Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole.

Slides:



Advertisements
Similar presentations
ASTR Fall Semester Joel E. Tohline, Alumni Professor Office: 247 Nicholson Hall [Slides from Lecture17]
Advertisements

1 Stellar Remnants White Dwarfs, Neutron Stars & Black Holes These objects normally emit light only due to their very high temperatures. Normally nuclear.
Black Holes. Dark stars a star that has an escape velocity greater than the speed of light.
Stellar Deaths II Neutron Stars and Black Holes 17.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Copyright © 2010 Pearson Education, Inc. Chapter 13 Black Holes.
1. black hole - region of space where the pull of gravity is so great that even light cannot escape. Possible end of a very massive star.
Black Holes. Outline Escape velocity Definition of a black hole Sizes of black holes Effects on space and time Tidal forces Making black holes Evaporation.
Neutron Stars and Black Holes
Active Galactic Nuclei Chapter 28 Revised Active Galactic Nuclei Come in several varieties; Starburst Nuclei – Nearby normal galaxies with unusually.
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.
Review for Test #3 Sunday 3-5 PM Topics: The Sun Stars (including our Sun) The Interstellar medium Stellar Evolution and Stellar Death for Low mass, medium.
Chapter 22: Black Holes Einstein’s relativity: –Special –General –Relativity and black holes Evidence of black holes Properties of black holes Long-time.
Black Holes Written for Summer Honors Black Holes Massive stars greater than 10 M  upon collapse compress their cores so much that no pressure.
Neutron Stars and Black Holes PHYS390: Astrophysics Professor Lee Carkner Lecture 18.
Black Holes Astronomy 315 Professor Lee Carkner Lecture 16.
Black Holes Old ideas for black holes Theory of black holes Real-life black holes Stellar mass Supermassive Speculative stuff (if time)
Chapter 5 Basic properties of light and matter. What can we learn by observing light from distant objects? How do we collect light from distant objects?
Black Holes Dennis O’Malley. How is a Black Hole Created? A giant star (more than 25x the size of the sun) runs out of fuel –The outward pressure of the.
Lecture 18 Black Holes (cont) ASTR 340 Fall 2006 Dennis Papadopoulos.
Chapter 12 Gravitation. Theories of Gravity Newton’s Einstein’s.
Black Holes By Irina Plaks. What is a black hole? A black hole is a region in spacetime where the gravitational field is so strong that nothing, not even.
Black Holes.
Neutron Stars and Black Holes Chapter 14. Formation of Neutron Stars Compact objects more massive than the Chandrasekhar Limit (1.4 M sun ) collapse beyond.
Lecture 6 Black hole (by D.Koo). The evolution of the Universe can be essentially derived using the Newtonian equations. This is due to a peculiarity.
Announcements Observing Monday-Thursday of this week counts on the third exam. Fourth exam is Wednesday, November 17 Review will be Monday, November 15.
Chapter 26 Relativity. General Physics Relativity II Sections 5–7.
SESSION: Black hole SUBMITTED BY: SUBMITTED TO: Dr.A.K.SRIVASTAVA UNDER SUPERVISION OF: SHRI SUSHEEL SINGH M.Sc FINAL Amaresh Singh.
Chapter 13 Black Holes. What do you think? Are black holes just holes in space? What is at the surface of a black hole? What power or force enables black.
Copyright © 2010 Pearson Education, Inc. Neutron Stars and Black Holes Unit 9.
Black Holes. Gravity is not a force – it is the curvature of space-time - Objects try and move in a straight line. When space is curved, they appear to.
A black hole is a region of space with such a strong gravitational field that not even light can escape.
Copyright © 2012 Pearson Education Inc. Orbital motion, final review Physics 7C lecture 18 Thursday December 5, 8:00 AM – 9:20 AM Engineering Hall 1200.
Black Holes This one’s green. I like green.. What happens after a SN? Material remaining after a supernova is 3 times more massive than the sun or more.
Black Holes Formation Spacetime Curved spacetime Event horizon Seeing black holes Demo: 1L Gravity Well - Black Hole.
Lecture 27: Black Holes. Stellar Corpses: white dwarfs white dwarfs  collapsed cores of low-mass stars  supported by electron degeneracy  white dwarf.
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
Black Holes Chapter Twenty-Four. Guiding Questions 1.What are the two central ideas behind Einstein’s special theory of relativity? 2.How do astronomers.
By Katy O’Donohue. Black Holes Black Holes are a region of space from which nothing can escape, including light. Light is made up of massless particles.
Historical SN and their properties Total energy released ~10 54 erg in a few hours.
Black Hole Vacuum Cleaner of the Universe. Formation of Black Hole nuclear fusionnuclear fusion - tends to blow the star's hydrogen outward from the star's.
Black Holes Chapter 14. Review What is the life cycle of a low mass star (
Physics 311 General Relativity Lecture 18: Black holes. The Universe.
Active Galactic Nuclei Chapter 26 Revised Active Galactic Nuclei Come in several varieties; Starburst Nuclei – Nearby normal galaxies with unusually.
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.
It was discovered in the early 1990’s that the pulse period of a millisecond pulsar 500 parsecs from earth varies in a regular way.
Neutron Stars & Black Holes (Chapter 11) APOD. Student Learning Objective Indentify properties of Neutron Stars & Black Holes NASA.
BLACK HOLES National College Iasi. What is a black hole?  A black hole is a region of space from which nothing, not even light, can escape.  It is the.
Announcements Grades for third exam are now available on WebCT Observing this week and next week counts on the third exam. Please print out the observing.
Universe Tenth Edition
A black hole: The ultimate space-time warp Ch. 5.4 A black hole is an accumulation of mass so dense that nothing can escape its gravitational force, not.
Black Holes. Escape Velocity The minimum velocity needed to leave the vicinity of a body without ever being pulled back by the body’s gravity is the escape.
© 2010 Pearson Education, Inc. The Bizarre Stellar Graveyard.
Black Holes A stellar mass black hole accreting material from a companion star 1.
Chapter 14: Chapter 14: Black Holes: Matters of Gravity.
Supernovas Neutron Stars and Black Holes
Black Holes By Katy O’Donohue.
This one’s green. I like green.
Black holes, neutron stars and binary star systems
Neutron Stars and Black Holes
Incredible Shrinking Stars The End States of Stars.
Black Holes.
Black Holes and Neutron Stars
(will not be included in the 1st exam)
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.
Parts, existence of, origin,
Black Holes Escape velocity Event horizon Black hole parameters
Presentation transcript:

Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole

Massive bodies and escape speed

Gravity bends the path of light

A nonrotating black hole has only a “center” and a “surface” The black hole is surrounded by an event horizon which is the sphere from which light cannot escape The distance between the black hole and its event horizon is the Schwarzschild radius (R Sch = 2GM/c 2 ) The center of the black hole is a point of infinite density and zero volume, called a singularity

Event horizon

Gravitational Redshift For photons emitted at event horizon, gravitational redshift is infinite. The observed frequency is zero, i.e. the photons are never observed.

Event Horizon How large is the event horizon for a one solar mass black hole? R S = 2GM/c 2 = 2.95 km How about a ten solar mass black hole?

Mass –As measured by the black hole’s effect on orbiting bodies, such as another star Total electric charge –As measured by the strength of the electric force Spin = angular momentum –How fast the black hole is spinning Three parameters completely describe the structure of a black hole Most properties of matter vanish when matter enters a black hole, such as chemical composition, texture, color, shape, size, distinctions between protons and electrons, etc

Rotating black holes A rotating black hole (one with angular momentum) has an ergosphere around the outside of the event horizon In the ergosphere, space and time themselves are dragged along with the rotation of the black hole

As you fall into to a black hole, you shine a blue flashlight at a friend exterior to the hole, she sees 1.blue light 2.blue light at first, then turning red 3.blue light, then red, then nothing 4.nothing

Black holes evaporate

Seeing Black Holes Observed properties of black holes Gravitational energy Rotating black holes Eddington luminosity Accretion disks Jets

Accretion disk

Accretion disks Disks form because infalling matter has angular momentum. Accretion leads to release of gravitational energy. Inner regions of disks rotate very rapidly – near the speed of light. The luminosity of a black hole is limited by its mass.

Seeing black holes

Observed properties of black holes Luminosity Orientation Jets

Gravitational energy Black holes generate energy from matter falling into them.

Rotating black holes For non-rotating black holes: - event horizon is at the Schwarzschild radius - inner edge of the disk is at 3 Schwarzschild radii For maximally rotating black holes: - event horizon is at ½ Schwarzschild radius - inner edge of the disk is at ½ Schwarzschild radius Schwarzschild radius = 3 km (M/M Sun )

Luminosity Gravitational energy is converted to kinetic energy as particles fall towards BH Efficiency of generators: –Chemical burning < % –Nuclear burning < 1% –Non-rotating black hole = 6% –Rotating black hole = 42%

Eddington Luminosity Limit on the brightness of a black hole

Eddington Luminosity

Black holes shine brightest in X-rays Why?

For the spherical object, the total power radiated = the total luminosity is: L = 4  R 2  T 4 T = temperature  = Stephan-Boltzman constant = 5.67  W/m 2 ·K 4 R = radius Luminosity of a ‘Black Body’ Radiator

Luminosity Law 1 2 If star A is 2 times as hot as star B, and the same radius, then it will be 2 4 = 16 times as luminous.

Black holes shine brightest in X-rays Take BH of one solar mass Event horizon is 3 km or 1/200,000 of Sun’s radius Luminosity can be 30,000 time the Sun’s luminosity

Black holes shine brightest in X-rays 1 2 T A = 6000  5700 K = 30,000,000 K

A object’s color depends on its surface temperature Wavelength of peak radiation: Wien Law max = 2.9 x 10 6 / T(K) [nm]

Electromagnetic spectrum Black holes are so hot that they mainly produce X-rays

Review Questions What are the two facts which caused Einstein to invent the special theory of relativity? What are two key consequences of special relativity for how we observe moving objects? What effect does gravity have on spacetime? How do astronomers search for black holes? How are black holes actually simpler than any other objects in astronomy?

Review Questions What are fundamental versus observed properties of black holes? What is the efficiency of a BH for conversion of matter to energy? What is the maximum luminosity for a BH of a given mass? At what wavelength range do stellar mass black holes produce most of their radiation?