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Theory of the Fireball

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(3.21), it is small compared to <strong>the</strong> free-free absorption at' this low<br />

frequency, except at T < 5000'. Its main effect is <strong>the</strong>refore to lower<br />

<strong>the</strong> radiating temperature in <strong>the</strong> infrared somewhat.<br />

Since <strong>the</strong> free-free transitions are <strong>the</strong> main cause <strong>of</strong> infrared<br />

absorption, <strong>the</strong> electron density governs <strong>the</strong> temperature and density<br />

dependence. For p/p, 2 10-1 and T 5 800o0, <strong>the</strong> ma& species <strong>of</strong> positive<br />

4-<br />

ions is NO The ionization energy <strong>of</strong> NO is 9-22 ev; tnerefore, <strong>the</strong><br />

electron density is roughly proportional to<br />

From 6000 to 8000°, this gives a factor <strong>of</strong> about 10 in <strong>the</strong> electron<br />

density, in accord with Gilmore's tables. Near 8000°, we' may write<br />

approximately<br />

-1.5<br />

Writing p - pT , this gives<br />

The temperature dependence<br />

out about <strong>the</strong> same.<br />

b. Visible<br />

<strong>of</strong> <strong>the</strong> absorption in <strong>the</strong> visible will turn<br />

In <strong>the</strong> visible and for temperatures below about 10,OOOo, <strong>the</strong> main<br />

34<br />

(4.3)<br />

(4.4)

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