxiv:astro-ph/ v1 8 May 2002 Mon. Not. R. Astron. Soc., () Printed 31 May 217 (MN LATEX style file v2.2) Blunting the Spike: the CV Minimum Period A.R. King 1, K. Schenker 1, J.M. Hameury 2 1. Theoretical Astrophysics Group, University

More information

Chapter 12 Stellar Evolution

Chapter 12 Stellar Evolution Chapter 12 Stellar Evolution Guidepost Stars form from the interstellar medium and reach stability fusing hydrogen in their cores. This chapter is about the long, stable middle age of stars on the main

More information

Optical Photometry of Dwarf Nova QZ Serpentis in Quiescence

Optical Photometry of Dwarf Nova QZ Serpentis in Quiescence Optical Photometry of Dwarf Nova QZ Serpentis in Quiescence Erica D. Jones Center for Astrophysics, Space Physics and Engineering Research at Baylor University Dr. Dwight Russell Department of Physics

More information

Lecture 20: Planet formation II. Clues from Exoplanets

Lecture 20: Planet formation II. Clues from Exoplanets Lecture 20: Planet formation II. Clues from Exoplanets 1 Outline Definition of a planet Properties of exoplanets Formation models for exoplanets gravitational instability model core accretion scenario

More information

Fundamental (Sub)stellar Parameters: Masses and Radii. PHY 688, Lecture 10

Fundamental (Sub)stellar Parameters: Masses and Radii. PHY 688, Lecture 10 Fundamental (Sub)stellar Parameters: Masses and Radii PHY 688, Lecture 10 Outline Review of previous lecture brown dwarf effective temperatures finding cool brown dwarfs current problem: what are the coolest

More information

Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version

Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version Analyzing X-Ray Pulses from Stellar Cores Pencil & Paper Version Purpose: To determine if two end products of stellar evolution GK Per and Cen X-3 could be white dwarfs or neutron stars by calculating

More information

Science Olympiad Astronomy C Division Event National Exam

Science Olympiad Astronomy C Division Event National Exam Science Olympiad Astronomy C Division Event National Exam University of Nebraska-Lincoln May 15-16, 2015 Team Number: Team Name: Instructions: 1) Please turn in all materials at the end of the event. 2)

More information

Stellar Astronomy Sample Questions for Exam 3

Stellar Astronomy Sample Questions for Exam 3 Stellar Astronomy Sample Questions for Exam 3 Chapter 7 1. A protostar is formed by a) the rapid expansion of gas from an exploding star. b) the gravitational collapse of a rotating interstellar cloud.

More information

Stellar Models ASTR 2110 Sarazin

Stellar Models ASTR 2110 Sarazin Stellar Models ASTR 2110 Sarazin Jansky Lecture Tuesday, October 24 7 pm Room 101, Nau Hall Bernie Fanaroff Observing the Universe From Africa Trip to Conference Away on conference in the Netherlands

More information

Evolution of binary stars

Evolution of binary stars Evolution of binary stars 1 Outline What is a binary? Mass transfer in binary systems Evolution in binary stars Late evolutionary states MESA 2 1 What are binary systems? CM X a 1 a 2 m 1 m 2 3 What are

More information

EART164: PLANETARY ATMOSPHERES

EART164: PLANETARY ATMOSPHERES EART164: PLANETARY ATMOSPHERES Francis Nimmo Last Week - Dynamics Reynolds number, turbulent vs. laminar flow Velocity fluctuations, Kolmogorov cascade Brunt-Vaisala frequency, gravity waves Rossby waves,

More information

Extrasolar Transiting Planets: Detection and False Positive Rejection

Extrasolar Transiting Planets: Detection and False Positive Rejection 4 Harvard-Smithsonian Center for Astrophysics Extrasolar Transiting Planets: Detection and False Positive Rejection Willie Torres Harvard-Smithsonian Center for Astrophysics Young Planetary Systems Workshop

More information

10/26/ Star Birth. Chapter 13: Star Stuff. How do stars form? Star-Forming Clouds. Mass of a Star-Forming Cloud. Gravity Versus Pressure

10/26/ Star Birth. Chapter 13: Star Stuff. How do stars form? Star-Forming Clouds. Mass of a Star-Forming Cloud. Gravity Versus Pressure 10/26/16 Lecture Outline 13.1 Star Birth Chapter 13: Star Stuff How do stars form? Our goals for learning: How do stars form? How massive are newborn stars? Star-Forming Clouds Stars form in dark clouds

More information

Long-time behavior of orbital periods of some Algol-type eclipsing binaries

Long-time behavior of orbital periods of some Algol-type eclipsing binaries ASTRONOMY & ASTROPHYSICS NOVEMBER I 2000, PAGE 377 SUPPLEMENT SERIES Astron. Astrophys. Suppl. Ser. 146, 377 384 (2000) Long-time behavior of orbital periods of some Algol-type eclipsing binaries Qian

More information

Searching For Planets Like Earth around stars like the Sun

Searching For Planets Like Earth around stars like the Sun Searching For Planets Like Earth around stars like the Sun Derek Buzasi FGCU Roadmap Who am I and how did I get here? Motivation for my research What makes a star like the Sun? How do we find planets?

