In this paper, power series solutions for strong spherical shocks of time dependent variable energy propagating in a two-phase gas-particle medium are presented taking into consideration the power series solution technique (Sakurai in J Phys Soc Jpn 8:662-669, 1953; Freeman in J Phys D Appl Phys 2(1): [1697][1698][1699][1700][1701][1702][1703][1704][1705][1706][1707][1708][1709][1710] 1968). Assuming the medium to be a mixture of a perfect gas and small solid particles, the power series solutions are obtained in terms of 2 − M , where M is the upstream Mach number of shock. This investigation presents an overview of the effects due to an increase in (i) the propagation distance from the inner expanding surface and, (ii) the dust loading parameters on flow-field variables such as the velocity of fluid, the pressure, the density, and also on the speed of sound, the adiabatic compressibility of mixture and the change-in-entropy behind the strong spherical shock front.
IntroductionIn 1942 Guderley [1] first obtained self-similar solutions describing a converging strong shock wave propagating in an ideal gas. Such families of solutions require invariant boundary conditions under the similarity transformation. Van Dyke and Guttmann [2] described a converging shock driven by a piston with the help of analytical series. In series, the zeroth order term corresponds to the plane problem and the higher order terms account for the spherical effects. Oshima [3] described a diverging shock wave with approximations valid in three domains depending on the Mach number: strong, intermediate, and weak shock. Sakurai [4] presented another method to describe the diverging shocks and obtained the solutions in power series of 2 − M , where M is the upstream shock Mach number. Sakurai's power series solutions are for initially strong shock waves of constant energy and the zeroth order term of series solutions corresponds to the self-similar solutions for the Taylor-Sedov problem of a point explosion. The mathematical proof of existence of this solution has been demonstrated in 2009 by Takahashi [5]. Hafner [6] presented a power series solution for strong converging shock waves near the centre of convergence. The series form