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Theory of the Fireball

Theory of the Fireball

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The concentration <strong>of</strong> all <strong>the</strong> absorbing species depends strongly on<br />

temperature: The N first positive absorption starts from <strong>the</strong> electronic<br />

2<br />

level A, which has an excitation energy <strong>of</strong> 5.7 ev; NO itself requires<br />

high temperature for its formation; and N2 and 0- are ions whose concen-<br />

tration behaves like <strong>the</strong> electron concentration, discussed above in<br />

See. 4a. Therefore, <strong>the</strong> absorption depends strongly on temperature.<br />

first positive is <strong>the</strong> most important absorber, and its temperature depend-<br />

ence (relative to <strong>the</strong> ground state <strong>of</strong> N2) is about<br />

5.7 ev (- KT )<br />

The concentration <strong>of</strong> N~ up to 6000' is nearly independent <strong>of</strong> density,<br />

but at 80Wo it is about proportional to p1l2 (per air atom) so that near<br />

"N2 -<br />

3/2 ,8<br />

which is nearly <strong>the</strong> same dependence as derived in ( 4.4) for <strong>the</strong> free -f ree<br />

transitions. In terms <strong>of</strong> pressure we get<br />

Table V gives <strong>the</strong> absorption coefficients for four temperatures,<br />

three densities, and -six wave lengths. In <strong>the</strong> visible (1-1/8 to 2-5/8 ev)<br />

<strong>the</strong> strong increase in absorption with temperature is evident, a factor<br />

I 37<br />

+<br />

N2<br />

, .

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