Black Hole Event Horizon

Slides:



Advertisements
Similar presentations
Estimating the Spin of Stellar-Mass Black Holes Jeffrey McClintock Harvard-Smithsonian CfA STScI Black Hole Symposium April 25, 2007.
Advertisements

Neutron Stars and Black Holes Please press “1” to test your transmitter.
Neutron Stars and Black Holes
Relativistic accretion disks: their dynamics and emission Yuan, Ye-Fei (袁业飞) Department of Astronomy, USTC ( ) Collaborators: Cao, X.; Shen, Z.Q.
Compact Objects Astronomy 315 Professor Lee Carkner Lecture 15.
1. White Dwarf If initial star mass < 8 M Sun or so. (and remember: Maximum WD mass is 1.4 M Sun, radius is about that of the Earth) 2. Neutron Star If.
Towards the Grand Unification of AGNs in Hierarchical Cosmologies Nikos Fanidakis and C.M. Baugh, R.G. Bower, S. Cole, C. Done, C.S. Frenk January 30,
Horizon and exotics. 2 Main reviews and articles gr-qc/ Black Holes in Astrophysics astro-ph/ No observational proof of the black-hole event-horizon.
Black Holes Old ideas for black holes Theory of black holes Real-life black holes Stellar mass Supermassive Speculative stuff (if time)
Announcements Observing Monday-Thursday of this week counts on the third exam. Fourth exam is Wednesday, November 17 Review will be Monday, November 15.
Goal: To understand special stars. Objectives: 1)To learn the basics about Black holes 2)To examine the different sizes/masses of Black holes 3)To learn.
Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole.
Black Hole Chaos The Environments of the most super- massive black holes in the Universe Belinda Wilkes, Chandra X-ray Center, CfA Francesca Civano, CfA.
Quasars Chapter 17. Topics Quasars –characteristics –what are they? –what is their energy source? –where are they? –how old are they? –interactions of.
Ramesh Narayan (McClintock, Shafee, Remillard, Davis, Li)
Astrophysical Black Holes Ramesh Narayan.
MEASURING SPIN PARAMETERS OF STELLAR-MASS BLACK HOLES Ramesh Narayan.
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
Black hole For large enough masses, as far as we know, nothing is stiff enough to stop the collapse. It continues down to a singularity: a defect in space.
Historical SN and their properties Total energy released ~10 54 erg in a few hours.
Black holes and accretion flows Chris Done University of Durham.
ASTR 1200 Announcements Website Second exam will be October 30. Thursday Review materials were posted.
THE BLACK HOLE EVENT HORIZON Ramesh Narayan. The Black Hole A remarkable prediction of the General Theory of Relativity Matter is crushed to a SINGULARITY.
Black Holes Pierre Cieniewicz. What are they? A Black Hole (BH) is a place in space from which nothing can escape The reason for this is gravity Some.
KERR BLACK HOLES Generalized BH description includes spin –Later researchers use it to predict new effects!! Two crucial surfaces –inner surface = horizon.
Accretion onto Black Hole : Advection Dominated Flow
Universe Tenth Edition
Formation of Redback and Black Widow Binary Millisecond Pulsars
Accretion #3 When is the thin disk model valid? Reynolds number, viscosity Time scales in disk BH spectra Using X-ray spectra to determine BH mass and.
Measuring the Spins of Stellar-Mass Black Holes by Fitting the X-ray Continuum Spectrum Jeff McClintock Credit: A. Broderick & E. Mer Probing Strong Gravity.
HOW TO DETECT A BLACK HOLE Effects on matter/light outside the horizon –gravitational attraction of other bodies –“dark star” with mass distinguish from.
Black Holes A stellar mass black hole accreting material from a companion star 1.
ASTROPHYSICAL BLACK HOLES. SOME HISTORY Escape velocity v u 2 = 2 GM/R Earth v esc = 11 km/s Jupiter v esc = 60 km/s Sun v esc = 600 km/s Moon v esc =
Rotating Black Hole Energy Mechanisms Dennis V. Perepelitsa MIT Department of Physics Final Project Presentation 9 May 2007 with Matias Lavista and.
Lively Accreting Black Holes in X-ray Binaries Jeff McClintock Harvard-Smithsonian Center for Astrophysics Black Holes’ New Horizons Oaxaca, May 2016 
Gravitational wave sources
Supernovas Neutron Stars and Black Holes
ASTR 1020 – March 9 Homework 5 due today .
The Role of Magnetic Fields in Black Hole Accretion
What is a black hole? Insert TCP 6e Figure 18.12c.
Neutron Stars and Black Holes
RXTE Spectral Observations of the Galactic Microquasar GRO J1655-40
Zhao-Ming Gan, Ding-Xiong Wang and Yang Li
Lecture 20 Accretion spectrum Gravitational redshift Iron Kα line
Black Hole Binaries in Quiescence
NuSTAR + XMM Observations of NGC 1365: A Constant Inner Disc
黑洞X射线双星的高频准周期振荡(HFQPO)与喷流(Jet)的 相关性
Black Holes.
Myeong-Gu Park (Kyungpook National University, KOREA)
Horizon and exotics.
Black Holes and Neutron Stars
X-ray Properties of Intermediate Mass Black Holes in Dwarf AGN
Chapter 14: The Bizarre Stellar Graveyard
Horizon and exotics.
Neutron Stars and Black Holes
General Relativity in X-ray Astronomy Astrosat and Future Experiments
What is a black hole? Insert TCP 6e Figure 18.12c.
Problem sets 5 and 6 due this week.
Medium-Sized Black Holes
Supernova in images of Greg Thorne and Nick McCaw
Announcements Observing Monday-Thursday of this week counts on the third exam. Fourth exam is Wednesday, November 17 Review will be Monday, November 15.
BH binaries.
Parts, existence of, origin,
Black holes: observations Lecture 7: Horizon and exotics
Black holes: observations Lecture 7: Horizon and exotics
Ricocheting Black Hole Jet Discovered By Chandra
Chandra Science Highlight
Black Holes Chapter 14.
Black Holes Escape velocity Event horizon Black hole parameters
Presentation transcript:

