170 likes | 303 Views
Extraordinary Concepts in Physics. Lecture 4. Trip to a Black Hole I. by Robert J. Nemiroff Michigan Tech. Physics X: About This Course. Officially "Extraordinary Concepts in Physics" Being taught for credit at Michigan Tech Light on math, heavy on concepts Anyone anywhere is welcome
E N D
Extraordinary Concepts in Physics Lecture 4 Trip to a Black Hole I by Robert J. Nemiroff Michigan Tech
Physics X: About This Course • Officially "Extraordinary Concepts in Physics" • Being taught for credit at Michigan Tech • Light on math, heavy on concepts • Anyone anywhere is welcome • No textbook required • Wikipedia, web links, and lectures only • Find all the lectures with Google at: • "Starship Asterisk" then "Physics X" • http://bb.nightskylive.net/asterisk/viewforum.php?f=39
Trip to a Black Hole: Overview • Schwarzschild black hole only • It's the easiest • It's what I know best • Based partly on my paper: • "Visual distortions near a neutron star and black hole" • American Journal of Physics 1993, 61, 619 • And my web page: • Virtual Trips to Black Holes and Neutron Stars
Trip to a Black Hole: Key Distances • r = infinity: space is flat: aN = GM/r2 • Near the black hole: a = aN / (1 - rs/r)1/2 • r = 3 rs: last stable orbit • r = 1.5 rs: photon sphere • r = rs: event horizon • r = rc: Compton radius • r = 0: GR singularity
Trip to a Black Hole: Far Away • r -> infinity: space is "flat" • all (1 - rs/r) terms go to 1. • gravity is Newtonian: aN = GM/r2 • black holes attract the same as normal matter • curved universe NOT flat as r -> infinity • can see lensing effects with a telescope • orbiting the same as spinning in place
Trip to a Black Hole: Approaching • black hole appears black • excludes evaporation effects • blackness everywhere inside photon sphere • cannot see to the event horizon • outside, average surface brightness unchanged • appears fuzzy as star images merge • distant universe • speeds up • appears bluer
Background: Gravitational Lensing • gravity bends light: "null geodesics"
Gravitational Lensing:Einstein Ring • Actual Einstein ring: APOD 2008 July 28
Gravitational Lensing:Einstein Ring • Detailed image of Einstein ring from AJP paper
Trip to a Black Hole: Orbiting at 10 rs • Stars CANNOT cross the Einstein ring • Einstein ring mapped point behind BH center • Einstein ring divides complete image sets • Angular speeds diverge at the Einstein ring • One can see oneself • All stars have two discernible images • One outside the ER, one inside • Observers also have two images • Actually, an infinite number of images exist
Trip to a Black Hole: Orbiting at 10 rs • Distant stars appear slightly bluer • Distant clocks appear to run faster • This also occurs for stars that appear next to the black hole • Objects ACTUALLY nearer to the black hole • Appear redder • Clocks appear to run slower
Trip to a Black Hole: Orbiting at the Photon Sphere • Everything below you is black • because those light paths fall into the BH • The whole sky appear above you • because those light paths escape the BH • The Einstein ring appears above the horizon • Stars still CANNOT cross the Einstein ring • Stars still speed up near the Einstein ring
Trip to a Black Hole: Orbiting at the Photon Sphere • Other image sets between other Einstein rings • "The" Einstein ring actually "First Sky Einstein ring" • There are infinitely many Sky Einstein rings • Every radius from the BH has • its own infinite set of Einstein rings • its own redshift (or blueshift)
Gravitational Lensing:Einstein Ring • Einstein rings near a black hole