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1 Lecture 31 Stellar Remnants January 14c, 2014

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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.

  • Neutron Stars

    3

    • Powerful magnetic field, a trillion times stronger

    than the Earth’s

    – 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

    A. Region A

    B. Region B

    C. Region C

    D. Region D

    E. Region E

    F. Region F

    G. Region G

    H. Region H

    Where would a neutron star be found

    on an H-R diagram?

  • 5

    A. Region A

    B. Region B

    C. Region C

    D. Region D

    E. Region E

    F. Region F

    G. Region G

    H. Region H

    Where would a neutron star be found

    on an H-R diagram?

    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

    • 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.

    Pulsars

  • 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.

    “Lighthouse Model”

    Pulsars

    Figure 22.3, Chaisson and McMillan, 5th ed.

    Astronomy Today, © 2005 Pearson Prentice Hall

  • 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 Earth never sees

    beam of energy

    Earth Earth sees beam of

    energy

    http://highered.mcgraw-hill.com/sites/0072509856/student_view0/chapter14/neutron_stars_interactive.html

  • 11

    Crab Nebula

    Figure 21.10,

    Chaisson and McMillan,

    6th ed. Astronomy Today,

    © 2008 Pearson Prentice Hall

  • 12

    Crab Pulsar

    animation

    The pulsar must be young because it is seen at visible and

    X-ray wavelengths. Old pulsars emit mostly at lower

    energy radio wavelengths.

    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.

    http://bcs.whfreeman.com/dtu7e/pages/bcs-main.asp?v=chapter&s=13000&n=00090&i=13090.05

  • 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.

    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

  • 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

    15

  • 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

    16

  • 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.

    • 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.

    escape

    211 km/s for Earth

    GMv

    R

  • 21

    Schwarzschild Radius

    Normal star: Light

    can escape surface

    (vescape < c)

    Radius > Schwarzschild Radius

    Black Hole: Light

    cannot escape surface

    (vescape > c) Radius Schwarzschild Radius

    Distance from the center of a supermassive object at

    which the escape velocity would be equal to the speed

    of light.

  • 22

    Event Horizon

    Black Hole

    Light cannot escape

    Light can escape

    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.

  • 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 11-

    solar-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-solar-

    mass black hole

    in the galaxy

    NGC 7052.

  • 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.

    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

  • 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.