Previous |  Up |  Next

Article

Full entry | Fulltext not available (moving wall 24 months)      Feedback
Keywords:
compressible flow; quasilinear differential equation; shock wave
Summary:
The paper examines the evolution of a weak discontinuity, specifically, an acceleration wave in a one-dimensional unsteady plasma flow influenced by an axial magnetic field in the presence of dust particles. We obtained self-similar solutions through the application of Lie group transformations. This study also explores the idea of interaction between the acceleration wave and a strong shock wave, with particular emphasis on the roles played by dust particles and the magnetic field. The effects of various parameters involved in the flow are examined. Additionally, the reflected and transmitted waves following the interactions are analyzed and the results are depicted.
References:
[1] Bluman, G. W., Cole, J. D.: Similarity Methods for Differential Equations. Applied Mathematical Sciences 13. Springer, New York (1974). DOI 10.1007/978-1-4612-6394-4 | MR 0460846 | Zbl 0292.35001
[2] Chadha, M., Jena, J.: Self-similar solutions and converging shocks in a non-ideal gas with dust particles. Int. J. Non-Linear Mech. 65 (2014), 164-172. DOI 10.1016/j.ijnonlinmec.2014.05.013
[3] Chadha, M., Jena, J.: Singular surface and steepening of waves in a non-ideal gas with dust particles. Comput. Appl. Math. 34 (2015), 729-739. DOI 10.1007/s40314-014-0135-x | MR 3365685 | Zbl 1357.76097
[4] Clarke, J. F.: Small amplitude gasdynamic disturbances in an exploding atmosphere. J. Fluid Mech. 89 (1978), 343-356. DOI 10.1017/S0022112078002633 | Zbl 0396.76050
[5] Conforto, F.: Interaction between weak discontinuities and shocks in a dusty gas. J. Math. Anal. Appl. 253 (2001), 459-472. DOI 10.1006/jmaa.2000.7152 | MR 1808148 | Zbl 0970.76101
[6] Jeffrey, A.: The propagation of weak discontinuities in quasi-linear hyperbolic systems with discontinuous coefficients. I. Fundamental theory. Appl. Anal. 3 (1973), 79-100. DOI 10.1080/00036817308839058 | MR 0393868 | Zbl 0256.35054
[7] Jena, J.: Self-similar solutions in a plasma with axial magnetic field ($\theta$-pinch). Meccanica 47 (2012), 1209-1215. DOI 10.1007/s11012-011-9505-2 | MR 2924642 | Zbl 1293.76180
[8] Jena, J., Chadha, M.: Interaction of acceleration wave with a strong shock is transient pinched plasma. J. Appl. Fluid Mech. 9 (2016), 2629-2634. DOI 10.18869/acadpub.jafm.68.236.22847
[9] Jena, J., Singh, R.: Existence and interaction of acceleration wave with a characteristic shock in transient pinched plasma. Meccanica 48 (2013), 733-738. DOI 10.1007/s11012-012-9627-1 | MR 3032417 | Zbl 1293.76080
[10] Kuwabara, S.: Similarity solutions for transient pinched plasma. J. Phys. Soc. Jap. 18 (1963), 713-718. DOI 10.1143/JPSJ.18.713
[11] Lax, P. D.: Hyperbolic systems of conservation laws. II. Commun. Pure Appl. Math. 10 (1957), 537-566. DOI 10.1002/cpa.3160100406 | MR 0093653 | Zbl 0081.08803
[12] Mentrelli, A., Ruggeri, T., Sugiyama, M., Zhao, N.: Interaction between a shock and an acceleration wave in a perfect gas for increasing shock strength. Wave Motion 45 (2008), 498-517. DOI 10.1016/j.wavemoti.2007.09.005 | MR 2406845 | Zbl 1231.76130
[13] Morro, A.: Interaction of acoustic waves with shock waves in elastic solids. Z. angew. Math. Phys. 29 (1978), 822-827. DOI 10.1007/BF01589293 | MR 0511914 | Zbl 0387.76069
[14] Pai, S. I., Hsieh, T.: Interaction terms in gas-solid two-phase flows. Z. Flugwiss. 21 (1973), 442-445. Zbl 0307.76059
[15] Palo, N. D., Jena, J., Chadha, M.: An analytical approach to study kinematics of shock waves in a dusty, cylindrical gas flow. ZAMM, Z. Angew. Math. Mech. 102 (2022), Article ID e202200019, 20 pages. DOI 10.1002/zamm.202200019 | MR 4559166 | Zbl 1536.76054
[16] Pandey, M.: Evolution of weak discontinuities in non-ideal magnetogasdynamic equations. Int. J. Appl. Comput. Math. 1 (2015), 257-265. DOI 10.1007/s40819-015-0033-y | MR 3346022 | Zbl 1320.76125
[17] Pandey, M., Sharma, V. D.: Interaction of a characteristic shock with a weak discontinuity in a non-ideal gas. Wave Motion 44 (2007), 346-354. DOI 10.1016/j.wavemoti.2006.12.002 | MR 2311431 | Zbl 1231.76132
[18] Radha, C., Sharma, V. D., Jeffrey, A.: On interaction of shock waves with weak discontinuities. Appl. Anal. 50 (1993), 145-166. DOI 10.1080/00036819308840191 | MR 1278323 | Zbl 0739.76029
[19] Ruggeri, T.: Interaction between a discontinuity wave and a shock wave: Critical time for the fastest transmitted wave, example of the polytropic fluid. Appl. Anal. 11 (1980), 103-112. DOI 10.1080/00036818008839323 | MR 0599258 | Zbl 0482.76062
[20] Sharma, V. D.: Quasilinear Hyperbolic Systems, Compressible Flows, and Waves. Chapman & Hall/CRC Monographs and Surveys in Pure and Applied Mathematics 142. CRC Press, Boca Raton (2010). DOI 10.1201/9781439836910 | MR 2668539 | Zbl 1200.76002
[21] Sharma, V. D., Ram, R., Sachdev, P. L.: Uniformly valid analytical solution to the problem of a decaying shock wave. J. Fluid Mech. 185 (1987), 153-170. DOI 10.1017/S0022112087003124 | Zbl 0651.76023
[22] Singh, R., Jena, J.: Interaction of an acceleration wave with a strong shock in reacting polytropic gases. Appl. Math. Comput. 225 (2013), 638-644. DOI 10.1016/j.amc.2013.09.074 | MR 3129679 | Zbl 1334.76138
Partner of
EuDML logo