The Calculus of Black Holes James Wang Elizabeth Lee Alina Leung Elizabeth Klinger.

Slides:



Advertisements
Similar presentations
F. Debbasch (LERMA-ERGA Université Paris 6) and M. Bustamante, C. Chevalier, Y. Ollivier Statistical Physics and relativistic gravity ( )
Advertisements

Gravitational Potential Energy When we are close to the surface of the Earth we use the constant value of g. If we are at some altitude above the surface.
MAXWELL’S EQUATIONS 1. 2 Maxwell’s Equations in differential form.
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
Chapter 11 – Gravity Lecture 2
Gerard ’t Hooft Dublin November 13, 2007 Utrecht University on.
Compact Objects Astronomy 315 Professor Lee Carkner Lecture 15.
Scott Johnson, John Rossman, Charles Harnden, Rob Schweitzer, Scott Schlef Department of Physics, Bridgewater State College // Bridgewater MA, Mentor:
Chapter 22: Black Holes Einstein’s relativity: –Special –General –Relativity and black holes Evidence of black holes Properties of black holes Long-time.
This set of slides This set of slides continues the late-in-life evolution and death of massive stars, stars > 8 solar masses. It starts with Special and.
Gravity is one of the four fundamental interactions. General Relativity (GR) is the modern interpretation of gravity. GR says gravity is not a force!
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.
PHYS 43, SRJC, Spring ’11: May 12, 2011 Joshua Chen, David Tran, and Eileen O’Byrne- Hudson.
Black Holes Old ideas for black holes Theory of black holes Real-life black holes Stellar mass Supermassive Speculative stuff (if time)
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.
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.
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.
Chapter 26 Relativity. General Physics Relativity II Sections 5–7.
Unit 06 “Circular Motion, Gravitation and Black Holes” “Gravitation and Black Holes”
Black Holes Fred Ikeler Shimon Masaki Danny Okano.
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.
Teaching Black Holes Donald Marolf, UCSB July 20, 2006.
General Relativity and the Expanding Universe Allan Johnston 4/4/06.
Black Holes Formation Spacetime Curved spacetime Event horizon Seeing black holes Demo: 1L Gravity Well - Black Hole.
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 - Observation How do you see something you can’t see ?????
Principle of Equivalence: Einstein 1907 Box stationary in gravity field Box falling freely Box accelerates in empty space Box moves through space at constant.
Flux Capacitor (Schematic)
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 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.
ASTR 1200 Announcements Website Second exam will be October 30. Thursday Review materials were posted.
Physics 55 Monday, December 5, Course evaluations. 2.General relativity with applications to black holes, dark matter, and cosmology. 3.Hubble’s.
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.
The Meaning of Einstein’s Equation*
General Relativity and Cosmology The End of Absolute Space Cosmological Principle Black Holes CBMR and Big Bang.
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.
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.
Energy-Mass Equivalence
Universe Tenth Edition
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.
연세대 특강 What is a Black Hole? Black-Hole Bomb(BHB) Mini Black Holes
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.
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.
The Rotating Black Hole
Black holes, neutron stars and binary star systems
Relativity H7: General relativity.
Black Holes.
GENERAL RELATIVITY General relativity describes the effect of gravitational fields on space and time.
GENERAL RELATIVITY General relativity describes the effect of gravitational fields on space and time.
Parts, existence of, origin,
Black Holes Escape velocity Event horizon Black hole parameters
What is gravity????.
Presentation transcript:

The Calculus of Black Holes James Wang Elizabeth Lee Alina Leung Elizabeth Klinger

What is a Black Hole? A region from which even light cannot escape –Thus the black hole itself cannot be seen –Detected through gravitational distortion of nearby planets and stars, and radiation Has infinite gravitational pull and density

What is the Event Horizon? An area around the singularity of the black hole where no particle can escape its pull No outside influences can affect the particle’s descent towards the black hole

What are Stationary Limits? Stationary limit – area around black hole (outer border) –Particles in area are in constant motion –Rotating black hole (Kerr’s) – distortion of space Doesn’t apply to Schwarzchild black hole – doesn’t rotate Gravity infinitely intense Limit between this and event horizon – ergosphere Limit at which light can escape

Diagram of a Black Hole

Pictures of Black Holes

How are Black Holes Modeled? Black holes create “indentations” in space/time continuum Curvature is the only logical way to model black holes Black holes follow the “no-hair” theorem Only three characteristics distinguishing black holes from one another are mass, angular momentum, and electric charge

Black Holes and Einstein’s General Theory of Relativity Gravity – curved space time –Caused by mass and radius of an object, as well as energy –Strong gravitational field = more curvature –Applies to light – light gets curved –Space affects movement of object –No material object can move faster than speed of light Black hole – area where space time curved so much that objects fall out of the universe –Escape velocity = speed of light Black Holes and Einstein’s Theory of Relativity

