2012
DOI: 10.5923/j.mechanics.20120202.04
|View full text |Cite
|
Sign up to set email alerts
|

Ionizing Cylindrical Shock Waves in a Rotating Homogeneous Non-ideal Gas

Abstract: Similarity Solutions are obtained for one-dimensional adiabatic flow behind ionizing cylindrical shock wave propagating in a rotating non-ideal gas in presence of an azimuthal magnetic field. The electrical conductivity in the medium ahead of the shock is assumed to be negligible, which becomes infinitely large after passage of the shock. In order to obtain the similarity solutions, the initial density of the medium is assumed to be constant and the initial angular velocity to be obeying a power law and to be … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
4
0

Year Published

2013
2013
2021
2021

Publication Types

Select...
3

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(4 citation statements)
references
References 25 publications
(30 reference statements)
0
4
0
Order By: Relevance
“…The distribution of the flow variables between the shock front (η = 1) and the inner expanding surface (η = η p ) is obtained by numerical integration of ( 46) -(52) with the boundary conditions (33) by Runge-Kutta method of fourth order. For the purpose of numerical integration, the values of the constant parameters are taken to be (Roberts and Wu [20], Elliott [3], Singh and Mishra [8], Rosenau [41], Vishwakarma and Singh [32 ], Singh and Nath [34] ρ2 are shown in tables 1 and 2 for different cases.…”
Section: Resultsmentioning
confidence: 99%
See 3 more Smart Citations
“…The distribution of the flow variables between the shock front (η = 1) and the inner expanding surface (η = η p ) is obtained by numerical integration of ( 46) -(52) with the boundary conditions (33) by Runge-Kutta method of fourth order. For the purpose of numerical integration, the values of the constant parameters are taken to be (Roberts and Wu [20], Elliott [3], Singh and Mishra [8], Rosenau [41], Vishwakarma and Singh [32 ], Singh and Nath [34] ρ2 are shown in tables 1 and 2 for different cases.…”
Section: Resultsmentioning
confidence: 99%
“…In addition to the shock conditions (33), the condition to be satisfied at the inner boundary surface is that the velocity of the fluid is equal to the velocity of the inner boundary itself. This kinematic condition, from (23) and (24), can be written as…”
Section: Similarity Solutionsmentioning
confidence: 99%
See 2 more Smart Citations