* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Chapter 13: Neutron Stars and Black Holes - Otto
Magnetic circular dichroism wikipedia , lookup
Gravitational wave wikipedia , lookup
Main sequence wikipedia , lookup
Nuclear drip line wikipedia , lookup
Accretion disk wikipedia , lookup
Gravitational lens wikipedia , lookup
Kerr metric wikipedia , lookup
Astronomical spectroscopy wikipedia , lookup
Hawking radiation wikipedia , lookup
Astrophysical X-ray source wikipedia , lookup
Stellar evolution wikipedia , lookup
Chapter 13 Neutron Stars and Black Holes Optical, Infrared and X-ray Image of Cassiopeia A Neutron Stars • Type I supernovae - star destroyed • Type II supernovae (core collapse) - part of core could survive • Ball of neutrons remain - neutron star • 20 km or so across (size of major city) • Mass greater than sun • Density 1017 to 1018 kg/m3 • Thimbleful would weigh 100 million tons • 150 lb human on surface would weigh 1 million tons Figure 13.1 Neutron Star Rotation and Magnetism • Newly formed neutron star rotates rapidly • Period of fraction of a second • Strong magnetic field • Trillions of times stronger than earth’s • Collapsing core concentrates magnetic field of original star Predicted by theory • Neutron stars (and black holes) predicted by theory before discovered • Fast rotation and strong magnetic fields allowed them to be detected Pulsars • Graduate student Jocelyn Bell at Cambridge University discovered rapid radio pulses in 1967 • More than 1500 now known, as pulsars • Bell’s thesis advisor, Anthony Hewish, reasoned it was a small rotating source of radiation Figure 13.2 Pulsar Radiation Pulsar explanation • Accelerated charged particles near magnetic poles of neutron star • Emit radiation along magnetic axis • Rotation and magnetic axes not aligned • Beam sweeps through space lighthouse model Figure 13.3 Pulsar Model Analogy 13.1 A lighthouse beacon Figure 13.4 Crab Pulsar Pulsar radiation • Most pulsars emit radio wavelengths • Some emit visible, X- and gamma-rays Figure 13.5 Gamma-Ray Pulsars Pulsars and Neutron stars • All pulsars are neutron stars • Not all neutron stars are pulsars: • Must be aligned just right to be visible from earth • Lose rapid rotation and magnetic field over tens of millions of years Figure 13.6 Isolated Neutron Star Neutron star binaries • Some neutron star binaries • Can measure mass - close to 1.4 M X-ray bursters • Neutron star tears matter from surface of binary companion • Accretion disk heats up - emits X-rays • Heats enough to fuse H - rapid burst of burning • Similar to nova, but much more violent Figure 13.7 X-Ray Burster Millisecond pulsars • Spin hundreds of times per second • Period is several milliseconds • Mass of sun, several km in size, spinning almost 1000 times per second • Many are old (and should be slow) • Are spun-up by infalling matter from binary companion Figure 13.8 Millisecond Pulsar Figure 13.9 Cluster X-Ray Binaries Pulsar planets • Several millisecond pulsars have variations in their periods • Explained by Doppler shift due to interaction with orbiting planets • Planets captured or formed from debris of companion star Gamma-Ray bursts • Gamma-rays are very high energy photons • Bursts first discovered in 1960’s by military satellites • Made public in 1970’s • Bright irregular bursts lasting few seconds • Compton Gamma-Ray Observatory - CGRO Figure 13.10 Gamma-Ray Bursts Gamma-Ray burst distances • Some optical counterparts measured • Distances of billions of parsecs • If energy emitted in all directions, then hundreds of times more energetic than supernovae, all in seconds Figure 13.11 Gamma-Ray Burst Counterpart Gamma-Ray burst explanation • • • • millisecond variation in intensity Light travels 300 km in 1 millisecond Must be small Relativistic fireball - gases traveling at speeds approaching speed of light • Probably jets Two GRB models • Merging stars - binary pair of neutron stars merge • Hypernova - collapsing star forming black hole • High temperature accretion disk in both cases • Relativistic outflow, perhaps in jets Figure 13.12 Gamma-Ray Burst Models Figure 13.13 Hypernova? Gravity waves • Predicted by Einstein’s theory of gravity • Very difficult to detect - wave amplitude smaller than atomic nucleus • Most likely candidates: • Merger of binary stars • Collapse of star into a black hole Discovery 13.1 Gravity Waves—A New Window on the Universe Black holes • Neutron stars can exist up to about 3 M • Above that, even tightly packed neutrons can’t prevent further gravitational collapse • Any main-sequence star above 25 M will collapse beyond neutron star • Gravity so great not even light escapes Two key facts from Einstein’s Relativity • Nothing can travel faster than the speed of light, 300,000 km/s • Even light is attracted by gravity Escape speed • How fast do you have to toss an object upward so that it never falls back? • 11 km/s ignoring the atmosphere • Depends on mass and radius of earth • If crushed earth to 1 cm radius, escape speed would be 300,000 km/s so not even light would escape - black hole Schwarzschild radius • Radius for a given mass at which escape speed is speed of light • 1 cm for mass of earth • 3 km for mass of sun • 9 km for 3 M stellar core • Surface of sphere of this radius is called event horizon Figure 13.14 Speed of Light More Precisely 13-1.1 Special Relativity More Precisely 13-1.2 Special Relativity Figure 13.15 Einstein’s Elevator Gravity and Curved Space • General relativity predicts gravity curves or warps space • Objects follow curvature of space • At black hole, curvature so great that space folds over and closes off • Can picture as a rubber sheet Figure 13.16 Curved Space Figure 13.17 Space Warping Tests of General Relativity • Deflection of starlight by gravity • Observable during solar eclipse • Planetary orbits should deviate from ellipses • Greatest for Mercury More Precisely 13-2.1 Tests of General Relativity More Precisely 13-2.2 Tests of General Relativity Space travel near a black hole • Beyond event horizon, objects orbit normally, and can escape • Once inside event horizon, no escape • Tidal forces very strong • Objects ripped and stretched apart into pieces • Frictional heating Figure 13.18 Black Hole Heating Figure 13.19 Robot-Astronaut Robot probe with clock and light source • As probe approaches event horizon, light from it more redshifted • Gravitational redshift • Redshift becomes infinite at event horizon • Robot’s clock slows down as approaches event horizon - time dilation Figure 13.20 Gravitational Redshift Singularity • General relativity predicts collapse to a point with infinite density - a singularity • Probably incomplete theory • Quantum gravity in future might properly explain Black hole observational evidence • Black holes in binary systems • Large black holes at centers of galaxies (more in later chapters) • Intermediate size black holes forming from tight clusters Figure 13.21 Cygnus X-1 - likely black hole Figure 13.22 Black Hole Figure 13.23 Intermediate-Mass Black Holes?