More information

AST Section 2: Test 2

AST Section 2: Test 2 AST1002 - Section 2: Test 2 Date: 11/05/2009 Name: Equations: E = m c 2 Question 1: The Sun is a stable star because 1. gravity balances forces from pressure. (!) Miniquiz 7, Q3 2. the rate of fusion equals

More information

The observations of deeply eclipsing polars FL Ceti and CSS :

The observations of deeply eclipsing polars FL Ceti and CSS : Mem. S.A.It. Vol. 83, 670 c SAIt 2012 Memorie della The observations of deeply ipsing polars FL Ceti and CSS 081231: 071126+440405 N. Katysheva 1 and S. Shugarov 1,2 1 Lomonosov Moscow State University,

More information

READ: Chapter 11.1, 11.2 (11.2.1, only), 11.3(

READ: Chapter 11.1, 11.2 (11.2.1, only), 11.3( HW READ: Chapter 11.1, 11.2 (11.2.1,11.2.2 only), 11.3( 11.3.1,11.3.2 only), 11.4,11.5 Question 11.2(HW#15) Problems 1(HW#16) (part a: recall: basic KE=1/2mv 2,Part tb: recall momentum conservation M f

More information

Microlensing Parallax with Spitzer

Microlensing Parallax with Spitzer Microlensing Parallax with Spitzer Pathway to the Galactic Distribution of Planets 2015 Sagan/Michelson Fellows Symposium May 7-8, 2015 Caltech Sebastiano Calchi Novati Sagan Visiting Fellow NExScI (Caltech),

More information

Formation Mechanisms of Brown Dwarfs: Observations & Theories. Dan Li April 2009

Formation Mechanisms of Brown Dwarfs: Observations & Theories. Dan Li April 2009 Formation Mechanisms of Brown Dwarfs: Observations & Theories Dan Li April 2009 What is brown dwarf (BD)? BD Mass : upper-limit ~ 0.075 M lower-limit ~ 0.013 M (?) Differences between BD and giant planet:

More information

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Homework Ch 7, 8, 9 Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) Our most detailed knowledge of Uranus and Neptune comes from 1) A) the

More information

Several Methods of Estimating Times of Minima in Cataclysmic Variables And Some Fesults for EX Dra

Several Methods of Estimating Times of Minima in Cataclysmic Variables And Some Fesults for EX Dra WDS'2 Proceedings of Contributed Papers, Part III, 6 22, 22. ISBN 978-8-7378-226-9 MATFYZPRESS Several Methods of Estimating Times of Minima in Cataclysmic Variables And Some Fesults for EX Dra L. Pilarčík

More information

Pulsations and planets at late stages of stellar evolution

Pulsations and planets at late stages of stellar evolution at late stages of stellar evolution 1,2 1 Eberhard-Karls-Universität Tübingen 2 Georg-August-Universität Göttingen Kepler Kolloquium, November 6 2009 1 2 Subdwarf B stars 3 PG 1159 white dwarfs at late

More information

HR Diagram, Star Clusters, and Stellar Evolution

HR Diagram, Star Clusters, and Stellar Evolution Ay 1 Lecture 9 M7 ESO HR Diagram, Star Clusters, and Stellar Evolution 9.1 The HR Diagram Stellar Spectral Types Temperature L T Y The Hertzsprung-Russel (HR) Diagram It is a plot of stellar luminosity

More information

Tidal Dissipation in Binaries

Tidal Dissipation in Binaries Tidal Dissipation in Binaries From Merging White Dwarfs to Exoplanetary Systems Dong Lai Cornell University March 14, 2013, Harvard ITC Colloquium Tidal Dissipation in Binaries I. Merging White Dwarf Binaries

More information

Habitable exoplanets: modeling & characterization

Habitable exoplanets: modeling & characterization Habitable exoplanets: modeling & characterization F. Selsis CNRS, Bordeaux, France flux at 10 pc (photons m -2 hr -1 µm -1 ) R. Wordsworth, F. Forget Laboratoire de Meteorologie Dynamique (LMD), Paris

More information

Lecture Outlines. Chapter 20. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

Lecture Outlines. Chapter 20. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc. Lecture Outlines Chapter 20 Astronomy Today 8th Edition Chaisson/McMillan Chapter 20 Stellar Evolution Units of Chapter 20 20.1 Leaving the Main Sequence 20.2 Evolution of a Sun-Like Star 20.3 The Death

More information

The Evolution of Low Mass Stars

The Evolution of Low Mass Stars The Evolution of Low Mass Stars Key Ideas: Low Mass = M < 4 M sun Stages of Evolution of a Low Mass star: Main Sequence star star star Asymptotic Giant Branch star Planetary Nebula phase White Dwarf star

More information

Boris Gänsicke. Eclipsing binaries, something different. York 2014 To commemorate the 250th anniversary of the birth of John Goodricke

