Theory of the Fireball

I
using (5.25) md y = 1.13 to 1.20. A given material element vllich went
through the cooling wave at temperature T' and pressure p Trill now (at
m m
pressure p) have the temperature
oe
Tt = pm
If we assume Tm to be independent of time, then at a given tfme in Cne
adiabatic region (Tv, of Fig. 2)
2
as defined in Sec. l;b. Since we now use material coordinates in gm/cm ,
we should use mean free paths in the same unit. Table VI and (4.10) md
(lk.12) give tine required information. We mite (4.12) in the form
57
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