Caption: This X-ray image of
the Cassiopeia A (Cas A) supernova remnant is the official
first light image Chandra
X-ray Observatory. Two shock waves
are visible: a fast outer shock and a slower inner shock. The
bright object near the center may be the long sought neutron
star or black hole that remained after the explosion that
produced Cas A.
NEUTRON STARSAt the end ... gravity always wins |
Neutron Stars:
A neutron star is the
stellar remnant left behind of one of the most cataclysmic
events in the Universe: a
Supernova explosion. As the
nuclear fuel in the star is exhausted, gravity takes over and
drives the star into its final state. The final state is a
compact star, such as a
White Dwarf, a Neutron Star, or
a Black Hole. Stars support themselves against gravitational
collapse by generating an enormous pressure in the interior of
the star. The three most important sources of pressure are:
"Radiation" Pressure | Scales as T4 |
"Classical" Pressure | Scales as T and N/V |
"Quantum" Pressure | Scales as (N/V)5/3 atT=0 |
Our Sun is now supported by
radiation and classical pressure. Yet, at the final stages of
its existence - as a white-dwarf star - it is the
quantum mechanical pressure from its electrons that will
support the Sun. For very massive stars, namely, those
exceeding the Chandrasekhar limit (of 1.4 Solar masses)
electron pressure is not effective and the star collapses
under its own weight.
In a fraction of a second the following very dramatic changes ensue:
The Nature of a Neutron
Star
As the core of a very massive star undergoes a collapse and its radius shrinks to an incredible size of only 10 km (the radius of the Sun is 700,000 km) its surface temperature will increase to about a few million degrees. According to Wien's law, this very hot object will radiate most of its energy at a wavelength of about 1 nm, or in the X-ray part of the electromagnetic spectrum. Thus, most of the radiation emitted from this very compact object is undetected by terrestrial Optical and Radio telescopes. Moreover, while the gravitational energy is being converted to kinetic energy (rising the temperature of the star) other quantities are being conserved (i.e., remain unchanged in the collapse). These are:
Angular Momentum: Scales as Radius2/Period Magnetic Flux: Scales as Radius2*MagField Mass of the Star: Scales as Radius3*Density
Properties | Sun | Neutron Star |
Radius (in km) | 700,000 | 10 |
Temperature (in K) | 5,800 | 1,000,000 |
Magnetic Field (Bsun) | 1.000 | 1,000,000,000 |
Density (grams/cm3) | 1.409 | 100,000,000,000,000 |
Hence, neutrons stars have
extremely large temperatures, magnetic fields and densities.
Yet in spite of being so hot, the neutron star has low
luminosity because of its very small size. Neutron Stars are
extremely difficult to detect, indeed! However, in 1967 a
graduate student by the name of Jocelyn
Bell detected a very peculiar radio signal made out
of very regular pulses of about one second.
At one point she and her Professor speculated that the signal
might have come from a distant civilization and considered
naming it LGM for the "Little
Green Men". As many more pulsars were found - with periods
ranging from few milliseconds to seconds - astronomers were
convinced that these were radio signals from astronomical
bodies which they named pulsars,
for "pulsating" stars. Now
we know that calling a neutron star a pulsar is a misnomer, as
the radio signal is due to the rotation of the star, rather
than to a pulsation. The rapidly-rotating neutron star emits
beams of radiation that sweep around the sky such as
lighthouses do. Once the beam of radiation crosses our line of
sight, we detect these periodic
"pulses". The best known pulsar to date lies in
the Crab Nebula which is the
remnant of a star whose explosion was witnessed by Chinese
astronomers in 1054 AD.