Maxwell’s Equations 1st equation: 2 nd equation: Determines total flow of electric charge out from closed surface Cover surface with patches of area of dA (represented as vectors), use dot product to find component of field that points in outward direction (only component that matters) Net magnetic flux is 0 Magnetic flux – product of magnetic field and area it goes through; integral of vector quantity (magnetic force) over surface

Maxwell’s Equations (cont’d) 3rd equation: Line integral – products of vector functions of electric and magnetic field Equation says line integral of electric field around closed loop is equal to negative rate of change of magnetic flux

Maxwell’s Equations (cont’d) 4 th equation: Light was in form of electromagnetic wave

How are Maxwell’s Equations Related to Black Holes? Moving electric field creates magnetic vortex Electromagnetic radiation – from charged particles that move towards black hole Light affected by extremely strong gravity Black hole is large magnetic field b/c electric field created when charge falls into black hole

Using Riemannian Manifolds to Describe Curvature Manifolds describe complex structures of non-Euclidian space within the context of Euclidian space using mathematical equations Riemannian manifolds are real differentiable manifolds that use angles Black holes are mapped into more simple structures using Riemannian manifolds

Equations Modeling Black Hole Curvature The Schwarzschild Metric Equation

Equations Modeling Black Hole Curvature The Schwarzschild Metric Equation (Continued)

Equations for Escape Velocity and Gravitational Force Gravitational Energy would have to equal kinetic energy Force as mass becomes infinite and radius 0

Significance of Change in Radius in Relation to Curvature Curvature is the deviation of an object from being flat A smaller radius has more curvature and vice versa Therefore, black holes with smaller radii have more curvature

Behavior and Emissions of a Black Hole Electromagnetic radiation comes from charged particles that move towards black hole Black hole is large magnetic field b/c electric field created when charge falls into black hole

Photon and Gamma Particle Radiation from Black Holes Black holes emit thermal radiation at temperature – = reduced Planck constant c = speed of light K = Boltzmann constant G = gravitational constant M = mass of black hole Unlike most objects, the temperature of a black hole increases as it radiates away mass

Gravitational Force Considerations Black holes become impossible to escape as it approaches the event horizon as the escape velocity required, regardless of mass, equals the speed of light Relativity, as c is constant, in order for energy to increase towards infinite, mass = infinite

Bibliography Andersen, Michael C. "Einstein's Field Equations and Black Holes." Niels Bohr Institute. 14 June Niels Bohr Institute. 14 May Ando, David. "An Introduction to Black Holes." 7 May Cumberlidge, Anne-Marie. "Everything You Need to Know About Black Holes." The Hitch- Hiker's Guide to Black Holes Keele University. 5 May "Curvature." Wikipedia. 7 May 2006.

Bibliography continued Darling, David. "Euclidean Space." The Encyclopedia of Astrobiology Astronomy and Spaceflight. 12 May Darling, David. "Non-Euclidean Geometry." The Encyclopedia of Astrobiology Astronomy and Spaceflight. 12 May "Escape Velocity." Wikipedia. 7 May "Euclidean Geometry." Wikipedia. 11 May Fowler, Michael. "Maxwell's Equations and Electromagnetic Waves." Physics Dept., University of Virginia. 10 May 2006.

Bibliography continued "Isomorphism." Wikipedia. 15 May Johnston, Robert. "Black Holes." Relativistic Physics. 14 Oct May Kobes, Randy, and Gabot Kunstatter. "Gravity as Curved Space: Einstein's Theory of General Relativity." Physics Modern Technology. 29 Sept University of Winnipeg. 9 May "Manifold." Wikipedia. 15 May "Maxwell's Equations in Curved Spacetime." Wikipedia. Apr May Nave, C.r. "Maxwell's Equations." HyperPhysics Georgia State University. 9 May 2006.

Bibliography continued "Q & a: Black Holes." Chandra X-Ray Observatory. 2 Aug Harvard University. 6 May "Radius of Curvature." Wikipedia. 17 May "Riemannian Manifold." Wikipedia. 12 May Salgado, Rob. "The Light Cone: the Schwarzchild Black Hole." Syracuse University. 7 May Seeds, Michael A. Horizons: Exploring the Universe. 7th ed. Pacific Grove, CA: Brooks/Cole, 2002.

Bibliography continued Smith, Gene E. "General Relativity & Black Holes." Gene Smith's Astronomy Tutorial. 9 Mar University of California San Diego. 17 May "The Mystery of Black Holes." Knowing the Universe and Its Secrets. 7 Feb May Weisstein, Eric W. "Neighborhood." MathWorld. 12 May Wyatt, Ryan, and Rachel Connolly. "From Einstein to Hawking Course Outline." 28 Apr American Museum of Natural History. 10 May 2006.