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1 Lecture 31 Stellar Remnants January 14c, 2014 2 Neutron Stars • • • • • Supernova remnant Tightly packed neutron core. Size ~ 20 km (small asteroid or medium city) Mass ~ 1.4 - 3 M Density very high – 1 tsp. (5 ml) weighs > 100,000,000 tons on Earth! • Rotates many times per second due to conservation of angular momentum; any rotating body spins faster when it shrinks. 3 • Powerful magnetic field, a trillion times stronger than the Earth’s Neutron Stars – When star collapses, magnetic field is concentrated. Artist rendering showing a neutron star is about the size of lower Manhattan Figure 22.1, Chaisson and McMillan, 5th ed. Astronomy Today, © 2005 Pearson Prentice Hall 4 Where would a neutron star be found on an H-R diagram? A. B. C. D. E. F. G. H. Region A Region B Region C Region D Region E Region F Region G Region H 5 Where would a neutron star be found on an H-R diagram? A. B. C. D. E. F. G. H. Region A Region B Region C Region D Region E Region F Region G Region H Neutron stars are hot and very tiny so they’d be found near region F on an H-R diagram. 6 Neutron Star -- HST 7 Pulsars • 1967 Jocelyn Bell – Observed object emitting pulses of radio waves. – Pulses repeated every 1.34 seconds 8 Pulsars • Hundreds more have been found. • Some pulse in optical, X-rays, or gamma rays. • Periods range from 0.03 to 0.30 sec. Periods gradually increase as pulsar loses energy and rotates slower • Some are associated with supernova remnants, many apparently not… hurled into space at high speed by the supernova explosion. 9 • Hewitt proposed it is a rapidly rotating neutron star beaming radiation. – Magnetic pole and rotational axis not quite lined up. – Charged particles at poles of magnetic fields emit large amounts of energy. Figure 22.3, Chaisson and McMillan, 5th ed. Astronomy Today, © 2005 Pearson Prentice Hall Pulsars “Lighthouse Model” 10 • Not all neutron stars are seen to pulse – Beam may not be pointed at the Earth – animation – Older neutron stars have lost energy and no longer pulse Earth never sees beam of energy Earth Earth sees beam of energy Earth 11 Crab Nebula Figure 21.10, Chaisson and McMillan, 6th ed. Astronomy Today, © 2008 Pearson Prentice Hall 12 Crab Pulsar The pulsar must be young because it is seen at visible and X-ray wavelengths. Old pulsars emit mostly at lower energy radio wavelengths. animation Figure 22.4, Chaisson and McMillan, 6th ed. Astronomy Today, © 2008 Pearson Prentice Hall and Figure 13-19b, Comins and Kaufmann, 8th ed. Discovering the Universe, © 2008 W.H. Freeman & Co. 13 What causes the radio pulses of a pulsar? A. The star vibrates. B. We observe pulses when one of the beams of radio radiation emitted by the spinning star points toward Earth. C. The star undergoes periodic nuclear explosions that generate radio emission. D. The star’s dark orbiting companion periodically eclipses the radio waves emitted by the main star. E. A black hole near the star absorbs energy from it and re-emits it as radio pulses. 14 What causes the radio pulses of a pulsar? A. The star vibrates. B. We observe pulses when one of the beams of radio radiation emitted by the spinning star points toward Earth. C. The star undergoes periodic nuclear explosions that generate radio emission. D. The star’s dark orbiting companion periodically eclipses the radio waves emitted by the main star. E. A black hole near the star absorbs energy from it and re-emits it as radio pulses. 15 Einstein’s Special Theory of Relativity • You cannot determine if a frame of reference is at rest or moving at constant velocity • All observers measure the same speed of light in vacuum • The distances and times between events depend upon your frame of reference • Length contraction and time dilation • Time and space are linked together in a single “fabric” called spacetime 16 Einstein’s General Theory of Relativity • You cannot determine if a frame of reference is accelerating or immersed in a uniform gravitational field • Space and time are affected by large masses 17 General Relativity • All matter warps spacetime. – Like a weight on a rubber sheet. – Warped spacetime affects the behavior of BOTH objects and light in its vicinity. Analogy: a rolling pool ball on an uneven surface