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.

Slides:



Advertisements
Similar presentations
Trip to a Black Hole I by Robert J. Nemiroff Michigan Tech
Advertisements

Black Holes. Dark stars a star that has an escape velocity greater than the speed of light.
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.
Pulsars A pulsar is a neutron star that beams radiation along a magnetic axis that is not aligned with the rotation axis.
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.
Neutron Stars and Black Holes
Black Holes - Chapter 22.
Scott Johnson, John Rossman, Charles Harnden, Rob Schweitzer, Scott Schlef Department of Physics, Bridgewater State College // Bridgewater MA, Mentor:
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.
Question The pressure that prevents the gravitational collapse of white dwarfs is a result of ______.  A) Conservation of energy  B) Conservation of.
1 Announcements There will be a star map on the exam. I will not tell you in advance what month. Grades are not yet posted, sorry. They will be posted.
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.
Black Holes.
Announcements Exam 4 is Monday May 4. Tentatively will cover Chapters 9, 10, 11 & 12 Sample questions will be posted soon Observing Night tomorrow night.
Special Relativity Speed of light is constant Time dilation Simultaneity Length Contraction Spacetime diagrams.
Stationary Elevator with gravity: Ball is accelerated down.
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.
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.
Bending Time Physics 201 Lecture 11. In relativity, perception is not reality Gravity affects the way we perceive distant events For example, although.
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.
Principle of Equivalence: Einstein 1907 Box stationary in gravity field Box falling freely Box accelerates in empty space Box moves through space at constant.
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 (
Pulsars, Neutron Stars and Black Holes Model of a Neutron Star.
Physics 311 General Relativity Lecture 18: Black holes. The Universe.
Astronomy 1020 Stellar Astronomy Spring_2015 Day-37.
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.
General Relativity and Cosmology The End of Absolute Space Cosmological Principle Black Holes CBMR and Big Bang.
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.
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.
Universe Tenth Edition
ASTR 113 – 003 Spring 2006 Lecture 08 March 22, 2006 Review (Ch4-5): the Foundation Galaxy (Ch 25-27) Cosmology (Ch28-29) Introduction To Modern Astronomy.
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.
Black Holes and Gravity 1)Type II Supernova 2)Neutron Stars 3)Black Holes 4)More Gravity April 7, 2003
Astronomy 1020 Stellar Astronomy Spring_2016 Day-34.
Black Holes A stellar mass black hole accreting material from a companion star 1.
Chapter 14: Chapter 14: Black Holes: Matters of Gravity.
18 October 2001Astronomy 102, Fall Today in Astronomy 102: “real” black holes, as formed in the collapse of massive, dead stars  Formation of a.
A neutron star over the Sandias?
Exam Monday Covers reading and related notes from chapters
The Rotating Black Hole
This one’s green. I like green.
Relativity H7: General relativity.
Black Holes.
Black Holes and Neutron Stars
Special Relativity Speed of light is constant Time dilation
Special Relativity Speed of light is constant Time dilation
Exam 3 average: 65%. You will have all of class time on Thursday to do the group review. The response “Exams” will be on Learning Suite by Wed noon. They.
Parts, existence of, origin,
Black Holes Escape velocity Event horizon Black hole parameters
Special Relativity Speed of light is constant Time dilation
Presentation transcript:

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 page from the web site before going observing.

Black Holes Formation Spacetime Curved spacetime Event horizon Seeing black holes Reading 20.3

Mass versus radius for a neutron star Objects too heavy to be neutron stars collapse to black holes

Speed of light is constant

Our conceptions of space and time has to be changed. Facts: Regardless of speed or direction, observers always measure the speed of light to be the same value. Speed of light is maximum possible speed. Consequences: –The length of an object decreases as its speed increases –Clocks passing by you run more slowly than do clocks at rest

Special Relativity: Length Contraction

Spacetime Diagram

Geodesic = shortest path between two points. Particles follow geodesics in spacetime.

Gravity deforms space-time

Geodesics in curved spacetime

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

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 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

Falling into a black hole Falling into a black hole gravitational tidal forces pull spacetime in such a way that time becomes infinitely long (as viewed by distant observer). The falling observer sees ordinary free fall in a finite time.

Falling into a black holes With a sufficiently large black hole, a freely falling observer would pass right through the event horizon in a finite time, would be not feel the event horizon. A distant observer watching the freely falling observer would never see her fall through the event horizon (takes an infinite time). Falling into smaller black hole, the freely falling observer would be ripped apart by tidal effects.

Falling into a black hole Signals sent from the freely falling observer would be time dilated and redshifted. Once inside the event horizon, no communication with the universe outside the event horizon is possible. But incoming signals from external world can enter. A black hole of mass M has exactly the same gravitational field as an ordinary mass M at large distances.

Seeing black holes

Black holes evaporate