Black Holes Written for Summer Honors 2009. Black Holes Massive stars greater than 10 M  upon collapse compress their cores so much that no pressure.

Slides:



Advertisements
Similar presentations
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 18 – Mass-radius relation for black dwarfs Chandrasekhar limiting mass Comparison.
Advertisements

White Dwarf Stars Low mass stars are unable to reach high enough temperatures to ignite elements heavier than carbon in their core become white dwarfs.
© 2010 Pearson Education, Inc. Chapter 18 The Bizarre Stellar Graveyard.
1 Stellar Remnants White Dwarfs, Neutron Stars & Black Holes These objects normally emit light only due to their very high temperatures. Normally nuclear.
Supernovae and nucleosynthesis of elements > Fe Death of low-mass star: White Dwarf White dwarfs are the remaining cores once fusion stops Electron degeneracy.
End States Read Your Textbook: Foundations of Astronomy
Chapter 18: Relativity and Black Holes
Stellar Deaths II Neutron Stars and Black Holes 17.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Chandrasekar Limit--white dwarfs form with remnant under 1.3 M sun.
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.
Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes
Neutron Stars and Black Holes
The mass of a neutron star cannot exceed about 3 solar masses. If a core remnant is more massive than that, nothing will stop its collapse, and it will.
Black Holes Old ideas for black holes Theory of black holes Real-life black holes Stellar mass Supermassive Speculative stuff (if time)
The Stellar Graveyard.
Question The pressure that prevents the gravitational collapse of white dwarfs is a result of ______.  A) Conservation of energy  B) Conservation of.
Lecture 18 Black Holes (cont) ASTR 340 Fall 2006 Dennis Papadopoulos.
Chapter 15 Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction.
Compact Objects Astronomy 315 Professor Lee Carkner Lecture 15 “How will we see when the sun goes dark?” “We will be forced to grope and feel our way.”
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.
13.3 Black Holes: Gravity’s Ultimate Victory Our Goals for Learning What is a black hole? What would it be like to visit a black hole? Do black holes really.
Goal: To understand gravity Objectives: 1)To understand who discovered what about gravity. 2)To learn about the Universal nature of gravity 3)To explore.
Black Holes Matthew Trimble 10/29/12.
Gravity & orbits. Isaac Newton ( ) developed a mathematical model of Gravity which predicted the elliptical orbits proposed by Kepler Semi-major.
BY: Nathan Schmidt Period: 5 Astronomy. A brief history of black holes About 2 centuries ago John Michel was the first person to suggest that it was possible.
1 Stellar Remnants White Dwarfs, Neutron Stars & Black Holes These objects normally emit light only due to their very high temperatures. Normally nuclear.
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.
Binary star motion demonstration What does the first demo represent? What will happen if I replace one ball with a smaller ball? What does the second model.
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.
Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole.
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.
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.
BLACK HOLES Black holes are thought to form from stars or other massive objects if and when they collapse from their own gravity to form an object whose.
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 (
Black Holes Astrophysics Lesson 14. Learning Objectives To know:-  How to define the event horizon for a black hole.  How to calculate the Schwarzschild.
Physics 311 General Relativity Lecture 18: Black holes. The Universe.
Stellar Corpses and Other Space Oddities
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.
KERR BLACK HOLES Generalized BH description includes spin –Later researchers use it to predict new effects!! Two crucial surfaces –inner surface = horizon.
Chapter 13: Neutron Stars and Black Holes. When a massive star begins its core collapse, the electrons get compressed into the protons to form neutrons.
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
Neutron Stars & Black Holes. Neutron Stars and Black Holes I. Neutron Stars A. Remnant from the collapse of a _________. B. During the core collapse of.
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 and Gravity 1)Type II Supernova 2)Neutron Stars 3)Black Holes 4)More Gravity April 7, 2003
Chapter 15 Stellar Remnants: White Dwarfs, Neutron Stars, and Black Holes Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction.
Black Holes A stellar mass black hole accreting material from a companion star 1.
Black Hole. Special Relativity Einstein’s special theory of relativity has two parts. –All objects moving at constant velocity have the same laws of physics.
Chapter 14: Chapter 14: Black Holes: Matters of Gravity.
 Sun-like star  WHITE DWARF  Huge Star  NEUTRON STAR  Massive Star  BLACK HOLE.
Supernovas Neutron Stars and Black Holes
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.
This one’s green. I like green.
Black holes, neutron stars and binary star systems
Black Holes.
Black Holes Escape velocity Event horizon Black hole parameters
“For thousands more years, the mighty ships tore across the empty wastes of space and finally dived screaming onto the first planet they came across which.
Enormous black holes in galaxies
Presentation transcript:

