Lecture 17: Neutron Stars and Black Holes in Astro 150 Spring 2005, Study notes of Astronomy

A portion of lecture notes from astro 150 spring 2005, covering the topics of neutron stars and black holes. Information on the properties of neutron stars, their discovery through pulsars, and the role of pulsars in astronomy and physics. Additionally, it discusses black holes, their environment, and how they can be identified.

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Astro 150 Spring 2005: Lecture 17 page 1
Reading: Chapter 18, Sect. 18.1-18.3
OBAFGKM Winners!
Exam 2: Thursday after break, March 24; essay (next) Tuesday
Brief review of last time: Stellar Evolution II
White Dwarf Stars
hot but faint –> very small (Sirius B)
supported by electron degeneracy pressure
evolution through cooling
Final evolution: 8Msun < M < 25Msun
burns C, etc. but with diminising efficiency
onion-skin structure
iron burning eats energy
Supernova
iron core collapse, rebound (in seconds)
synthesis of all heavy elements
expanding supernova remnant
Neutron Stars
supported by neutron degeneracy
M ~ 2Msun, R ~ 20 km: density ~ 1014 g/cc
small and very faint
Astro 150 Spring 2005: Lecture 17 page 2
Neutron Stars
Mass ~ 2.0 Msun
Radius ~ 0.00002 Rsun
Temperature ~ 5x105 K
so, L/Lsun ~ 0.001 - nearly all in X-ray
rarity of neutron stars (end product of O, B star
evolution) means:
!closest is still pretty far away
!very unlikely to see in optical (or even X-ray)
L
Lsun
=R
Rsun
2T
Tsun
4
Astro 150 Spring 2005: Lecture 17 page 3
Discovery of Neutron Stars - Pulsars (1967)
1967: S. Jocelyn Bell discovers a radio signal:
regularly pulsing
rapid
(once every 1.33 seconds)
extraterrestrial
aliens? LGM1, LGM2, ...
Neutron stars !
1968: Tommy Gold (and Franco Pacini)
pulsars are rapidly rotating neutron stars
beaming by e- in magnetic field
NS rotation sweeps beams
confirmed by measures change in spin rate
PSR 0329:
0.72 s
1974 Nobel Prize to... Tony Hewish
(Bell’s advisor ?!#@)
Astro 150 Spring 2005: Lecture 17 page 4
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Reading: Chapter 18, Sect. 18.1-18. OBAFGKM Winners! Exam 2: Thursday after break, March 24; essay (next) Tuesday

Brief review of last time: Stellar Evolution II

White Dwarf Stars

• hot but faint –> very small (Sirius B)

• supported by electron degeneracy pressure

• evolution through cooling

Final evolution: 8M sun

< M < 25M

sun

burns C, etc. but with diminising efficiency

onion-skin structure

• iron burning eats energy

Supernova

• iron core collapse,^ rebound (in seconds)

• synthesis of all heavy elements

• expanding supernova remnant

• Neutron Stars

• supported by^ neutron degeneracy

M ~ 2M sun,

R ~ 20 km: density ~ 10

14 g/cc

• small and very faint

Neutron Stars

Mass ~ 2.0 M

sun

Radius ~ 0.00002 R

sun

• Temperature ~ 5x

K

so, L/L

sun

~ 0.001 - nearly all in X-ray

rarity of neutron stars (end product of O, B star

evolution) means:

! closest is still pretty far away

! very unlikely to see in optical (or even X-ray)

L

L (^) sun

=

R

Rsun

2 T

Tsun

4

Astro 150 Spring 2005: Lecture 17 page 3 Discovery of Neutron Stars - Pulsars (1967)

1967 : S. Jocelyn Bell discovers a radio signal:

regularly pulsing

rapid (once every 1.33 seconds)

extraterrestrial

aliens? LGM1, LGM2, ...

Neutron stars!

1968: Tommy Gold (and Franco Pacini)

pulsars are rapidly rotating neutron stars

• beaming by e

  • in magnetic field

NS rotation sweeps beams

confirmed by measures change in spin rate

PSR 0329: 0.72 s

1974 Nobel Prize to... Tony Hewish

(Bell’s advisor ?!#@)

Astro 150 Spring 2005: Lecture 17 page 4

Pulsars - a new tool for astronomy and physics

Binary Pulsars

! precise tests of general relativity (1993 Nobel, Hulse & Taylor)

Millisecond Pulsars

! recycled pulsars spun-up by companion (Don Backer)

“Black Widow” Pulsars

! pulsar blasts away its companion (Dan Stinebring)

Pulsars with Planets

" timing “jitter” -> planet-sized companions (Alex Wolsczan)

PSR 1937 (0.00167s)

Crab Pulsar

(0.033 s)

M > 25 M

sun

  • iron core > 5 M sun

" • even neutron degeneracy can’t stop collapse

complete gravitational collapse to...

Why black?

Escape velocity:

  • from^ Earth^ = 11.3 km/s = 25,400 mph
  • from^ Sun^ = 600 km/s = 1,350,000 mph
  • from a^ WD!= 5000 km/s
  • from a^ NS!^ = 200,000 km/s!^ = 2/3 the speed of^ light!

1783 : John Mitchell

escape velocity > speed of light when

!!!!!! R < R

sch

= 3 km x M/M

sun

A

BLACK

HOLE

Astro 150 Spring 2005: Lecture 17 page 7

1905: Albert Einstein

NOTHING can travel faster than light

... the ultimate speed limit is 300,000 km/s

near Black Holes, light cannot escape

no light = no information

EVENT HORIZON = point of no return

• within Event Horizon^ = central singularity

Anything that enters the Event Horizon loses contact

with the rest of the Universe... forever

Life near a Black Hole

far outside: (d >> R sch ): feel gravity as elsewhere

just outside: tidal forces...

inside: (d < R sch

): cut off from Universe

Astro 150 Spring 2005: Lecture 17 page 8

The Black Hole Environment

Dangerous - tidal forces are enormous