Our Nuclear Future: Facts, Dangers and OpportunitiesTeller, Edward
Science
Our Nuclear Future: Facts, Dangers and Opportunities
Teller, Edward
Nuclear energy -- Popular works; Nuclear weapons; Radioactivity -- Physiological effect
These forces are definitely not of gravitational origin. Gravitational
attraction is extremely weak compared to the attraction between neutrons
and protons, and is utterly negligible in the realm of nuclear
phenomena. Neither can the nuclear forces be electrical in origin. The
neutrons are electrically neutral; and the protons actually repel each
other by virtue of their electrical charge. The nuclear forces are
something entirely new. They are the strongest forces yet encountered,
and they are without a counterpart in the macroscopic world.
Nuclear forces are not yet completely understood. But to understand
nuclear stability we need to know only one peculiar fact governing the
behavior of neutrons and protons (and incidentally also electrons): They
want to be different. To each particle a state or pattern of motion can
be assigned. When any two neutrons are compared, their pattern of motion
must be essentially different. The same holds for any two protons. A
neutron and a proton, however, may be found in similar patterns since
they differ anyway in their charge.
Now among the possible patterns of motion some have lower and some have
higher energies. Individual neutrons and protons will first occupy the
lowest energy states, in accordance with the rule of least energy for
maximum stability. Then the demand for a difference will force
subsequent particles into patterns of higher and higher energies.
Since a neutron does not exclude a proton from being in the same
pattern, the lowest energy state may be occupied simultaneously by one
neutron and one proton.[4] If another neutron or proton is added, it
must be put into the next state of higher energy. For this reason we
would expect that nuclei are most stable when they contain an equal or
nearly equal number of neutrons and protons. For nuclei which are not
too heavy, this is indeed the case. For example, nitrogen, which has
seven protons, has two stable isotopes, N¹⁴ and N¹⁵, with seven and
eight neutrons respectively. For heavy nuclei, however, the situation is
a little different.
The nuclear force between neutrons and protons acts only over a very
short range—the particles must almost be in contact with each other in
order to experience a sizeable attraction. Consequently a neutron or a
proton interacts only with its immediate neighbors in the nucleus. The
electrical repulsion between the protons, however, acts over a much
longer range. A proton is repelled by all the other protons in the
nucleus. For heavy nuclei this repulsion is sufficient to reduce the
number of protons relative to the number of neutrons. Lead, for example,
with 82 protons, has four stable isotopes, with 122, 124, 125, and 126
neutrons.
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