' . Let the gas be compressed inte a shell with thickness 42 (RE remaining constant).
Cr (Wek
fhe new gas volume is expressed as V, vith a density of
BAR).
The mass has not changed; thus
Me Veo = hyR? AR CO (AR<<R)
s7mPe sg h7RPAaRe,
(2.5)
A RR,
(1.6)
RC
a
Bquation 1.6 iudicates that a ray originating in the center ef the
sphere would traverse enly 1/3 of the mass in the shell model that it
~WULA fin the hemegencous model. ‘Tee result would be an enhancement of
Fediation. Once the shell of material in the shock freat passes the
“t
ate
| Q@etertor, an even greater enhancement results.
As previously stated, the #* (n,/ ) component of initial ratiation
is eneentially enitted vithis 0.2 second. Since it taxes st least one
second for the shock front te reach « detector at a distance ef 7000 feet
(even for devices in the order of 6 Mt), the F* (n,,/) component is net
significantly enhanced. fhe fission-profuct games continue te contribute
for the first 30 secomfis. ‘Therefore, this refiation is strongly enhanced
Wy the shock vare.
ST. LOWS FRC