In an environment with a density of $\rho_0$, a point explosion with an energy of $E_0$ occurred, which caused an expanding shock wave with a radius of $R$. In the first approximation, the dependence $R(t)$ will be power-law for each of the arguments $\rho_0, E_0, t$:
\[R = S(\gamma) \cdot E^a_0 \cdot \rho_0^b \cdot t^c,\]where $S(\gamma)$ is a dimensionless constant depending on the gas.