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Theory of the Fireball

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highest possible density <strong>of</strong> about lop For explosions at nigher alti-<br />

0.<br />

tude, this conclusion is even more true.<br />

Tne tables by Meyerott et al.. do not include absorption by triatomic<br />

(and more complicated) molecules, Of <strong>the</strong>se, NO2 is known to have strong<br />

absorption bands in <strong>the</strong> visible. After this paper was completed, I<br />

received new calculations by Gilmoreg3 which include <strong>the</strong> effect <strong>of</strong> U02.<br />

The effect is very striking as is shown by Table I, which gives <strong>the</strong><br />

absorption coefficient for <strong>the</strong> "typical" frequency hv = 2-1/8 ev, and<br />

for several temperatures and densities (<strong>the</strong> absorption is strong from<br />

about 1-314 to 2-3/4 ev) .<br />

PIP.<br />

T<br />

Without<br />

With<br />

Table I. Absorption Coefficients at hv = 2-l/8 ev<br />

with and without NO2<br />

10 10 10 10 1<br />

Note: For each value, <strong>the</strong> power <strong>of</strong> 10 is indicated by a strperscript.<br />

Because NO is triatomic, its absorption depends strongly on density.<br />

2<br />

As <strong>the</strong> shocked gas expands, <strong>the</strong> NO2 dissociates and <strong>the</strong> gas becomes trans-

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