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(1) 50% as blast;
(2) 35% as thermal radiation; made up of a wide range of the electromagnetic spectrum, including infrared, visible, and
ultraviolet light and some soft x-ray emitted at the time of the explosion; and
(3) 15% as nuclear radiation; including 5% as initial ionizing radiation consisting chiefly of neutrons and gamma rays
emitted within the first minute after detonation, and 10% as residual nuclear radiation. Residual nuclear radiation is the
hazard in fallout.
b. Considerable variation from this distribution will occur with changes in yield or location of the detonation. This
is best shown by comparing the ranges of damage due to these effects of weapons of different size yields (Table 3-I).
c. The distribution of weapon energy yield is altered significantly by the enhanced radiation nuclear warhead. In simplest
terms an enhanced radiation warhead is designed specifically to reduce the percentage of energy that is dissipated as blast
and heat with a consequent increase in the percentage yield of initial radiation. Approximate percentage energies are 30%
blast; 20% thermal; 45% initial radiation; and 5% residual radiation.
[Pic 52 pcf.city.Hiroshima]
303. Initial Energy Transfer and Formation of Fireball.
a. Because of the tremendous amounts of energy liberated per unit mass in a nuclear detonation, temperatures of several
tens of million degrees centigrade develop in the immediate area of the detonation. This is in marked contrast to the few
thousand degrees of a conventional explosion. At these very high temperatures the nonfissioned parts of the nuclear weapon
are vaporized. The atoms do not release the energy as kinetic energy but release it in the form of large amounts of electromagnetic
radiation. In an atmospheric detonation, this electromagnetic radiation, consisting chiefly of soft x-ray, is absorbed within
a few meters of the point of detonation by the surrounding atmosphere, heating it to extremely high temperatures and forming
a brilliantly hot sphere of air and gaseous weapon residues, the so-called fireball. Immediately upon formation, the fireball
begins to grow rapidly and rise like a hot air balloon. Within a millisecond after detonation, the diameter of the fireball
from a 1 megaton (Mt) air burst is 150 m. This increases to a maximum of 2200 m within 10 seconds, at which time the fireball
is also rising at the rate of 100 m/sec. The initial rapid expansion of the fireball severely compresses the surrounding atmosphere,
producing a powerful blast wave, discussed below.
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