a
(R remaining constant).
The nev. gos volume is exnressed as V, with a
density of P,. (v, = der” R)
The mass has not changed; thus
MEVDS = darn”aro,
(an << R)
harp/3 = dar’aro,
(1.5)
Ap, = Ro/3
(1.6)
Lyuation 1.6 indicstes that a rey cricinetins in the center of the
Sore would travers¢ only 1/5 cf the mice in the eieli model
would in the hemogenesus model.
radiation.
thet 4t
Tre result would be ar enhancanent cf
Once tic shell of mterial in the shock front passes the es
detector, an even grcater enhancement results.
fo previcucly steted, the ho”
(no x) coegencu. .f initict wodictios
is etsenticlly esittes witidn Ce Seeomc.
Cinec di takes at lecsi cone
second for tx succh from t. rece. c dcicctur at a disvarec of 7,0
4
fect (even fcr devices in the order of 6 Mt), the N”
is not significantly enhanced.
(n, y) component
The fission-produci gemmac continue tc
contribute during thc first 3° seconds; therefore, this radiction is
strongly enhanced by the shock wove.