is deflected in much the same way as a planet’s curved orbit is determined by warped spacetime near the Sun. Figure 22.18b, Chaisson and McMillan, 6th ed. Astronomy Today, © 2008 Pearson Prentice Hall 18 Evidence for General Relativity • On May 29, 1919 Arthur Eddington carefully measured star positions around the eclipsed Sun. Precession of Mercury’s orbit, and that of a neutron star binary system, offered further confirming evidence in support of General Relativity 19 Formation of Black Holes • If core of star has M >3 M the neutron pressure cannot hold up the core – Nothing remains to stop collapse. – Becomes a “singularity” -- object with infinite density and infinitely small size. – Rips a hole in the fabric of spacetime 20 Why are Black Holes Black? • Escape velocity = velocity needed to escape the gravitational pull of an object. vescape 2GM 11 km/s for Earth R • As mass increases or size decreases, gravity on the surface of the star increases, and a larger velocity is needed to escape surface. • When the escape velocity at the surface becomes greater than the speed of light, no light can escape. 21 Schwarzschild Radius Distance from the center of a supermassive object at which the escape velocity would be equal to the speed of light. Normal star: Light can escape surface (vescape < c) Black Hole: Light cannot escape surface (vescape > c) Radius > Schwarzschild Radius Radius Schwarzschild Radius 22 Event Horizon • The event horizon of a black hole is one Schwarzschild Radius away from its center. – No events or communication inside the event horizon can be observed. Event Horizon Light cannot escape Black Hole Light can escape 23 Evidence for Black Holes Isolated black holes are hard to observe, but we might be able to detect gravitational lensing. Figure 23.23, Chaisson and McMillan, 6th ed. Astronomy Today, © 2008 Pearson Prentice Hall 24 Evidence for Black Holes • We can observe how the black hole’s gravity affects nearby objects. – Unseen companion – Accretion disk – X-ray emission Figure 14-15, Comins and Kaufmann, 8th ed. Discovering the Universe, © 2008 W.H. Freeman & Co. 25 Cygnus X-1 • A flickering X-ray source that must be smaller than the Earth • The X-ray source seems to force the nearby supergiant star to wobble • Conclusion: It’s a 30-solar-mass B0 supergiant and an 11solar-mass black hole that are orbiting each other Figure 22.23, Chaisson and McMillan, 6th ed. Astronomy Today, © 2008 Pearson Prentice Hall 26 Black Holes in Galaxies • BHs may have formed in center when galaxy formed. • Mass of billions of stars in size of SS (Kepler’s 3rd Law). • Black hole likely in center of the Milky Way. Accretion disk surrounding a 300-million-solarmass black hole in the galaxy NGC 7052. 27 The Schwarzschild radius of a body is A. the distance from its center at which nuclear fusion ceases. B. the distance from its surface at which an orbiting companion will be broken apart. C. the maximum radius a white dwarf can have before it collapses. D. the maximum radius a neutron star can have before it collapses. E. the radius of a body at which its escape velocity equals the speed of light. 28 The Schwarzschild radius of a body is A. the distance from its center at which nuclear fusion ceases. B. the distance from its surface at which an orbiting companion will be broken apart. C. the maximum radius a white dwarf can have before it collapses. D. the maximum radius a neutron star can have before it collapses. E. the radius of a body at which its escape velocity equals the speed of light. 29 Traveling into a Black Hole -Tidal Forces • Extremely large tidal forces near a BH. • Difference in forces of gravity on near and far side would pull object apart. 30 Time Dilation • From outside, observer sees clock on board tick more and more slowly than outside of craft. • The closer to black hole, the slower time appears to run. • At event horizon, time appears to stop! – An observer far away never sees the craft fall into BH – An observer inside the craft sees time proceed at its normal rate. 31 Inside of a Black Hole • Scientists to not know for sure what is inside of a black hole. • Theories of physics break down for such high densities. • Hard to make and test new model since black holes cannot be directly observed.