By consolidating shock propagation data from two distinct sources [1][2] into a single chart using a log scale for both axes, the contrasting speeds associated with two distinct phases of an explosion, which contribute to the formation of a shock front, become clearly evident.
The detonation phase involves the expansion of hot gaseous products at an initial hypersonic speed. This speed eventually decays to the speed of sound, marking the transition to the blast wave. The blast wave detaches upon the completion of the detonation phase and then propagates as a pressure wave at the speed of sound in the surrounding air, or Mach 1.0.
The timing and location of this transition depend on the type and size of the explosion, with the blast wave originating within milliseconds of the detonation of a chemical explosion up to a few seconds of a nuclear explosion. In all cases, the blast wave propagates at Mach 1.0.
1 Kenney G. F and Graham K. J, (1985) Explosive Shocks in Air, Springer Science+Business Media, LLC, Table XI
[2] Bethe H. A, Fuchs K., Hirschfelder J, Magee J., Pearls R. and von Neumann J. (1958) Blast Wave U. S. Atomic Energy Commission, p. 185 ("The Los Alamos report")