Numerical Simulations of Shock-driven Heavy Fluid Layer
DOI:
https://doi.org/10.13052/jgeu0975-1416.1314Keywords:
Shock wave, heavy fluid layer, vorticity, interface deformationAbstract
The present study presents the numerical simulations for a shocked-heavy fluid layer with a stratified N2/SF6/N2 configuration. Simulations were conducted using a third-order modal discontinuous Galerkin method to solve the compressible two-component Euler equations. The results were validated against experimental data, confirming the accuracy of the computational approach. Dynamics of the heavy fluid layer were found to be strongly influenced by the shock Mach numbers Ms = 1.15, 1.25, 1.5. At a lower Mach number Ms = 1.15, the interface deformations remained smooth and relatively symmetric, with limited vorticity generation and weak perturbations. Baroclinic effects at this stage were minimal, and the instability growth remained linear. As the Mach number increased to Ms = 1.25, the interaction became nonlinear, leading to the formation of small-scaled vortex structures driven by moderate baroclinic effects. Interface mixing intensified as rotational motion increased. At the highest Mach number Ms = 1.5, the interface rapidly evolved into chaotic structures, characterized by significant vorticity amplification, vortex roll-up, and the onset of turbulence. The baroclinic vorticity, resulting from the misalignment of pressure and density gradients, dominated the vorticity production mechanism, particularly at higher Mach numbers. Quantitative analysis demonstrated that average vorticity, baroclinic vorticity, and enstrophy grew rapidly with increasing Mach numbers. Enstrophy, which quantifies turbulence intensity, exhibited pronounced growth at Ms = 1.5, marking the transition to turbulent mixing.
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References
R.D. Richtmyer, ‘Taylor instability in shock acceleration of compressible fluids,’ Communications on Pure and Applied Mathematics, 13:297, 1960.
E.E. Meshkov, ‘Instability of the interface of two gases accelerated by a shock wave,’ Fluid Dynamics, 4:101–104, 1969.
S. Singh, ‘Role of Atwood number on flow morphology of a planar shock-accelerated square bubble: A numerical study,’ Physics of Fluids, 32: 126112, 2020.
J. Lindl, O. Landen, J. Edwards, E. Moses, and NIC team, ‘Review of the national ignition campaign 2009-201,’ Physics of Plasmas, 21: 020501, 2014.
D. Arnett, ‘The role of mixing in astrophysics,’ The Astrophysical Journal Supplement Series, 127: 2131, 2000.
K.O. Mikaelian, ‘The role of mixing in astrophysics,’ Physical Review A, 28: 1637–1646, 1983.
J.W. Jacobs, D.G. Jenkins, D.L. Klein, and R.F. Benjamin, ‘Nonlinear growth of the shock-accelerated instability of a thin fluid layer,’ Physical Review A, 28: 1637–1646, 1983.
G.I. Taylor, ‘The instability of liquid surfaces when accelerated in a direction perpendicular to their planes. I,’ Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 201: 192–196, 1950.
L. Rayleigh, ‘Investigation of the character of the equilibrium of an incompressible heavy fluid of variable density,’ Proceedings of the London Mathematical Society, 14: 170–177, 1883.
K.O. Mikaelian, ‘Richtmyer-Meshkov instabilities in stratified fluids,’ Physical Review A, 31: 410–419, 1985.
K.O. Mikaelian, ‘Rayleigh–Taylor and Richtmyer–Meshkov instabilities in finite thickness fluid layers,’ Physics of Fluids, 7: 888–890, 1995.
B.J. Balakumar, G.C. Orlicz, J.R. Ristorcelli, S. Balasubramanian, K.P. Prestridge, and C.D. Tomkins, ‘Turbulent mixing in a Richtmyer–Meshkov fluid layer after reshock: velocity and density statistics,’ Journal of Fluid Mechanics, 696: 67–93, 2012.
J.W. Jacobs, D.G. Jenkins, D.L. Klein, and R.F. Benjamin, ‘Turbulent mixing in a Richtmyer–Meshkov fluid layer after reshock: velocity and density statistics,’ Journal of Fluid Mechanics, 28: 23–42, 1995.
Y. Liang, and X. Luo, ‘Review on hydrodynamic instabilities of a shocked gas layer,’ Science China Physics, Mechanics & Astronomy, 66: 104701, 2023.
Y. Liang, and X. Luo, ‘On shock-induced heavy-fluid-layer evolution,’ Journal of Fluid Mechanics, 920: A131, 2021.
L. Li, T. Jin, L. Zou, K. Luo, and J. Fan, ‘Numerical study of Richtmyer-Meshkov instability in finite thickness fluid layers with reshock,’ Physical Review E, 109: 055105, 2024.
X. Guo, Z. Cong, T. Si, and X. Luo, ‘On Richtmyer–Meshkov finger collisions in a light fluid layer under reshock conditions,’ Journal of Fluid Mechanics, 1000: A87, 2024.
S. Singh, A. Karchani, T. Chourushi, and R.S. Myong, ‘A three-dimensional modal discontinuous Galerkin method for second-order Boltzmann-Curtiss constitutive models of rarefied and microscale gas flow,’ Journal of Computational Physics, 457: 111052, 2022.
L. Krivodonova, ‘Limiters for high-order discontinuous Galerkin methods,’ Journal of Computational Physics, 226: 879–896, 2007.
X. Luo, P. Dong, T. Si, and Z. Zhai, ‘The Richtmyer–Meshkov instability of a ‘V’ shaped air/SF6
interface,’ Journal of Fluid Mechanics, 802: 186–202, 2016.