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
Energetic particles may be charged or neutral, light or heavy, or
electromagnetic in nature. Because of this diversity one might think
there would be no common grounds for comparing the action on matter of
different particles. Each particle might conceivably make its own
inimitable variety of chemical rearrangements. Actually this is not the
case.
Unlike some chemical poisons, which seek out specific molecules in our
body, the energetic particles strike at whatever atoms or molecules
happen to get in their way. They act, in this sense, like a sledge
hammer. Their effects can be measured directly from the strength (or
energy) of the blow. Which particle delivers the blow is of little
consequence provided the same amount of energy is delivered and provided
the same tissues are affected (in the case of living matter). After the
blow, however, some specific chemical effects may occur. When water or
some other molecule in the body is broken up by radiation, the fragments
produced may themselves be chemical poisons and attack the biologically
important large molecules in a secondary way. In fact, it seems probable
that a considerable part of the radiation damage caused in living
systems, both healthwise and genetically, occurs in this manner.
Although the energetic particles are all similar in their ultimate
action on matter, namely in producing wholesale destruction of atoms and
molecules, they differ somewhat in the way in which they bring about
this destruction. Charged particles act in one way, gamma rays in
another, and neutrons in still another. It is simplest to begin our
discussion with the charged particles.
The most important charged particles are those connected with the
natural background of radioactivity and cosmic rays, and the fission
process. These include alpha rays, beta rays, mesons, and fission
fragments. For review, a table of the weights and charges of these
particles, as well as a few others, is shown. As usual, we have used the
weight and charge of the proton as units.
_Particle_ _Weight_ _Charge_
proton 1 1
alpha 4 2
electron beta rays 1/1840 -1
positron ” 1/1840 1
deuteron 2 1
triton 3 1
meson 1/8 1, -1
average light fission fragment 97 20
average heavy fission fragment 138 22
Public-domain text, read in full here on John Shaqi.
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