' . 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