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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 />

21

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