Our Nuclear Future: Facts, Dangers and Opportunities — John Shaqi
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
Thus fission remained a secret. But in England Leo Szilard obtained
patent papers on the nuclear chain reaction. He pointed out that in some
nuclear reactions free neutrons might be released. These neutrons might
then succeed in producing further reactions which would produce more
neutrons. Provided that at least one neutron made in each reaction were
able to induce a reaction in another nucleus, a chain reaction would
take place.
The main problem, of course, was to avoid excessive neutron losses.
There are two ways in which the losses mainly occur. One is by wasteful,
nonreproductive capture in the nuclei; the other, by neutron leakage
from the material surface. This second loss, Szilard showed, could be
minimized by using a sufficiently large amount of chain-reacting
material.
The point is that a neutron born in a nuclear reaction must travel on
the average a certain distance before it can produce another reaction.
If the size of the chain-reacting material is much less than this
distance, practically all of the neutrons produced will be able to
escape through the material surface, and no chain reaction will be
possible. If the size of the material is large compared to this
distance, the leakage loss becomes negligible, and the possibility of a
chain reaction depends entirely on the magnitude of the first kind of
loss, the wasteful captures in nuclei. If this loss is not too great,
and a chain reaction is possible, there will be a _critical_ size of the
material at which on the average exactly one neutron per reaction will
be able to induce another reaction. A just critical chain reaction of
this kind is what is needed for an atomic reactor.
If the size of the material is greater than the critical size, on the
average more than one neutron per reaction will cause another reaction
and the chain reaction will run away. If, for example, two neutrons can
cause another reaction, there will be two neutrons after the first
generation, four after the second, eight after the third, and so forth.
This is the principle of the atomic bomb.
After about 80 generations, an appreciable fraction of all the nuclei in
the material will have undergone a nuclear transformation and so much
energy will have been released that the material will not stay together
even for the short time needed to produce the next generation. The whole
material begins to fly apart, the system becomes sub-critical, and the
chain reaction stops. The entire process lasts only a fraction of a
microsecond.
Thus even before fission was discovered, Szilard laid the basis for
constructing the atomic bomb and the nuclear chain reactor. As materials
in which a chain reaction might conceivably be made to occur he named
thorium, uranium and beryllium. On beryllium he was wrong because the
mass of this atom was incorrectly known. On thorium, his guess was good.
On uranium, he hit the bull’s eye.
Public-domain text, read in full here on John Shaqi.
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