Boris Gänsicke. Eclipsing binaries, something different. York 2014 To commemorate the 250th anniversary of the birth of John Goodricke Boris Gänsicke Eclipsing binaries, something different York 2014 To commemorate the 250th anniversary of the birth of John Goodricke John Goodricke White dwarfs Cosmology Eclipsing binaries Masses and

More information

Importance of the study of extrasolar planets. Exoplanets Introduction. Importance of the study of extrasolar planets

Importance of the study of extrasolar planets. Exoplanets Introduction. Importance of the study of extrasolar planets Importance of the study of extrasolar planets Exoplanets Introduction Planets and Astrobiology (2017-2018) G. Vladilo Technological and scientific spin-offs Exoplanet observations are driving huge technological

More information

The Stars. Chapter 14

The Stars. Chapter 14 The Stars Chapter 14 Great Idea: The Sun and other stars use nuclear fusion reactions to convert mass into energy. Eventually, when a star s nuclear fuel is depleted, the star must burn out. Chapter Outline

More information

Observed Properties of Stars - 2 ASTR 2120 Sarazin

Observed Properties of Stars - 2 ASTR 2120 Sarazin Observed Properties of Stars - 2 ASTR 2120 Sarazin Properties Location Distance Speed Radial velocity Proper motion Luminosity, Flux Magnitudes Magnitudes Hipparchus 1) Classified stars by brightness,

More information

Globular Clusters. This list contains 135 of the brightest and largest globular clusters from the Astroleague's observing program/list.

Globular Clusters. This list contains 135 of the brightest and largest globular clusters from the Astroleague's observing program/list. Globular Clusters A globular cluster is a spherical collection of stars that orbit a galactic core as a satellite. Globular clusters are very tightly bound by gravity, giving them their spherical shapes

More information

Extrasolar Planets. Today. Dwarf Planets. Extrasolar Planets. Next week. Review Tuesday. Exam Thursday. also, Homework 6 Due

Extrasolar Planets. Today. Dwarf Planets. Extrasolar Planets. Next week. Review Tuesday. Exam Thursday. also, Homework 6 Due Extrasolar Planets Today Dwarf Planets Extrasolar Planets Next week Review Tuesday Exam Thursday also, Homework 6 Due will count best 5 of 6 homeworks 2007 Pearson Education Inc., publishing as Pearson

More information

Based on the reduction of the intensity of the light from a star with distance. It drops off with the inverse square of the distance.

Based on the reduction of the intensity of the light from a star with distance. It drops off with the inverse square of the distance. 6/28 Based on the reduction of the intensity of the light from a star with distance. It drops off with the inverse square of the distance. Intensity is power per unit area of electromagnetic radiation.

More information

Heading for death. q q

Heading for death. q q Hubble Photos Credit: NASA, The Hubble Heritage Team (STScI/AURA) Heading for death. q q q q q q Leaving the main sequence End of the Sunlike star The helium core The Red-Giant Branch Helium Fusion Helium

More information

THE AGE OF THE KIC SYSTEM. James MacDonald and D. J. Mullan Department of Physics and Astronomy, DE 19716, USA

THE AGE OF THE KIC SYSTEM. James MacDonald and D. J. Mullan Department of Physics and Astronomy, DE 19716, USA THE AGE OF THE KIC 7177553 SYSTEM James MacDonald and D. J. Mullan Department of Physics and Astronomy, DE 19716, USA ABSTRACT KIC 7177553 is a quadruple system containing two binaries of orbital periods

More information

Relativity and Astrophysics Lecture 15 Terry Herter. RR Lyrae Variables Cepheids Variables Period-Luminosity Relation. A Stellar Properties 2

Relativity and Astrophysics Lecture 15 Terry Herter. RR Lyrae Variables Cepheids Variables Period-Luminosity Relation. A Stellar Properties 2 Stellar Properties Relativity and Astrophysics Lecture 15 Terry Herter Outline Spectroscopic Parallax Masses of Stars Periodic Variable Stars RR Lyrae Variables Cepheids Variables Period-Luminosity Relation

More information

Kozai-Lidov oscillations

Kozai-Lidov oscillations Kozai-Lidov oscillations Kozai (1962 - asteroids); Lidov (1962 - artificial satellites) arise most simply in restricted three-body problem (two massive bodies on a Kepler orbit + a test particle) e.g.,

More information

Friday, September 23, 2011

Friday, September 23, 2011 Friday, September 23, 2011 Astronomy in the news? Fall Equinox Friday, September 23 at 4:05 a.m. Story on Tatooine planet in double star system in Thursday s Texan. Upper Atmosphere Research Satellite,

More information

Physical Parameters of KID , a Low-Mass, Double- Lined Eclipsing Binary

Physical Parameters of KID , a Low-Mass, Double- Lined Eclipsing Binary Physical Parameters of KID 6131659, a Low-Mass, Double- Lined Eclipsing Binary Gideon Bass Jerome Orosz, William Welsh, Gur Windmiller, Trevor Gregg, Tara Fetherolf, Richard Wade, Samuel Quinn Paper available

More information