Stellar remnants II. Neutron Stars 10/18/2010. (progenitor star 1.4 < M< 3 Msun) Stars, Galaxies & the Universe Announcements

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Stars, Galaxies & the Universe Announcements Exam #2 on Wednesday Review sheet and study guide posted by Thursday Use office hours and Astronomy Tutorial hours Covers material since Exam #1 (plus background material) 1 Stars, Galaxies & the Universe Lecture Outline 1. Neutron Stars - properties of neutron stars - pulsars 2. Black holes - Einstein s view of gravity - Properties of black holes 2 Stellar remnants II Neutron Stars (progenitor star 1.4 < M< 3 Msun) 3 1

Life of a High Mass Star (25 Mo) LT MS: 5 million years LT P-MS: <1 million years blue main sequence (CNO cycle of hydrogen burning) Red supergiant He-burning supergiant Multiple shell supergiant (all the way to Iron core) collapse of star onto inert iron core supernova explosion neutron star/black hole 4 and supernova remnant Neutron Stars - Forming Degenerate stars heavier than 1.4 solar masses collapse to become neutron stars Formed in supernova explosions Electrons are not separate Combine with nuclei to form neutrons Neutron stars are degenerate gas of neutrons (White dwarfs were an electron degenerate gas) 5 Neutron Stars - Properties Very compact about 10-15 km radius Very dense one teaspoon of neutron star material weighs as much as all the buildings in Manhattan Spin rapidly as fast as 600 times per second High magnetic fields compressed from magnetic field of progenitor star 6 2

one teaspoon full 1 billion tons surface gravitational field 300,000 times that of Earth normal laws of physics start to break down (Monday!) in order for an object to escape from a neutron star, it would have to be traveling at 1/2 the speed of light! 7 20 15 Mass v Radius 10 5 8 Theoretical Properties of Neutron Stars must rotate rapidly because of their small sizes Star like the Sun takes about a month to rotate on its own axis if the Sun were collapsed to the size of a neutron star, it would rotate 10000x per second! artist s conception of a rotating neutron star 9 3

Collapse of star increases both spin and magnetic field Spinning of neutron star artist s conception of a rotating neutron star 10 Theoretical Properties of Neutron Stars MUST BE STRONGLY MAGNETIC with a radius=15 km, Sun s magnetic field would be 10 10 x as strong! Magnetic field for regular star: a few Gauss (G) Strongest magnetic field produced in a laboratory (for a few sec): 10 6 G Magnetic field for neutron star: 10 15 G theoretical cartoon of an object with a strong magnetic field 11 Neutron star and black hole formation (History channel video) http://www.youtube.com/watch?v=jt2wkbpfuyc 12 4

How do we detect neutron stars? neutron stars are very very small (10-15 km) even though very hot, no direct detection! 1.Pulsars radio detections of pulsing signals spinning radio beams pointed toward us 2. X-ray binaries 2 stars in orbit 1. main sequence/giant/supergiant 2. neutron star big star loses mass onto neutron star explosions on surface, X-ray emission 13 The discovery of pulsars proved neutron stars exist 1967: Jocelyn Bell student of Anthony Hewish at Cambridge U., England Built a radio telescope to study variations in the solar wind by looking at twinkling of radio sources as they pass through h the solar wind/corona Jocelyn Bell discovered a regular radio signal every ~ 1 second Thought it could be detection of ET LGM1 14 Pulsations were much more rapid than any known type of astronomical object one of the most plausible ideas was a rotating white dwarf s hot spot but only if pulses were approximately every 1 second otherwise the white dwarf would fly apart Soon many of these sources were detected and called pulsars Their periods range from 0.25 to 1.5 seconds But still their relationship to supernovae/neutron stars unknown PSR 0329+54 Interval between pulses=0.714 seconds 15 5

Major clue to nature of pulsars occurred when a pulsar was discovered at the heart of the Crab Nebula Period of this pulsar: 0.0333 seconds or rotations 30x a second! could not be a white dwarf Had to be an even more compact object: a neutron star! Pulsar sounds webpage 16 Unusual physics near the surface of a pulsar creates radiation due to strong magnetic fields due to intense rotation intense electric field set up near surface, where electrons can be made through pair production 17 BEAMS of radio emission originate close to poles - electrons made through pair production interact with strong magnetic fields - generate SYNCHROTRON radiation at radio (X-ray,optical) wavelengths - we observe pulses as the neutron star spins, bringing beam into our sight line 18 6

Observational Properties of PULSARS Observations of pulsars confirmed theoretical ideas In order to explain pulses Neutron stars emit radio emission from their poles 2. The BEAM must be directed toward us in order to detect it Because they are spinning so fast (1-1000x/s) we see pulses Two Nobel prizes came out of pulsars: 1. Hewish (1967) first discovery of pulsed signals (really the work of Jocelyn Bell) 2. Taylor & Hulse (1993) discovery of a pulsar binary! 19 20 21 7

