ments. In stars less massive than the sun, the
reaction converting hydrogen into helium is
the only one that takes place. In stars more
massive than the sun but less massive than
about eight solar masses, further reactions
that convert helium to carbon and oxygen take
place in successive stages before such stars
explode. Only in very massive stars (that are
more massive than eight solar masses), the
chain reaction continues to produce elements
up to iron.
A star is a balancing act between two
huge forces. On the one hand, there is the
crushing force of the star’s own gravity trying
to squeeze the stellar material into the small-
est and tightest ball possible. On the other
hand, there is tremendous heat and pressure
from the nuclear reactions at the star’s center
trying to push all of that material outward.
The iron nucleus is the most stable
nucleus in nature, and it resists fusing into
any heavier nuclei. When the central core of a
very massive star becomes pure iron nuclei,
the core can no longer support the crushing
force of gravity resulting from all of the matter
above the core, and the core collapses under
its own weight.
The collapse of the core happens so fast
that it makes enormous shock waves that
blow the outer part of the star into space—a
supernova. It is during the few seconds of
the collapse that the very special conditions of
pressure and temperature exist in the super-
nova that allow for the formation of elements
heavier than iron. The newly created elements
are ejected into the interstellar dust and gas
surrounding the star.
“The amount of elements released
through a supernova is truly phenomenal,”
says Stan Woosley, professor of astronomy
and astrophysics at the University of Califor-
nia at Santa Cruz. “For example, SN1987A, a
supernova seen in 1987, ejected 25,000 Earth
masses of iron alone.”
How stars make
elements heavier
than iron
Elements that are heavier than iron can
be assembled within stars through the capture
of neutrons—a mechanism called the “s” pro-
cess. The process starts when an iron nucleus
captures neutrons, thus creating new nuclei.
These nuclei can be either stable, that is, they
do not change, or radioactive, meaning that
they transform, or decay, into another element
after a certain amount of time, which can be
as short as a fraction of a second and as long
as a few million years.
Also, the newly formed nuclei can be
different versions of a given element. These
different versions of an element are called
isotopes. They all contain the same number
of protons in their nucleus but have differ-
ent numbers of neutrons. Some isotopes are
radioactive, while others are stable and never
change.
For example, nickel can appear in
the form of 23 different isotopes. They all
have 28 protons, but each isotope contains
between 20 and 50 neutrons. Of these 23
isotopes, only five are stable, while the others
are radioactive.
If a nucleus produced through the “s”
process is stable, it may capture another
neutron. If it is radioactive, it transforms into
another nucleus. This other nucleus can, in
turn, absorb another neutron, leading to a
heavier nucleus.
For example, nickel-64, which contains
28 protons and 36 neutrons, can absorb a
neutron, leading to nickel-65, which contains
28 protons and 37 neutrons:
Nickel-65 is radioactive. It exists for only 2
and a-half hours, and then transforms into
copper-65—the next element in the periodic
table, which contains 29 protons and 36 neu-
trons. This is a process called beta decay, in
which a neutron transforms into a proton and
an electron:
Copper-65 is stable, so nothing happens after
that.
This neutron capture mechanism, called
the “s” process, is extremely slow. Hundreds
or thousands of years might elapse between
neutron strikes. But another process, called
the “r” process, which stands for “rapid,”
allows for the rapid capture of neutrons.
Unlike the “s” process, which occurs inside a
star before it explodes, the “r” process hap-
pens only during the explosion of a star.
Exploding and
cooking elements
at the same time
When a star explodes into a supernova, it
produces a huge amount of light and releases
an extremely high number of neutrons (on the
order of 10 thousand billion billion neutrons
per square inch per second). These neutrons
are then rapidly captured by the various nuclei
that are also released by the exploding star,
producing new nuclei through the “r” process.
In this process, even though
many neutrons are available, only
a limited number can be added
to a given nucleus; otherwise,
a nucleus becomes radioactive
and breaks up. Neutrons in a nucleus are
thought to occupy shells—similar to succes-
sive shells on a hard candy. When a nucleus
gets “saturated” with neutrons, that is, when
its shells are filled up, it undergoes a beta
decay process to become the nucleus of the
next element on the periodic table. This new
nucleus, in turn, absorbs as many neutrons
Ni-65 (28 protons, 37 neutrons) ➞
electron + Cu-65 (29 protons, 36 neutrons)
Ni-64 (28 protons, 36 neutrons) + neutron ➞
Ni-65 (28 protons, 37 neutrons)
Combined X-ray and optical images of the Crab
Nebula.
The Crab Nebula is a six-light-year-wide expanding
remnant of a star’s supernova explosion.
ChemMatters, OCTOBER 2009 7
NASA, ESA, J. HESTER AND A. LOLL (ARIZONA STATE UNIVERSITY)
NASA/CXC/ASU/J. HESTER ET AL.