Theory of the Fireball
Theory of the Fireball
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)