Theory of the Fireball
Theory of the Fireball
Theory of the Fireball
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Table 11. Adiabats<br />
( 'Present" density, 0. 1-p shock density, lopo)<br />
0;<br />
T 4,000 6,000 8, ooo 12,000<br />
T 9,000 10,500 18,000 28,000<br />
S<br />
y' - 1 0 213 0.194 0.144 0 1-53<br />
Y; - 1 0.208 0 190 0.190 0.20<br />
z 1-13 1.27 - 1.68 2.06<br />
=S 1-03<br />
. 1.6 2.06 3<br />
Assming an adiabat <strong>of</strong> constant 7 = y', <strong>the</strong> density <strong>of</strong> a mass<br />
element is<br />
P = PS(k)1/Y (3.5)<br />
Now ps is a constant, and at any given time, p is <strong>the</strong> s&e for all mass<br />
elements except those very close to <strong>the</strong> shock, hence<br />
4 7<br />
P - Ps<br />
(w means proportional- to)<br />
If we now introduce <strong>the</strong> abbreviation<br />
3<br />
m = r (3.7)<br />
which is proportional to <strong>the</strong> mass inside <strong>the</strong> mass element considered,<br />
and if we use ( 3.2), we find that at any given time<br />
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