Black Hole Event Horizon A Black Hole has a truly unique property: it possesses an Event Horizon A “virtual” surface One-way membrane --- matter/energy can fall in, but nothing gets out, not even light Event Horizon Singularity

A Black Hole is Amazingly Simple Mass: M Spin: a* (J=a*GM2/c) Charge: Q Even though it is a macroscopic object, a BH is as simple as an elementary particle!

Can We Test These Features? Confirm that astrophysical BHs actually do have Event Horizons Measure the two fundamental parameters of BHs Mass (relatively easy) Spin (much harder) Ramesh Narayan, Jeff McClintock

Do Black Hole Candidates Have Event Horizons? Are Black Hole Candidates really BHs? Can we find independent evidence that our BH candidates actually possess Event Horizons

X-ray Binaries Image credit: Robert Hynes (2002)

Narayan, Garcia & McClintock (1997) The Idea Find BH X-ray Binaries in which the accretion flow radiates very little Objects with surfaces (NSs) will then be much brighter than objects with event horizons (BHs) Look for a huge difference in luminosity Narayan, Garcia & McClintock (1997)

Large difference in luminosity between BHs and NSs is dramatically verified (Narayan, Garcia & McClintock; Garcia et al. 2001; McClintock et al. 2003; …) Black Holes are really black!!  Event Horizon

Black Hole Spin The material from which a BH is formed almost always has angular momentum Also, accretion adds angular momentum So we expect astrophysical BHs to be spinning: J = a*GM2/c, 0  a*  1 Can we measure a*?

The Basic Idea Measure radius of hole by estimating area of the bright inner disk (Zhang et al. 1997; Shafee et al. 2006; McClintock et al. 2006)

Black Hole Parameters X-ray Binary Mass (M) a* 4U1543-47 7.4—11.4 0.75—0.85 LMC X-3 5.9—9.2 < 0.3 GRO J1655-40 6.0—6.6 0.65—0.75 GRS 1915+105 10--18 0.98—1