2019
DOI: 10.1007/s11587-019-00472-w
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Propagation of non-planar weak and strong shocks in a non-ideal relaxing gas

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Cited by 9 publications
(3 citation statements)
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“…where Ω = (m∕x) x=X and v = u s − Π. With the help of equations ( 6), (9), and (10) (2,3) , we get the nonlinear differential equation describing the shock strength [u] as…”
Section: Evolution Equation For Shock Progressionmentioning
confidence: 99%
See 1 more Smart Citation
“…where Ω = (m∕x) x=X and v = u s − Π. With the help of equations ( 6), (9), and (10) (2,3) , we get the nonlinear differential equation describing the shock strength [u] as…”
Section: Evolution Equation For Shock Progressionmentioning
confidence: 99%
“…After the developments of ideal theory, many authors extended the propagation of growth and decay behavior of converging and diverging shocks in non‐ideal distinct mediums (one may see [7] to [8]). Shah and Singh investigated the propagation of weak and strong shocks in a non‐ideal relaxing gas in [9] and the profiles of imploding shocks in [10] and also determined the evolution equation for singular surface in non‐ideal reacting gases with dust particles in [11].…”
Section: Introductionmentioning
confidence: 99%
“…Gupta and Jena [11] explained the kinematics of the spherical shock wave in interstellar gas clouds and Mehla and Jena [13] studied the effect in a relaxing gas due to the presence of dust particles. Shah and Singh [14] discussed the evolutionary behavior of non-planar weak and strong shock waves propagating into a non-ideal relaxing gas by using the kinematics of one-dimensional motion. The approximation method was used by Lee [24] and Van Dyke and Guttman [25] to solve the initial value problem of propagation of shock waves by expanding the solution in the powers of the time, where Chisnell [26] used the theory of singular point to explain the propagation of shock analytically.…”
Section: Introductionmentioning
confidence: 99%