Pulsars also lose energy over time into the ISM 22 X-ray movie showing material flowing outwards into Pulsar Wind Nebula 23 Life of a Solar Mass Star (Low-Mass) LT MS: 10 billion years LT P-MS: 1 billion years main sequence red giant: shell Hydrogen burning He-burning star (horizontal branch) Helium shell burning & Hydrogen shell burning (double shell burning) planetary nebula white dwarf 24 8

Life of a High Mass Star (25 Mo) LT MS: 5 million years LT P-MS: <1 million years blue main sequence (CNO cycle of hydrogen burning) Red supergiant He-burning supergiant Multiple shell supergiant (all the way to Iron core) collapse of star onto inert iron core supernova explosion neutron star/black hole 25 and supernova remnant Are all pulsars neutron stars? Are all neutron stars pulsars? Black Holes!! 26 In Einstein s picture, TIME becomes another coordinate of space SPACETIME (x,y,z,t) 27 9

Einstein s theory of General Relativity Einstein revised Newton s ideas on gravity in hopes of putting together a GENERAL theory of all physics; major implications were in regards to gravity, however 28 Newton s Theory of Universal Gravitation every pair of objects exerts a gravitational force on each other strength of force depends on MASS of each object DISTANCE between two objects 29 NEWTON vs. EINSTEIN View of Gravitational Force Newton Einstein Einstein s theory much more robust than Newton s 4 experiments that Newton s view fails to explain 30 10

Newton s Theory of General Relativity - Gravity all objects feel the same curvature or well this explains why different objects feel same gravity This is why things don t get SUCKED into a black hole unless you are really close to a BH, you don t feel the curvature (e.g. for a 10 solar mass BH, you will only be affected within 1000 km) 31 Einstein s Theory of General Relativity massive objects affect the SPACE and TIME around them warping of space-time the stronger the gravity, the more spacetime is CURVED Light can even be deflected from its original path (something Newton s laws don t predict b/c light is massless)! 32 Experimental Test #1 of Einstein s Theory of General Relativity: gravitational bending of light - light rays travel in straight lines - in the presence of mass, the straight line is bent - happening all the time, but difficult to observe - even happens when light from stars near Sun passes by Sun observe coordinates of stars very close to the Sun during eclipse compare these to their positions when they are not close to the Sun (in a different part of space) find that their positions have changed due to the light being bent around the Sun very SMALL! 33 11

Experimental Test #2 of Einstein s Theory of General Relativity: precession of Mercury s orbit - the orbit of Mercury changes orientation with respect to Sun - due to the gravitational pull of all the planets measure Mercury s changing orbit figure out how much the rest of the planets affect the orbit leftover amount of change MUST be due to a gravitational correction from the proximity of the Sun! 34 Experimental Test #3 of Einstein s Theory: Gravitational redshift & time dilation - mass warps time and space - clocks on the ground floor of a building should tick more slowly - light will become redder (longer wavelength) and lose energy as it travels up from ground floor because time slows down - VERY tiny effects not measurable but important - this is DIFFERENT than the Doppler effect (no motion)! 35 Experimental Test #4 of Einstein s Theory: Gravitational waves! - like EM radiation waves, but due to oscillating massive objects - much less powerful, but trace a whole new spectrum 36 12

Sources of gravitational radiation: binary pulsars! two neutron stars in a tight (small) binary system will lose gravitational energy as they orbit each other 2 neutron stars in a binary system Taylor & Hulse: Nobel Prize (1993) for detecting the shrinking of an orbit of a binary pulsar system 37 Testing the theory of General Relativity: LIGO Laser Interferometer Gravitational wave Observatory attempting to detect gravitational waves one site: eastern Washington state other site: Louisiana 38 Black Holes are a natural consequence of Einstein s theory of gravity 39 13

A black hole has only a center and a surface The black hole is surrounded by an event horizon which is the sphere for which light cannot escape surface 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 or center A black hole is TRULY black! 40 What would a journey into a Black Hole be like? 41 Schwarzchild radius (R sh ): the radius at which an object MUST be a black hole the radius at which density is so great, no light escapes depends on the mass of an object larger mass, larger R Object Mass R sh ------------ ---------- -------- massive star 10 M o 30 km mid-mass star 3 M o 9 km Sun-like star 1 M o 3 km Earth 3x10-6 M o 9 mm person ~60 kg (3x10-29 M o ) 10-28 m 42 14

Falling into a black hole: get stretched along axis parallel to the path of motion get stretched VERY severely in one direction, squeezed in the other direction: spaghetti-fication from observer s point of view, appear redder (gravitational redshift) because TIME slows, then you would appear to never really get there to an observer! 43 What would happen if you observed me fall into a black hole??? I would start to fall slowly because time appears to slow down due to the high gravity I would also appear to contract into a thin strand by tidal forces I would hover at the event horizon forever from the observer s perspective sketch I would be shredded and stretched from my perspective (unpleasant!) 44 15