Black Holes Written for Summer Honors 2009

Black Holes Massive stars greater than 10 M  upon collapse compress their cores so much that no pressure is capable of supporting it – a black hole results A black hole is an “object” (region of space) that has an escape velocity that exceeds the speed of light – hence the name –Using the equation for the escape velocity at an object’s surface, equating it to the speed of light c, and solving for radius R known as the Schwarzschild radius. R s = 2GM/c 2 –where M is the object’s mass, G is the gravitational constant and c is the speed of light. –For the Sun, R s is about 3 km – if the mass of the Sun could be compressed into a radius of 3 km it would become a black hole

The Schwarzschild Radius Karl Schwarzschild did find a simple expression for the size of a black hole – its Schwarzschild radius – and it was exactly the same as the radius derived by the escape velocity approach. It is the radius a body must approach to become a black hole. Once inside the Schwarzchild radius the black hole retains the charge, angular momentum and mass of the original body.

Black Holes Einstein’s general theory of relativity gave a mathematical and physical picture to black holes –Gravity is related to the curvature of space –A black hole is a place where the curvature of space is so extreme that a hole forms –Typical analogy – imagine a water bed with a heavier and heavier object placed on it –This analogy is only approximate and a mathematical treatment is very difficult

The Event Horizon The spherical surface that encompasses the black hole is called the event horizon. (Don’t confuse it with the Schwarzschild radius) –This name expresses the fact that everything within the black hole (any events) are beyond our ability to see (like a ship beyond the horizon) –We are only capable of knowing a black hole’s mass, electric charge, and spin (a spinning black hole will not have a spherical event horizon) –However, the radius of the Event Horizon equals the Schwarzchild radius

The Event Horizon A black hole’s gravitational field is no different than any other object with the same mass (except for their interiors) The curvature of space will bend light and this is indeed observed

Formation of Black Holes Not all astronomers are convinced of the existence of black holes Astronomers are virtually convinced that supernova explosions create neutron holes, and it is only a “small” extrapolation to create black holes However, it remains to be demonstrated by observation that black holes exist A New Zeeland mathematician Roy P. Kerr found a solution from Einstein’s equations that describes a rotating black hole. Such a black hole is called the Kerr Black Hole. The ergosphere is a region outside the event horizon in which space times rotates with the black hole.

General approach to “observing” black holes is an indirect approach – look for an effect on an object that can be uniquely attributed to an interaction with a black hole Observing a Black Hole

A black hole in a closed binary system –An accretion disk may form around the black hole as it draws in material from its companion –Material swirling around at or near the speed of light at the black hole’s event horizon will emit X-rays due to the extreme temperatures

If the black hole is eclipsed by the companion, an x-ray telescope will observe the periodic disappearance of the x-ray signal From the periodicity of the X-rays and the known mass of the companion, the mass of the invisible black hole can be found Observing a Black Hole

If this mass exceeds the maximum allowed for a neutron star (Cygnus X-1 and A are two examples), a black hole is currently the only known object that can have high mass and not be visible (and yet its companion is)

Hawking Radiation In 1974, Steven Hawking predicted that black holes should radiate a blackbody spectrum – Hawking radiation Maximum radiation is at a wavelength 16 times the Schwarzschild radius Using Wien’s law, a solar mass black hole will radiate with a temperature of 6 × K Although this level of radiation is too small to detect, it does imply that black holes are not truly black The basis of Hawking radiation is a quantum process that allows energy to escape the black hole despite its intense gravity The net result: If left alone, a black hole, whose only source of energy is its mass, will eventually “evaporate”, albeit with a very large time scale (10 67 years!)

Picture taken with our Scanning Tunneling Microscope which utilizes quantum tunneling.